100% FREE Updated: Mar 2026 Calculus Differential Equations

Higher-Order Linear Differential Equations

Comprehensive study notes on Higher-Order Linear Differential Equations for CUET PG Mathematics preparation. This chapter covers key concepts, formulas, and examples needed for your exam.

Higher-Order Linear Differential Equations

This chapter focuses on the systematic methodologies for solving higher-order linear differential equations, a cornerstone topic in advanced calculus. It thoroughly examines equations with constant coefficients, the Cauchy-Euler equation, and the method of variation of parameters. Proficiency in these analytical techniques is essential for the CUET PG MA examination, as they represent frequently tested concepts within the Differential Equations component.

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Chapter Contents

| # | Topic |
|---|-------|
| 1 | Equations with Constant Coefficients |
| 2 | Cauchy-Euler Equation |
| 3 | Method of Variation of Parameters |

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We begin with Equations with Constant Coefficients.

Part 1: Equations with Constant Coefficients

We investigate linear ordinary differential equations where the coefficients of the derivatives are constants. These equations are fundamental in various scientific and engineering disciplines, providing models for systems ranging from electrical circuits to population dynamics. Mastery of their solution techniques is essential for the CUET PG examination.

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Core Concepts

1. General Form and Classification of ODEs

A general nn-th order ordinary differential equation can be expressed as

F(x,y,y,,y(n))=0F(x, y, y', \dots, y^{(n)}) = 0

We classify ODEs based on their order, linearity, and homogeneity.

📖 Linear vs. Non-linear ODE

An nn-th order ODE is linear if it can be written in the form

an(x)y(n)+an1(x)y(n1)++a1(x)y+a0(x)y=f(x)a_n(x)y^{(n)} + a_{n-1}(x)y^{(n-1)} + \dots + a_1(x)y' + a_0(x)y = f(x)

Otherwise, it is non-linear.

📖 Homogeneous vs. Non-homogeneous ODE

A linear ODE is homogeneous if f(x)=0f(x) = 0. If f(x)0f(x) \neq 0, it is non-homogeneous.

Quick Example: Classify the ODE

d2ydx2+xdydx+y2=0\frac{d^2y}{dx^2} + x\frac{dy}{dx} + y^2 = 0

Step 1: Determine the order.
> The highest derivative is d2ydx2\frac{d^2y}{dx^2}, so the order is 2.

Step 2: Check for linearity.
> The term y2y^2 makes the equation non-linear.
>
> The equation is a second-order non-linear homogeneous ODE.

:::question type="MCQ" question="Classify the differential equation

x2d3ydx3+5dydxsin(y)=exx^2 \frac{d^3y}{dx^3} + 5 \frac{dy}{dx} - \sin(y) = e^x
" options=["Third-order linear non-homogeneous","Third-order non-linear homogeneous","Third-order non-linear non-homogeneous","Second-order linear non-homogeneous"] answer="Third-order non-linear non-homogeneous" hint="Check the highest derivative for order, and powers/functions of yy or its derivatives for linearity. The exe^x term indicates non-homogeneity." solution="Step 1: Order
The highest derivative is d3ydx3\frac{d^3y}{dx^3}, so the order is 3.

Step 2: Linearity
The term sin(y)\sin(y) is a non-linear function of yy. Therefore, the equation is non-linear.

Step 3: Homogeneity
The term exe^x on the right-hand side is a non-zero function of xx. Therefore, the equation is non-homogeneous.

Combining these, the equation is a third-order non-linear non-homogeneous differential equation."
:::

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2. Homogeneous Linear ODEs with Constant Coefficients

We consider equations of the form

any(n)+an1y(n1)++a1y+a0y=0a_n y^{(n)} + a_{n-1} y^{(n-1)} + \dots + a_1 y' + a_0 y = 0

where aia_i are constants. The general solution, known as the Complementary Function (CF), is obtained by solving the characteristic equation.

📖 Characteristic Equation

For a homogeneous linear ODE with constant coefficients,

any(n)++a0y=0a_n y^{(n)} + \dots + a_0 y = 0

the characteristic equation is formed by replacing y(k)y^{(k)} with mkm^k:
anmn+an1mn1++a1m+a0=0a_n m^n + a_{n-1} m^{n-1} + \dots + a_1 m + a_0 = 0

The roots of this polynomial determine the form of the general solution.

The dimension of the solution space for an nn-th order linear homogeneous ODE is nn. This means its general solution will be a linear combination of nn linearly independent solutions.

📐 Superposition Principle

If y1(x)y_1(x), y2(x)y_2(x), \dots, yn(x)y_n(x) are nn linearly independent solutions to an nn-th order linear homogeneous ODE, then their linear combination

yc(x)=c1y1(x)+c2y2(x)++cnyn(x)y_c(x) = c_1 y_1(x) + c_2 y_2(x) + \dots + c_n y_n(x)

is the general solution, where cic_i are arbitrary constants.

Quick Example: Determine the dimension of the solution space for

y2y+y5y=0y''' - 2y'' + y' - 5y = 0

Step 1: Identify the order of the ODE.
> The highest derivative is yy''', so the order is 3.

Step 2: Apply the dimension rule.
> For an nn-th order linear homogeneous ODE, the dimension of the solution space is nn.
>
> Thus, the dimension of the solution space is 3.

:::question type="MCQ" question="The dimension of the solution space for the differential equation

d4ydx43d2ydx2+2y=0\frac{d^4y}{dx^4} - 3\frac{d^2y}{dx^2} + 2y = 0

is:" options=["1","2","3","4"] answer="4" hint="The dimension of the solution space for an nn-th order linear homogeneous ODE is nn." solution="The given differential equation is
d4ydx43d2ydx2+2y=0\frac{d^4y}{dx^4} - 3\frac{d^2y}{dx^2} + 2y = 0

This is a fourth-order linear homogeneous differential equation.
The dimension of the solution space for an nn-th order linear homogeneous ODE is nn.
Here, n=4n=4.
Therefore, the dimension of the solution space is 4."
:::

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3. Cases for Roots of the Characteristic Equation

The form of the complementary function yc(x)y_c(x) depends critically on the nature of the roots of the characteristic equation.

3.1. Case 1: Distinct Real Roots

If the characteristic equation has nn distinct real roots m1m_1, m2m_2, \dots, mnm_n, then the nn linearly independent solutions are em1xe^{m_1x}, em2xe^{m_2x}, \dots, emnxe^{m_nx}.

📐 Distinct Real Roots

If m1m_1, m2m_2, \dots, mnm_n are distinct real roots, the general solution is:

yc(x)=c1em1x+c2em2x++cnemnxy_c(x) = c_1 e^{m_1x} + c_2 e^{m_2x} + \dots + c_n e^{m_nx}

Quick Example: Find the general solution of

y5y+6y=0y'' - 5y' + 6y = 0

Step 1: Form the characteristic equation.

m25m+6=0m^2 - 5m + 6 = 0

Step 2: Solve for the roots.

(m2)(m3)=0(m-2)(m-3) = 0

m1=2,m2=3m_1 = 2, m_2 = 3

Step 3: Write the general solution.

yc(x)=c1e2x+c2e3xy_c(x) = c_1 e^{2x} + c_2 e^{3x}

:::question type="MCQ" question="A complete solution of

y+a1y+a2y=0y'' + a_1y' + a_2y = 0

is
y=c1e2x+c2e5xy = c_1e^{2x} + c_2e^{5x}

The respective values of a1a_1 and a2a_2 are:" options=["7,10-7, 10","7,107, -10","7,10-7, -10","7,107, 10"] answer="7,10-7, 10" hint="If the roots are m1m_1 and m2m_2, the characteristic equation is (mm1)(mm2)=0(m-m_1)(m-m_2)=0. Expand this to find a1a_1 and a2a_2." solution="Step 1: Identify the roots from the given solution.
The given solution is
y=c1e2x+c2e5xy = c_1e^{2x} + c_2e^{5x}

This implies the roots of the characteristic equation are m1=2m_1 = 2 and m2=5m_2 = 5.

Step 2: Form the characteristic equation.
The characteristic equation is (mm1)(mm2)=0(m - m_1)(m - m_2) = 0.

(m2)(m5)=0(m - 2)(m - 5) = 0

m25m2m+10=0m^2 - 5m - 2m + 10 = 0

m27m+10=0m^2 - 7m + 10 = 0

Step 3: Compare with the general form.
The characteristic equation for

y+a1y+a2y=0y'' + a_1y' + a_2y = 0

is
m2+a1m+a2=0m^2 + a_1m + a_2 = 0

Comparing
m27m+10=0m^2 - 7m + 10 = 0

with
m2+a1m+a2=0m^2 + a_1m + a_2 = 0

we find:
a1=7a_1 = -7
a2=10a_2 = 10

Thus, the respective values of a1a_1 and a2a_2 are 7-7 and 1010."
:::

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3.2. Case 2: Repeated Real Roots

If a real root mm has multiplicity kk, then the kk linearly independent solutions associated with this root are emx,xemx,x2emx,,xk1emxe^{mx}, xe^{mx}, x^2e^{mx}, \dots, x^{k-1}e^{mx}.

📐 Repeated Real Roots

If mm is a real root with multiplicity kk, the part of the general solution corresponding to this root is:

yc(x)=(c1+c2x+c3x2++ckxk1)emxy_c(x) = (c_1 + c_2 x + c_3 x^2 + \dots + c_k x^{k-1})e^{mx}

Quick Example: Find the general solution of y+4y+4y=0y'' + 4y' + 4y = 0.

Step 1: Form the characteristic equation.
>

m2+4m+4=0m^2 + 4m + 4 = 0

Step 2: Solve for the roots.
>

(m+2)2=0(m+2)^2 = 0

>
m1=2,m2=2 (multiplicity 2)m_1 = -2, m_2 = -2 \text{ (multiplicity 2)}

Step 3: Write the general solution.
>

yc(x)=(c1+c2x)e2xy_c(x) = (c_1 + c_2 x)e^{-2x}

:::question type="MCQ" question="The general solution of the differential equation:

d3ydx33d2ydx2+3dydxy=0\frac{d^3y}{dx^3} - 3\frac{d^2y}{dx^2} + 3\frac{dy}{dx} - y = 0
is:" options=["c1ex+c2ex+c3xexc_1e^x + c_2e^{-x} + c_3xe^{-x}","c1ex+c2xex+c3x2exc_1e^x + c_2xe^x + c_3x^2e^x","c1ex+c2xex+c3x2exc_1e^{-x} + c_2xe^{-x} + c_3x^2e^{-x}","c1ex+c2x2ex+c3x3exc_1e^x + c_2x^2e^x + c_3x^3e^x"] answer="c1ex+c2xex+c3x2exc_1e^x + c_2xe^x + c_3x^2e^x" hint="Recognize the characteristic polynomial as a binomial expansion. The roots will be repeated." solution="Step 1: Form the characteristic equation.
The characteristic equation is:
m33m2+3m1=0m^3 - 3m^2 + 3m - 1 = 0

Step 2: Factor the characteristic equation.
This is a standard binomial expansion:

(m1)3=m33m2(1)+3m(1)213(m-1)^3 = m^3 - 3m^2(1) + 3m(1)^2 - 1^3

So,
(m1)3=0(m-1)^3 = 0

Step 3: Identify the roots and their multiplicity.
The root is m=1m = 1 with multiplicity 3.

Step 4: Write the general solution.
For a root mm with multiplicity kk, the solutions are emx,xemx,,xk1emxe^{mx}, xe^{mx}, \dots, x^{k-1}e^{mx}.
Here, m=1m=1 and k=3k=3. So the solutions are ex,xex,x2exe^x, xe^x, x^2e^x.
The general solution is:

yc(x)=c1ex+c2xex+c3x2exy_c(x) = c_1e^x + c_2xe^x + c_3x^2e^x

Answer: c1ex+c2xex+c3x2ex\boxed{c_1e^x + c_2xe^x + c_3x^2e^x}"
:::

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3.3. Case 3: Complex Conjugate Roots

If the characteristic equation has complex conjugate roots of the form m=α±iβm = \alpha \pm i\beta, then the two linearly independent solutions are eαxcos(βx)e^{\alpha x}\cos(\beta x) and eαxsin(βx)e^{\alpha x}\sin(\beta x).

📐 Complex Conjugate Roots

If m=α±iβm = \alpha \pm i\beta are complex conjugate roots, the part of the general solution corresponding to these roots is:

yc(x)=eαx(c1cos(βx)+c2sin(βx))y_c(x) = e^{\alpha x}(c_1 \cos(\beta x) + c_2 \sin(\beta x))

If complex roots α±iβ\alpha \pm i\beta have multiplicity kk, then the solutions are:
yc(x)=eαx[(c1+c2x++ckxk1)cos(βx)+(d1+d2x++dkxk1)sin(βx)]y_c(x) = e^{\alpha x}[(c_1 + c_2 x + \dots + c_k x^{k-1})\cos(\beta x) + (d_1 + d_2 x + \dots + d_k x^{k-1})\sin(\beta x)]

Quick Example: Find the general solution of y+2y+5y=0y'' + 2y' + 5y = 0.

Step 1: Form the characteristic equation.
>

m2+2m+5=0m^2 + 2m + 5 = 0

Step 2: Solve for the roots using the quadratic formula:
>

m=b±b24ac2am = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}

>
>>m=2±224(1)(5)2(1)>m=2±4202>m=2±162>m=2±4i2>m=1±2i>>> \begin{aligned}> m & = \frac{-2 \pm \sqrt{2^2 - 4(1)(5)}}{2(1)} \\
> m & = \frac{-2 \pm \sqrt{4 - 20}}{2} \\
> m & = \frac{-2 \pm \sqrt{-16}}{2} \\
> m & = \frac{-2 \pm 4i}{2} \\
> m & = -1 \pm 2i
> \end{aligned}
>

Step 3: Identify α\alpha and β\beta.
> Here, α=1\alpha = -1 and β=2\beta = 2.

Step 4: Write the general solution.
>

yc(x)=ex(c1cos(2x)+c2sin(2x))y_c(x) = e^{-x}(c_1 \cos(2x) + c_2 \sin(2x))

:::question type="MCQ" question="The complete solution of the differential equation:

d3ydx3+d2ydx2+4dydx+4y=0\frac{d^3y}{dx^3} + \frac{d^2y}{dx^2} + 4\frac{dy}{dx} + 4y = 0
is:" options=["y=c1ex+c2cosx+c3sinxy = c_1 e^x + c_2 \cos x + c_3 \sin x","y=c1ex+c2cosx+c3sinxy = c_1 e^{-x} + c_2 \cos x + c_3 \sin x","y=c1ex+c2cos2x+c3sin2xy = c_1 e^{-x} + c_2 \cos 2x + c_3 \sin 2x","y=c1ex+c2cos2x+c3sin2xy = c_1 e^x + c_2 \cos 2x + c_3 \sin 2x"] answer="y=c1ex+c2cos2x+c3sin2xy = c_1 e^{-x} + c_2 \cos 2x + c_3 \sin 2x" hint="Factor the characteristic polynomial to find one real root and a pair of complex conjugate roots." solution="Step 1: Form the characteristic equation.
m3+m2+4m+4=0m^3 + m^2 + 4m + 4 = 0

Step 2: Factor the characteristic equation.
We can factor by grouping:

m2(m+1)+4(m+1)=0m^2(m + 1) + 4(m + 1) = 0

(m2+4)(m+1)=0(m^2 + 4)(m + 1) = 0

Step 3: Find the roots.
From (m+1)=0(m+1) = 0, we get m1=1m_1 = -1.
From (m2+4)=0(m^2+4) = 0, we get m2=4m^2 = -4, so m=±4=±2im = \pm \sqrt{-4} = \pm 2i.
So, the roots are m1=1m_1 = -1, m2=2im_2 = 2i, m3=2im_3 = -2i.

Step 4: Write the general solution.
For the real root m1=1m_1 = -1, the solution is c1exc_1 e^{-x}.
For the complex conjugate roots m=±2im = \pm 2i, we have α=0\alpha = 0 and β=2\beta = 2. The solution is e0x(c2cos(2x)+c3sin(2x))=c2cos(2x)+c3sin(2x)e^{0x}(c_2 \cos(2x) + c_3 \sin(2x)) = c_2 \cos(2x) + c_3 \sin(2x).
Combining these, the complete solution is:

y=c1ex+c2cos(2x)+c3sin(2x)y = c_1 e^{-x} + c_2 \cos(2x) + c_3 \sin(2x)

Answer: y=c1ex+c2cos(2x)+c3sin(2x)\boxed{y = c_1 e^{-x} + c_2 \cos(2x) + c_3 \sin(2x)}"
:::

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4. Special Solution Properties

Certain homogeneous ODEs, particularly y+y=0y''+y=0, lead to solutions with useful properties. For y+y=0y''+y=0, the solution is y(x)=c1cosx+c2sinxy(x) = c_1 \cos x + c_2 \sin x. If y(x)=f(x)y(x)=f(x), then y(x)=f(x)=g(x)y'(x)=f'(x)=g(x). We observe that f(x)=f(x)f''(x) = -f(x), and g(x)=f(x)=f(x)g'(x) = f''(x) = -f(x).

Consider the function h(x)=[f(x)]2+[g(x)]2h(x) = [f(x)]^2 + [g(x)]^2.
Differentiating h(x)h(x) with respect to xx:

h(x)=2f(x)f(x)+2g(x)g(x)Substitute f(x)=g(x) and g(x)=f(x):h(x)=2f(x)g(x)+2g(x)(f(x))h(x)=2f(x)g(x)2f(x)g(x)h(x)=0\begin{aligned}h'(x) & = 2f(x)f'(x) + 2g(x)g'(x) \\
\text{Substitute } f'(x)=g(x) \text{ and } g'(x)=-f(x): \\
h'(x) & = 2f(x)g(x) + 2g(x)(-f(x)) \\
h'(x) & = 2f(x)g(x) - 2f(x)g(x) \\
h'(x) & = 0\end{aligned}

Since h(x)=0h'(x)=0, h(x)h(x) must be a constant. This property can be used to solve specific problems.

Quick Example: If f(x)=f(x)f''(x) = -f(x), f(x)=g(x)f'(x) = g(x), h(x)=[f(x)]2+[g(x)]2h(x) = [f(x)]^2 + [g(x)]^2 and h(0)=5h(0) = 5, find h(π)h(\pi).

Step 1: Establish the relationship between f(x)f(x) and g(x)g(x).
> Given f(x)=f(x)f''(x) = -f(x) and f(x)=g(x)f'(x) = g(x). This implies g(x)=f(x)=f(x)g'(x) = f''(x) = -f(x).

Step 2: Differentiate h(x)h(x).
>

>>h(x)=[f(x)]2+[g(x)]2>h(x)=2f(x)f(x)+2g(x)g(x)>>> \begin{aligned}> h(x) & = [f(x)]^2 + [g(x)]^2 \\
> h'(x) & = 2f(x)f'(x) + 2g(x)g'(x)
> \end{aligned}
>

Step 3: Substitute the relationships.
>

>>h(x)=2f(x)g(x)+2g(x)(f(x))>h(x)=2f(x)g(x)2f(x)g(x)>h(x)=0>>> \begin{aligned}> h'(x) & = 2f(x)g(x) + 2g(x)(-f(x)) \\
> h'(x) & = 2f(x)g(x) - 2f(x)g(x) \\
> h'(x) & = 0
> \end{aligned}
>

Step 4: Conclude the value of h(x)h(x).
> Since h(x)=0h'(x) = 0, h(x)h(x) is a constant.
> Given h(0)=5h(0) = 5, then h(π)h(\pi) must also be 5.

:::question type="MCQ" question="Let y(x)y(x) be a solution to the differential equation y+9y=0y'' + 9y = 0. If z(x)=[y(x)]2+19[y(x)]2z(x) = [y(x)]^2 + \frac{1}{9}[y'(x)]^2 and z(0)=4z(0) = 4, then z(π/2)z(\pi/2) is:" options=["1/91/9","4/94/9","44","99"] answer="44" hint="Differentiate z(x)z(x) with respect to xx and use the given differential equation to simplify. If z(x)=0z'(x)=0, then z(x)z(x) is a constant." solution="Step 1: Use the given differential equation to find y(x)y''(x).
From y+9y=0y'' + 9y = 0, we have y=9yy'' = -9y.

Step 2: Differentiate z(x)z(x) with respect to xx.

z(x)=[y(x)]2+19[y(x)]2z(x)=2y(x)y(x)+192y(x)y(x)\begin{aligned}z(x) & = [y(x)]^2 + \frac{1}{9}[y'(x)]^2 \\
z'(x) & = 2y(x)y'(x) + \frac{1}{9} \cdot 2y'(x)y''(x)\end{aligned}

Step 3: Substitute y(x)=9y(x)y''(x) = -9y(x) into z(x)z'(x).

z(x)=2y(x)y(x)+29y(x)(9y(x))z(x)=2y(x)y(x)2y(x)y(x)z(x)=0\begin{aligned}z'(x) & = 2y(x)y'(x) + \frac{2}{9}y'(x)(-9y(x)) \\
z'(x) & = 2y(x)y'(x) - 2y'(x)y(x) \\
z'(x) & = 0\end{aligned}

Step 4: Conclude the value of z(x)z(x).
Since z(x)=0z'(x) = 0, z(x)z(x) is a constant function.
Given z(0)=4z(0) = 4, it follows that z(x)=4z(x) = 4 for all xx.
Therefore, z(π/2)=4z(\pi/2) = 4.
Answer: 4\boxed{4}"
:::

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Non-Homogeneous Linear ODEs with Constant Coefficients

For a non-homogeneous linear ODE any(n)++a0y=F(x)a_n y^{(n)} + \dots + a_0 y = F(x), the general solution is the sum of the complementary function (ycy_c) and a particular integral (ypy_p).

y(x)=yc(x)+yp(x)y(x) = y_c(x) + y_p(x)

We have already discussed methods for finding ycy_c. We now focus on determining ypy_p.

1. Method of Undetermined Coefficients

This method is applicable when F(x)F(x) is a polynomial, exponential function, sine or cosine function, or finite sums/products of these. The form of ypy_p is assumed based on F(x)F(x) and then coefficients are determined by substitution into the ODE.

⚠️ Common Mistake: Resonance

❌ Assuming the standard form of ypy_p when F(x)F(x) is part of the complementary function.
✅ If a term in F(x)F(x) is a solution to the homogeneous equation, multiply the assumed ypy_p by xsx^s, where ss is the smallest non-negative integer such that no term in xsypx^s y_p is a solution to the homogeneous equation. This ss is the multiplicity of the root in the characteristic equation that corresponds to the exponential part of F(x)F(x).

We summarize the forms of ypy_p for common F(x)F(x):

| F(x)F(x) | Form of ypy_p (Initial Guess) | Modification for Resonance (yp=xs(Initial Guess)y_p = x^s \cdot (\text{Initial Guess})) |
| :---------------------------------------- | :------------------------------------------------ | :----------------------------------------------------------------------------------------- |
| Pn(x)=Anxn++A0P_n(x) = A_n x^n + \dots + A_0 | Qn(x)=Bnxn++B0Q_n(x) = B_n x^n + \dots + B_0 | s=0s=0 if m=0m=0 is not a root of CF, s=ks=k if m=0m=0 is a root of CF with multiplicity kk. |
| AeαxAe^{\alpha x} | BeαxBe^{\alpha x} | s=0s=0 if α\alpha is not a root of CF, s=ks=k if α\alpha is a root of CF with multiplicity kk. |
| Asin(βx)A\sin(\beta x) or Acos(βx)A\cos(\beta x) | Bcos(βx)+Csin(βx)B\cos(\beta x) + C\sin(\beta x) | s=0s=0 if ±iβ\pm i\beta are not roots of CF, s=ks=k if ±iβ\pm i\beta are roots of CF with multiplicity kk. |
| Pn(x)eαxP_n(x)e^{\alpha x} | Qn(x)eαxQ_n(x)e^{\alpha x} | s=0s=0 if α\alpha is not a root of CF, s=ks=k if α\alpha is a root of CF with multiplicity kk. |
| Pn(x)sin(βx)P_n(x)\sin(\beta x) or Pn(x)cos(βx)P_n(x)\cos(\beta x) | (Qn(x)cos(βx)+Rn(x)sin(βx))(Q_n(x)\cos(\beta x) + R_n(x)\sin(\beta x)) | s=0s=0 if ±iβ\pm i\beta are not roots of CF, s=ks=k if ±iβ\pm i\beta are roots of CF with multiplicity kk. |
| eαxsin(βx)e^{\alpha x}\sin(\beta x) or eαxcos(βx)e^{\alpha x}\cos(\beta x) | eαx(Bcos(βx)+Csin(βx))e^{\alpha x}(B\cos(\beta x) + C\sin(\beta x)) | s=0s=0 if α±iβ\alpha \pm i\beta are not roots of CF, s=ks=k if α±iβ\alpha \pm i\beta are roots of CF with multiplicity kk. |

Note: If F(x)F(x) is a sum of terms, ypy_p is the sum of particular integrals for each term.

1.1. F(x)=AeαxF(x) = Ae^{\alpha x}

Quick Example: Find the PI of y4y=3e2xy'' - 4y = 3e^{2x}.

Step 1: Find the roots of the characteristic equation (for CF).
>

m24=0m=±2m^2 - 4 = 0 \Rightarrow m = \pm 2

> The roots are m1=2,m2=2m_1 = 2, m_2 = -2.

Step 2: Determine the initial form of ypy_p.
> F(x)=3e2xF(x) = 3e^{2x}. The value α=2\alpha = 2.
> Since α=2\alpha = 2 is a root of the characteristic equation with multiplicity s=1s=1, we must multiply by xx.
> Initial guess: yp=Ae2xy_p = Ae^{2x}.
> Modified guess: yp=Axe2xy_p = Axe^{2x}.

Step 3: Find derivatives of ypy_p.
>

>>yp=A(e2x+2xe2x)=Ae2x(1+2x)>yp=A(2e2x(1+2x)+e2x(2))=Ae2x(2+4x+2)=Ae2x(4+4x)>>> \begin{aligned}> y_p' & = A(e^{2x} + 2xe^{2x}) = Ae^{2x}(1 + 2x) \\
> y_p'' & = A(2e^{2x}(1+2x) + e^{2x}(2)) = Ae^{2x}(2+4x+2) = Ae^{2x}(4+4x)
> \end{aligned}
>

Step 4: Substitute yp,ypy_p, y_p' into the ODE.
>

>>Ae2x(4+4x)4(Axe2x)=3e2x>4Ae2x+4Axe2x4Axe2x=3e2x>4Ae2x=3e2x>>> \begin{aligned}> Ae^{2x}(4+4x) - 4(Axe^{2x}) & = 3e^{2x} \\
> 4Ae^{2x} + 4Axe^{2x} - 4Axe^{2x} & = 3e^{2x} \\
> 4Ae^{2x} & = 3e^{2x}
> \end{aligned}
>

Step 5: Equate coefficients to find AA.
>

4A=3A=344A = 3 \Rightarrow A = \frac{3}{4}

Step 6: Write the particular integral.
>

yp=34xe2xy_p = \frac{3}{4}xe^{2x}

:::question type="MCQ" question="The particular integral (PI) of the differential equation:

2d2ydx2dydx3y=5e(3/2)x2\frac{d^2y}{dx^2} - \frac{dy}{dx} - 3y = 5e^{(3/2)x}
is given as:" options=["xe(3/2)xxe^{(3/2)x}","e(3/2)xe^{(3/2)x}","xe(3/2)xxe^{-(3/2)x}","e(3/2)xe^{-(3/2)x}"] answer="xe(3/2)xxe^{(3/2)x}" hint="First, find the roots of the characteristic equation. Check if the exponent in F(x)F(x) is one of the roots (resonance case)." solution="Step 1: Find the roots of the characteristic equation.
The characteristic equation is:
2m2m3=02m^2 - m - 3 = 0

Using the quadratic formula:
m=b±b24ac2am = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}

m=1±(1)24(2)(3)2(2)m=1±1+244m=1±254m=1±54\begin{aligned}m & = \frac{1 \pm \sqrt{(-1)^2 - 4(2)(-3)}}{2(2)} \\
m & = \frac{1 \pm \sqrt{1 + 24}}{4} \\
m & = \frac{1 \pm \sqrt{25}}{4} \\
m & = \frac{1 \pm 5}{4}\end{aligned}

The roots are m1=1+54=64=32m_1 = \frac{1+5}{4} = \frac{6}{4} = \frac{3}{2} and m2=154=44=1m_2 = \frac{1-5}{4} = \frac{-4}{4} = -1.

Step 2: Determine the form of F(x)F(x) and check for resonance.
The forcing function is F(x)=5e(3/2)xF(x) = 5e^{(3/2)x}.
The exponent is α=3/2\alpha = 3/2.
Since α=3/2\alpha = 3/2 is a root of the characteristic equation (specifically, m1=3/2m_1 = 3/2) with multiplicity 1, we must multiply the initial guess by xx.

Step 3: Propose the particular integral ypy_p.
Initial guess: yp=Ae(3/2)xy_p = Ae^{(3/2)x}.
Modified guess (due to resonance): yp=Axe(3/2)xy_p = Axe^{(3/2)x}.

Step 4: Calculate derivatives of ypy_p.

yp=A(e(3/2)x+x32e(3/2)x)=Ae(3/2)x(1+32x)yp=A(32e(3/2)x(1+32x)+e(3/2)x(32))yp=Ae(3/2)x(32+94x+32)=Ae(3/2)x(3+94x)\begin{aligned}y_p' & = A \left( e^{(3/2)x} + x \cdot \frac{3}{2}e^{(3/2)x} \right) = A e^{(3/2)x} \left(1 + \frac{3}{2}x \right) \\
y_p'' & = A \left( \frac{3}{2}e^{(3/2)x} \left(1 + \frac{3}{2}x \right) + e^{(3/2)x} \left(\frac{3}{2} \right) \right) \\
y_p'' & = A e^{(3/2)x} \left( \frac{3}{2} + \frac{9}{4}x + \frac{3}{2} \right) = A e^{(3/2)x} \left( 3 + \frac{9}{4}x \right)\end{aligned}

Step 5: Substitute yp,ypy_p, y_p' and ypy_p'' into the differential equation.

2[Ae(3/2)x(3+94x)][Ae(3/2)x(1+32x)]3[Axe(3/2)x]=5e(3/2)xDivide by e(3/2)x (since e(3/2)x0):2A(3+94x)A(1+32x)3Ax=56A+92AxA32Ax3Ax=5(6AA)+(92A32A3A)x=55A+(62A3A)x=55A+(3A3A)x=55A+0x=5\begin{aligned}2 \left[ A e^{(3/2)x} \left( 3 + \frac{9}{4}x \right) \right] - \left[ A e^{(3/2)x} \left(1 + \frac{3}{2}x \right) \right] - 3 \left[ A x e^{(3/2)x} \right] & = 5e^{(3/2)x} \\
\text{Divide by } e^{(3/2)x} \text{ (since } e^{(3/2)x} \neq 0 \text{):} \\
2A \left( 3 + \frac{9}{4}x \right) - A \left(1 + \frac{3}{2}x \right) - 3Ax & = 5 \\
6A + \frac{9}{2}Ax - A - \frac{3}{2}Ax - 3Ax & = 5 \\
(6A - A) + \left(\frac{9}{2}A - \frac{3}{2}A - 3A \right)x & = 5 \\
5A + \left(\frac{6}{2}A - 3A \right)x & = 5 \\
5A + (3A - 3A)x & = 5 \\
5A + 0x & = 5\end{aligned}

Step 6: Solve for AA.

5A=5A=15A = 5 \Rightarrow A = 1

Step 7: Write the particular integral.

yp=(1)xe(3/2)x=xe(3/2)xy_p = (1)xe^{(3/2)x} = xe^{(3/2)x}

Answer: xe(3/2)x\boxed{xe^{(3/2)x}}"
:::

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1.2. F(x)=Asin(βx)F(x) = A\sin(\beta x) or Acos(βx)A\cos(\beta x)

Quick Example: Find the PI of y+y=sinxy'' + y = \sin x.

Step 1: Find the roots of the characteristic equation.
>

m2+1=0m=±im^2 + 1 = 0 \Rightarrow m = \pm i

> The roots are m1=i,m2=im_1 = i, m_2 = -i.

Step 2: Determine the initial form of ypy_p.
> F(x)=sinxF(x) = \sin x. Here, β=1\beta = 1. The complex roots of the characteristic equation are ±iβ=±i(1)\pm i\beta = \pm i(1).
> Since ±i\pm i are roots of the characteristic equation with multiplicity s=1s=1, we must multiply by xx.
> Initial guess: yp=Acosx+Bsinxy_p = A\cos x + B\sin x.
> Modified guess: yp=x(Acosx+Bsinx)y_p = x(A\cos x + B\sin x).

Step 3: Find derivatives of ypy_p.
>

>>yp=Axcosx+Bxsinx>yp=A(cosxxsinx)+B(sinx+xcosx)>yp=A(sinx(sinx+xcosx))+B(cosx+(cosxxsinx))>yp=A(2sinxxcosx)+B(2cosxxsinx)>>> \begin{aligned}> y_p & = Ax\cos x + Bx\sin x \\
> y_p' & = A(\cos x - x\sin x) + B(\sin x + x\cos x) \\
> y_p'' & = A(-\sin x - (\sin x + x\cos x)) + B(\cos x + (\cos x - x\sin x)) \\
> y_p'' & = A(-2\sin x - x\cos x) + B(2\cos x - x\sin x)
> \end{aligned}
>

Step 4: Substitute yp,ypy_p, y_p'' into the ODE.
>

>>(A(2sinxxcosx)+B(2cosxxsinx))+(Axcosx+Bxsinx)=sinx>2AsinxAxcosx+2BcosxBxsinx+Axcosx+Bxsinx=sinx>2Asinx+2Bcosx=sinx>>> \begin{aligned}> (A(-2\sin x - x\cos x) + B(2\cos x - x\sin x)) + (Ax\cos x + Bx\sin x) & = \sin x \\
> -2A\sin x - Ax\cos x + 2B\cos x - Bx\sin x + Ax\cos x + Bx\sin x & = \sin x \\
> -2A\sin x + 2B\cos x & = \sin x
> \end{aligned}
>

Step 5: Equate coefficients.
> Coefficients of sinx\sin x: 2A=1A=12-2A = 1 \Rightarrow A = -\frac{1}{2}
> Coefficients of cosx\cos x: 2B=0B=02B = 0 \Rightarrow B = 0

Step 6: Write the particular integral.
>

yp=x(12cosx+0sinx)=12xcosxy_p = x\left(-\frac{1}{2}\cos x + 0\sin x\right) = -\frac{1}{2}x\cos x

:::question type="MCQ" question="For the differential equation:

(D23D4)y=2sinx(D^2 - 3D - 4)y = 2\sin x
the particular integral is:" options=["517sinx+317cosx-\frac{5}{17}\sin x + \frac{3}{17}\cos x","213sinx1013cosx\frac{2}{13}\sin x - \frac{10}{13}\cos x","15sinx+35cosx\frac{1}{5}\sin x + \frac{3}{5}\cos x","517sinx317cosx\frac{5}{17}\sin x - \frac{3}{17}\cos x"] answer="517sinx+317cosx-\frac{5}{17}\sin x + \frac{3}{17}\cos x" hint="Find the roots of the characteristic equation. Since ii is not a root, no modification is needed for the PI. Substitute yp=Acosx+Bsinxy_p = A\cos x + B\sin x." solution="Step 1: Find the roots of the characteristic equation.
The characteristic equation is:
m23m4=0m^2 - 3m - 4 = 0

(m4)(m+1)=0(m-4)(m+1) = 0

The roots are m1=4,m2=1m_1 = 4, m_2 = -1.

Step 2: Determine the form of F(x)F(x) and check for resonance.
The forcing function is F(x)=2sinxF(x) = 2\sin x. Here, β=1\beta = 1.
The roots ±iβ=±i\pm i\beta = \pm i are not roots of the characteristic equation. So, no modification is needed.

Step 3: Propose the particular integral ypy_p.

yp=Acosx+Bsinxy_p = A\cos x + B\sin x

Step 4: Calculate derivatives of ypy_p.

yp=Asinx+Bcosxyp=AcosxBsinx\begin{aligned}y_p' & = -A\sin x + B\cos x \\
y_p'' & = -A\cos x - B\sin x\end{aligned}

Step 5: Substitute yp,yp,ypy_p, y_p', y_p'' into the differential equation.

(AcosxBsinx)3(Asinx+Bcosx)4(Acosx+Bsinx)=2sinxAcosxBsinx+3Asinx3Bcosx4Acosx4Bsinx=2sinxGroup terms by sinx and cosx:(B+3A4B)sinx+(A3B4A)cosx=2sinx(3A5B)sinx+(5A3B)cosx=2sinx\begin{aligned}( -A\cos x - B\sin x ) - 3( -A\sin x + B\cos x ) - 4( A\cos x + B\sin x ) & = 2\sin x \\
-A\cos x - B\sin x + 3A\sin x - 3B\cos x - 4A\cos x - 4B\sin x & = 2\sin x \\
\text{Group terms by } \sin x \text{ and } \cos x \text{:} \\
(-B + 3A - 4B)\sin x + (-A - 3B - 4A)\cos x & = 2\sin x \\
(3A - 5B)\sin x + (-5A - 3B)\cos x & = 2\sin x\end{aligned}

Step 6: Equate coefficients.
Comparing coefficients of sinx\sin x:

3A5B=2(1)3A - 5B = 2 \quad (1)

Comparing coefficients of cosx\cos x:
5A3B=0(2)-5A - 3B = 0 \quad (2)

From (2), 3B=5AB=53A3B = -5A \Rightarrow B = -\frac{5}{3}A.

Substitute BB into (1):

3A5(53A)=23A+253A=29A+25A3=234A3=2A=634=317\begin{aligned}3A - 5\left(-\frac{5}{3}A\right) & = 2 \\
3A + \frac{25}{3}A & = 2 \\
\frac{9A + 25A}{3} & = 2 \\
\frac{34A}{3} & = 2 \\
A & = \frac{6}{34} = \frac{3}{17}\end{aligned}

Now find BB:
B=53A=53(317)=517B = -\frac{5}{3}A = -\frac{5}{3}\left(\frac{3}{17}\right) = -\frac{5}{17}

Step 7: Write the particular integral.

yp=317cosx517sinxy_p = \frac{3}{17}\cos x - \frac{5}{17}\sin x

Answer: 517sinx+317cosx\boxed{-\frac{5}{17}\sin x + \frac{3}{17}\cos x}"
:::

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1.3. F(x)=Pn(x)eαxF(x) = P_n(x)e^{\alpha x} or F(x)=eαxsin(βx)F(x) = e^{\alpha x}\sin(\beta x) or eαxcos(βx)e^{\alpha x}\cos(\beta x)

For F(x)=Pn(x)eαxcos(βx)F(x) = P_n(x)e^{\alpha x}\cos(\beta x) or Pn(x)eαxsin(βx)P_n(x)e^{\alpha x}\sin(\beta x), the initial form of ypy_p is xseαx[Qn(x)cos(βx)+Rn(x)sin(βx)]x^s e^{\alpha x} [Q_n(x)\cos(\beta x) + R_n(x)\sin(\beta x)], where Qn(x)Q_n(x) and Rn(x)R_n(x) are general polynomials of degree nn, and ss is the multiplicity of α±iβ\alpha \pm i\beta as roots of the characteristic equation. If β=0\beta=0, this reduces to Pn(x)eαxP_n(x)e^{\alpha x}.

💡 Shift Theorem for PI

To find ypy_p for F(x)=eαxG(x)F(x) = e^{\alpha x}G(x), one can use the operator method:

yp=1P(D)eαxG(x)=eαx1P(D+α)G(x)y_p = \frac{1}{P(D)}e^{\alpha x}G(x) = e^{\alpha x}\frac{1}{P(D+\alpha)}G(x)

This shifts the exponential part out and simplifies the operator for G(x)G(x).

Quick Example: Find the PI of y4y=xexy'' - 4y = xe^x.

Step 1: Find the roots of the characteristic equation.
>

m24=0m=±2m^2 - 4 = 0 \Rightarrow m = \pm 2

> The roots are m1=2,m2=2m_1 = 2, m_2 = -2.

Step 2: Determine the initial form of ypy_p.
> F(x)=xexF(x) = xe^x. Here, Pn(x)=xP_n(x)=x (degree 1), α=1\alpha = 1, β=0\beta = 0.
> Since α=1\alpha = 1 is not a root of the characteristic equation, s=0s=0.
> yp=(Ax+B)exy_p = (Ax+B)e^x.

Step 3: Find derivatives of ypy_p.
>

yp=Aex+(Ax+B)ex=(Ax+A+B)exy_p' = A e^x + (Ax+B)e^x = (Ax+A+B)e^x

>
yp=Aex+(Ax+A+B)ex=(Ax+2A+B)exy_p'' = A e^x + (Ax+A+B)e^x = (Ax+2A+B)e^x

Step 4: Substitute yp,ypy_p, y_p'' into the ODE.
>

(Ax+2A+B)ex4(Ax+B)ex=xex(Ax+2A+B)e^x - 4(Ax+B)e^x = xe^x

> Divide by exe^x:
>
(Ax+2A+B)4(Ax+B)=x(Ax+2A+B) - 4(Ax+B) = x

>
Ax+2A+B4Ax4B=xAx + 2A + B - 4Ax - 4B = x

>
3Ax+(2A3B)=x-3Ax + (2A - 3B) = x

Step 5: Equate coefficients.
> Coefficients of xx: 3A=1A=13-3A = 1 \Rightarrow A = -\frac{1}{3}
> Constant terms: 2A3B=02(13)3B=023=3BB=292A - 3B = 0 \Rightarrow 2(-\frac{1}{3}) - 3B = 0 \Rightarrow -\frac{2}{3} = 3B \Rightarrow B = -\frac{2}{9}

Step 6: Write the particular integral.
>

yp=(13x29)exy_p = \left(-\frac{1}{3}x - \frac{2}{9}\right)e^x

:::question type="MCQ" question="The complete solution of the differential equation d2ydx24y=xsinhx\frac{d^2y}{dx^2} - 4y = x \sinh x is:" options=["y=c1e2x+c2e2xx3sinhx29coshxy = c_1e^{2x} + c_2e^{-2x} - \frac{x}{3} \sinh x - \frac{2}{9} \cosh x","y=c1e2x+c2e2x+x3sinhx29coshxy = c_1e^{-2x} + c_2e^{2x} + \frac{x}{3} \sinh x - \frac{2}{9} \cosh x","y=c1ex+c2exx3sinhx29coshxy = c_1e^{x} + c_2e^{-x} - \frac{x}{3} \sinh x - \frac{2}{9} \cosh x","y=c1e2x+c2e2xx3sinhx+29coshxy = c_1e^{2x} + c_2e^{-2x} - \frac{x}{3} \sinh x + \frac{2}{9} \cosh x"] answer="y=c1e2x+c2e2xx3sinhx29coshxy = c_1e^{2x} + c_2e^{-2x} - \frac{x}{3} \sinh x - \frac{2}{9} \cosh x" hint="First, find the CF. Then, rewrite sinhx\sinh x in terms of exponentials and find PI for each part using the method of undetermined coefficients, paying attention to resonance." solution="Step 1: Find the Complementary Function (ycy_c).
The characteristic equation is m24=0m^2 - 4 = 0.
So, m2=4m=±2m^2 = 4 \Rightarrow m = \pm 2.
Thus, yc=c1e2x+c2e2xy_c = c_1e^{2x} + c_2e^{-2x}.

Step 2: Rewrite the forcing function F(x)F(x).
We know sinhx=exex2\sinh x = \frac{e^x - e^{-x}}{2}.
So, F(x)=xsinhx=x(exex2)=12xex12xexF(x) = x \sinh x = x \left(\frac{e^x - e^{-x}}{2}\right) = \frac{1}{2}xe^x - \frac{1}{2}xe^{-x}.
We will find a particular integral for each term: F1(x)=12xexF_1(x) = \frac{1}{2}xe^x and F2(x)=12xexF_2(x) = -\frac{1}{2}xe^{-x}.

Step 3: Find PI for F1(x)=12xexF_1(x) = \frac{1}{2}xe^x.
Here, α=1\alpha = 1. Since m=1m=1 is not a root of m24=0m^2-4=0, no resonance.
Assume yp1=(Ax+B)exy_{p1} = (Ax+B)e^x.

yp1=(Ax+A+B)exy_{p1}' = (Ax+A+B)e^x

yp1=(Ax+2A+B)exy_{p1}'' = (Ax+2A+B)e^x

Substitute into y4y=12xexy'' - 4y = \frac{1}{2}xe^x:
(Ax+2A+B)ex4(Ax+B)ex=12xex(Ax+2A+B)e^x - 4(Ax+B)e^x = \frac{1}{2}xe^x

Divide by exe^x:
(Ax+2A+B)4(Ax+B)=12x(Ax+2A+B) - 4(Ax+B) = \frac{1}{2}x

3Ax+(2A3B)=12x-3Ax + (2A-3B) = \frac{1}{2}x

Equating coefficients:
3A=12A=16-3A = \frac{1}{2} \Rightarrow A = -\frac{1}{6}
2A3B=02(16)3B=013=3BB=192A-3B = 0 \Rightarrow 2(-\frac{1}{6}) - 3B = 0 \Rightarrow -\frac{1}{3} = 3B \Rightarrow B = -\frac{1}{9}
So, yp1=(16x19)exy_{p1} = \left(-\frac{1}{6}x - \frac{1}{9}\right)e^x.

Step 4: Find PI for F2(x)=12xexF_2(x) = -\frac{1}{2}xe^{-x}.
Here, α=1\alpha = -1. Since m=1m=-1 is not a root of m24=0m^2-4=0, no resonance.
Assume yp2=(Cx+D)exy_{p2} = (Cx+D)e^{-x}.

yp2=(Cx+CD)exy_{p2}' = (-Cx+C-D)e^{-x}

yp2=(Cx2C+D)exy_{p2}'' = (Cx-2C+D)e^{-x}

Substitute into y4y=12xexy'' - 4y = -\frac{1}{2}xe^{-x}:
(Cx2C+D)ex4(Cx+D)ex=12xex(Cx-2C+D)e^{-x} - 4(Cx+D)e^{-x} = -\frac{1}{2}xe^{-x}

Divide by exe^{-x}:
(Cx2C+D)4(Cx+D)=12x(Cx-2C+D) - 4(Cx+D) = -\frac{1}{2}x

3Cx+(2C3D)=12x-3Cx + (-2C-3D) = -\frac{1}{2}x

Equating coefficients:
3C=12C=16-3C = -\frac{1}{2} \Rightarrow C = \frac{1}{6}
2C3D=02(16)3D=013=3DD=19-2C-3D = 0 \Rightarrow -2(\frac{1}{6}) - 3D = 0 \Rightarrow -\frac{1}{3} = 3D \Rightarrow D = -\frac{1}{9}
So, yp2=(16x19)exy_{p2} = \left(\frac{1}{6}x - \frac{1}{9}\right)e^{-x}.

Step 5: Combine yp1y_{p1} and yp2y_{p2} to get ypy_p.

yp=yp1+yp2=(16x19)ex+(16x19)exy_p = y_{p1} + y_{p2} = \left(-\frac{1}{6}x - \frac{1}{9}\right)e^x + \left(\frac{1}{6}x - \frac{1}{9}\right)e^{-x}

yp=16xex19ex+16xex19exy_p = -\frac{1}{6}xe^x - \frac{1}{9}e^x + \frac{1}{6}xe^{-x} - \frac{1}{9}e^{-x}

yp=16x(exex)19(ex+ex)y_p = -\frac{1}{6}x(e^x - e^{-x}) - \frac{1}{9}(e^x + e^{-x})

Recall exex=2sinhxe^x - e^{-x} = 2\sinh x and ex+ex=2coshxe^x + e^{-x} = 2\cosh x.
yp=16x(2sinhx)19(2coshx)y_p = -\frac{1}{6}x(2\sinh x) - \frac{1}{9}(2\cosh x)

yp=13xsinhx29coshxy_p = -\frac{1}{3}x\sinh x - \frac{2}{9}\cosh x

Step 6: Write the complete solution.

y=yc+yp=c1e2x+c2e2xx3sinhx29coshxy = y_c + y_p = \boxed{c_1e^{2x} + c_2e^{-2x} - \frac{x}{3}\sinh x - \frac{2}{9}\cosh x}
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1.4. F(x)=eαxsin(βx)F(x) = e^{\alpha x}\sin(\beta x) or eαxcos(βx)e^{\alpha x}\cos(\beta x)

Quick Example: Find the PI of (D22D+4)y=exsinx(D^2-2D+4)y = e^x \sin x.

Step 1: Find the roots of the characteristic equation.
>

m22m+4=0m^2 - 2m + 4 = 0

>
m=2±44(1)(4)2=2±122=2±2i32=1±i3m = \frac{2 \pm \sqrt{4 - 4(1)(4)}}{2} = \frac{2 \pm \sqrt{-12}}{2} = \frac{2 \pm 2i\sqrt{3}}{2} = 1 \pm i\sqrt{3}

> The roots are 1+i31+i\sqrt{3} and 1i31-i\sqrt{3}.

Step 2: Determine the initial form of ypy_p.
> F(x)=exsinxF(x) = e^x \sin x. Here, α=1,β=1\alpha = 1, \beta = 1. The complex roots are α±iβ=1±i\alpha \pm i\beta = 1 \pm i.
> Since 1±i1 \pm i are not roots of the characteristic equation (1±i31 \pm i\sqrt{3} are the roots), no resonance. So s=0s=0.
> yp=ex(Acosx+Bsinx)y_p = e^x(A\cos x + B\sin x).

Step 3: Find derivatives of ypy_p.
>

yp=ex(Acosx+Bsinx)+ex(Asinx+Bcosx)=ex((A+B)cosx+(BA)sinx)y_p' = e^x(A\cos x + B\sin x) + e^x(-A\sin x + B\cos x) = e^x((A+B)\cos x + (B-A)\sin x)

>
yp=ex((A+B)cosx+(BA)sinx)+ex((A+B)sinx+(BA)cosx)y_p'' = e^x((A+B)\cos x + (B-A)\sin x) + e^x(-(A+B)\sin x + (B-A)\cos x)

>
yp=ex((A+B+BA)cosx+(BAAB)sinx)=ex(2Bcosx2Asinx)y_p'' = e^x( (A+B+B-A)\cos x + (B-A-A-B)\sin x ) = e^x(2B\cos x - 2A\sin x)

Step 4: Substitute yp,yp,ypy_p, y_p', y_p'' into the ODE.
>

ex(2Bcosx2Asinx)2ex((A+B)cosx+(BA)sinx)+4ex(Acosx+Bsinx)=exsinxe^x(2B\cos x - 2A\sin x) - 2e^x((A+B)\cos x + (B-A)\sin x) + 4e^x(A\cos x + B\sin x) = e^x\sin x

> Divide by exe^x:
>
(2Bcosx2Asinx)2((A+B)cosx+(BA)sinx)+4(Acosx+Bsinx)=sinx(2B\cos x - 2A\sin x) - 2((A+B)\cos x + (B-A)\sin x) + 4(A\cos x + B\sin x) = \sin x

>
(2B2A2B+4A)cosx+(2A2B+2A+4B)sinx=sinx(2B - 2A - 2B + 4A)\cos x + (-2A - 2B + 2A + 4B)\sin x = \sin x

>
(2A)cosx+(2B)sinx=sinx(2A)\cos x + (2B)\sin x = \sin x

Step 5: Equate coefficients.
> Coefficients of cosx\cos x: 2A=0A=02A = 0 \Rightarrow A = 0
> Coefficients of sinx\sin x: 2B=1B=122B = 1 \Rightarrow B = \frac{1}{2}

Step 6: Write the particular integral.
>

yp=ex(0cosx+12sinx)=12exsinxy_p = e^x\left(0\cos x + \frac{1}{2}\sin x\right) = \frac{1}{2}e^x\sin x

:::question type="MCQ" question="If xRx \in \mathbb{R} and a particular integral (P.I.) of (D22D+4)y=exsinx(D^2-2D+4)y = e^x \sin x is 12exf(x)\frac{1}{2}e^x f(x), then f(x)f(x) is:" options=["an increasing function on [0,π][0, \pi]","a decreasing function on [0,π][0, \pi]","a continuous function on [2π,2π][-2\pi, 2\pi]","not differentiable function at x=0x = 0"] answer="a continuous function on [2π,2π][-2\pi, 2\pi]" hint="First, find the particular integral ypy_p. Then identify f(x)f(x) and analyze its properties." solution="Step 1: Find the particular integral (PI).
The characteristic equation is m22m+4=0m^2 - 2m + 4 = 0.
The roots are m=2±4162=2±122=1±i3m = \frac{2 \pm \sqrt{4 - 16}}{2} = \frac{2 \pm \sqrt{-12}}{2} = 1 \pm i\sqrt{3}.
The forcing function is F(x)=exsinxF(x) = e^x \sin x. Here, α=1,β=1\alpha = 1, \beta = 1. The complex number 1+i1+i is not a root of the characteristic equation. Thus, there is no resonance.
We assume the particular integral ypy_p to be of the form yp=ex(Acosx+Bsinx)y_p = e^x(A\cos x + B\sin x).

Calculate the derivatives:

yp=ex((A+B)cosx+(BA)sinx)y_p' = e^x((A+B)\cos x + (B-A)\sin x)

yp=ex((A+B)cosx+(BA)sinx)+ex((A+B)sinx+(BA)cosx)y_p'' = e^x((A+B)\cos x + (B-A)\sin x) + e^x(-(A+B)\sin x + (B-A)\cos x)

yp=ex((A+B+BA)cosx+(BAAB)sinx)=ex(2Bcosx2Asinx)y_p'' = e^x( (A+B+B-A)\cos x + (B-A-A-B)\sin x ) = e^x(2B\cos x - 2A\sin x)

Substitute into the differential equation (D22D+4)y=exsinx(D^2-2D+4)y = e^x \sin x:

ex(2Bcosx2Asinx)2ex((A+B)cosx+(BA)sinx)+4ex(Acosx+Bsinx)=exsinxe^x(2B\cos x - 2A\sin x) - 2e^x((A+B)\cos x + (B-A)\sin x) + 4e^x(A\cos x + B\sin x) = e^x \sin x

Divide by exe^x:
(2Bcosx2Asinx)2(Acosx+Bcosx+BsinxAsinx)+4(Acosx+Bsinx)=sinx(2B\cos x - 2A\sin x) - 2(A\cos x + B\cos x + B\sin x - A\sin x) + 4(A\cos x + B\sin x) = \sin x

Group coefficients of cosx\cos x and sinx\sin x:
cosx(2B2A2B+4A)+sinx(2A2B+2A+4B)=sinx\cos x (2B - 2A - 2B + 4A) + \sin x (-2A - 2B + 2A + 4B) = \sin x

2Acosx+2Bsinx=sinx2A\cos x + 2B\sin x = \sin x

Equating coefficients:
For cosx\cos x: 2A=0A=02A = 0 \Rightarrow A = 0
For sinx\sin x: 2B=1B=122B = 1 \Rightarrow B = \frac{1}{2}

So, yp=ex(0cosx+12sinx)=12exsinxy_p = e^x\left(0\cos x + \frac{1}{2}\sin x\right) = \frac{1}{2}e^x\sin x.

Step 2: Identify f(x)f(x).
We are given that yp=12exf(x)y_p = \frac{1}{2}e^x f(x).
Comparing this with our result yp=12exsinxy_p = \frac{1}{2}e^x\sin x, we find f(x)=sinxf(x) = \sin x.

Step 3: Analyze the properties of f(x)=sinxf(x) = \sin x.
* Continuity: sinx\sin x is continuous everywhere on R\mathbb{R}, including on [2π,2π][-2\pi, 2\pi].
* Differentiability: sinx\sin x is differentiable everywhere on R\mathbb{R}, including at x=0x=0. So, 'not differentiable at x=0x=0' is false.
* Increasing/Decreasing on [0,π][0, \pi]: To check this, we look at f(x)=cosxf'(x) = \cos x.
* On [0,π/2)[0, \pi/2), cosx>0\cos x > 0, so sinx\sin x is increasing.
* On (π/2,π](\pi/2, \pi], cosx<0\cos x < 0, so sinx\sin x is decreasing.
Therefore, sinx\sin x is neither strictly increasing nor strictly decreasing on the entire interval [0,π][0, \pi].

Based on the analysis, f(x)=sinxf(x) = \sin x is a continuous function on [2π,2π][-2\pi, 2\pi]. Answer: a continuous function on [2π,2π]\boxed{\text{a continuous function on } [-2\pi, 2\pi]}"
:::

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2. Method of Variation of Parameters

This method is more general than Undetermined Coefficients, as it works for any continuous F(x)F(x), not just specific forms. However, it typically involves more complex integrations. For an nn-th order ODE, it requires nn linearly independent solutions of the homogeneous equation, y1,,yny_1, \dots, y_n.

For a second-order ODE y+P(x)y+Q(x)y=F(x)y'' + P(x)y' + Q(x)y = F(x), and given yc=c1y1(x)+c2y2(x)y_c = c_1y_1(x) + c_2y_2(x):

📐 Variation of Parameters (2nd Order)

The particular integral is given by:

yp(x)=y1(x)y2(x)F(x)W(y1,y2)(x)dx+y2(x)y1(x)F(x)W(y1,y2)(x)dxy_p(x) = -y_1(x) \int \frac{y_2(x)F(x)}{W(y_1, y_2)(x)} dx + y_2(x) \int \frac{y_1(x)F(x)}{W(y_1, y_2)(x)} dx

Where:
W(y1,y2)(x)=det[y1y2y1y2]=y1y2y2y1W(y_1, y_2)(x) = \det \begin{bmatrix} y_1 & y_2 \\ y_1' & y_2' \end{bmatrix} = y_1 y_2' - y_2 y_1'
is the Wronskian of y1y_1 and y2y_2.
When to use: When F(x)F(x) is not one of the forms suitable for Undetermined Coefficients, or when coefficients P(x),Q(x)P(x), Q(x) are not constant (though this topic focuses on constant coefficients).

Quick Example: Find the PI of y+y=secxy'' + y = \sec x.

Step 1: Find the CF.
> Characteristic equation: m2+1=0m=±im^2+1=0 \Rightarrow m=\pm i.
> yc=c1cosx+c2sinxy_c = c_1\cos x + c_2\sin x. So y1=cosxy_1 = \cos x, y2=sinxy_2 = \sin x.

Step 2: Calculate the Wronskian.
>

W(y1,y2)=det[cosxsinxsinxcosx]=cos2x(sin2x)=cos2x+sin2x=1W(y_1, y_2) = \det \begin{bmatrix} \cos x & \sin x \\ -\sin x & \cos x \end{bmatrix} = \cos^2 x - (-\sin^2 x) = \cos^2 x + \sin^2 x = 1

Step 3: Apply the formula for ypy_p.
> Here, F(x)=secxF(x) = \sec x.
>

yp=y1y2F(x)Wdx+y2y1F(x)Wdxy_p = -y_1 \int \frac{y_2 F(x)}{W} dx + y_2 \int \frac{y_1 F(x)}{W} dx

>
yp=cosxsinxsecx1dx+sinxcosxsecx1dxy_p = -\cos x \int \frac{\sin x \sec x}{1} dx + \sin x \int \frac{\cos x \sec x}{1} dx

>
yp=cosxsinxcosxdx+sinxcosxcosxdxy_p = -\cos x \int \frac{\sin x}{\cos x} dx + \sin x \int \frac{\cos x}{\cos x} dx

>
yp=cosxtanxdx+sinx1dxy_p = -\cos x \int \tan x dx + \sin x \int 1 dx

Step 4: Evaluate the integrals.
> tanxdx=lnsecx\int \tan x dx = \ln|\sec x|
> 1dx=x\int 1 dx = x
>
>

yp=cosx(lnsecx)+sinx(x)y_p = -\cos x (\ln|\sec x|) + \sin x (x)

>
yp=xsinxcosxlnsecxy_p = x\sin x - \cos x \ln|\sec x|

:::question type="NAT" question="Using the method of variation of parameters, find the particular integral of y4y+4y=e2xxy'' - 4y' + 4y = \frac{e^{2x}}{x} for x>0x>0. Express the coefficient of e2xe^{2x}." answer="x \ln x" hint="First, find y1y_1 and y2y_2 from the homogeneous solution. Calculate the Wronskian. Then apply the variation of parameters formula, performing the integrations." solution="Step 1: Find the complementary function (ycy_c).
The characteristic equation is m24m+4=0m^2 - 4m + 4 = 0.

(m2)2=0(m-2)^2 = 0

So, m=2m=2 is a root with multiplicity 2.
The complementary function is yc=c1e2x+c2xe2xy_c = c_1e^{2x} + c_2xe^{2x}.
Thus, y1=e2xy_1 = e^{2x} and y2=xe2xy_2 = xe^{2x}.

Step 2: Calculate the Wronskian W(y1,y2)W(y_1, y_2).
y1=e2x    y1=2e2xy_1 = e^{2x} \implies y_1' = 2e^{2x}
y2=xe2x    y2=e2x+2xe2x=e2x(1+2x)y_2 = xe^{2x} \implies y_2' = e^{2x} + 2xe^{2x} = e^{2x}(1+2x)

W(y1,y2)=y1y2y2y1W(y_1, y_2) = y_1 y_2' - y_2 y_1'

W(y1,y2)=e2x(e2x(1+2x))xe2x(2e2x)W(y_1, y_2) = e^{2x}(e^{2x}(1+2x)) - xe^{2x}(2e^{2x})

W(y1,y2)=e4x(1+2x)2xe4xW(y_1, y_2) = e^{4x}(1+2x) - 2xe^{4x}

W(y1,y2)=e4x(1+2x2x)=e4xW(y_1, y_2) = e^{4x}(1+2x-2x) = e^{4x}

Step 3: Apply the Variation of Parameters formula.
The given ODE is y4y+4y=e2xxy'' - 4y' + 4y = \frac{e^{2x}}{x}. Here, F(x)=e2xxF(x) = \frac{e^{2x}}{x}.

yp(x)=y1(x)y2(x)F(x)W(y1,y2)(x)dx+y2(x)y1(x)F(x)W(y1,y2)(x)dxy_p(x) = -y_1(x) \int \frac{y_2(x)F(x)}{W(y_1, y_2)(x)} dx + y_2(x) \int \frac{y_1(x)F(x)}{W(y_1, y_2)(x)} dx

yp(x)=e2xxe2xe2xxe4xdx+xe2xe2xe2xxe4xdxy_p(x) = -e^{2x} \int \frac{xe^{2x} \cdot \frac{e^{2x}}{x}}{e^{4x}} dx + xe^{2x} \int \frac{e^{2x} \cdot \frac{e^{2x}}{x}}{e^{4x}} dx

yp(x)=e2xe4xe4xdx+xe2x1xdxy_p(x) = -e^{2x} \int \frac{e^{4x}}{e^{4x}} dx + xe^{2x} \int \frac{1}{x} dx

yp(x)=e2x(x)+xe2x(lnx)y_p(x) = -e^{2x}(x) + xe^{2x}(\ln x)

Since x>0x>0, we have lnx\ln x.
yp(x)=xe2x+xe2xlnxy_p(x) = -xe^{2x} + xe^{2x}\ln x

yp(x)=e2x(x+xlnx)y_p(x) = e^{2x}(-x + x\ln x)

yp(x)=e2x(x(lnx1))y_p(x) = e^{2x}(x(\ln x - 1))

Step 4: Identify the coefficient of e2xe^{2x}.
The particular integral is yp(x)=e2x(x(lnx1))y_p(x) = e^{2x}(x(\ln x - 1)).
The coefficient of e2xe^{2x} is x(lnx1)x(\ln x - 1).
The question asks for the coefficient of e2xe^{2x}. This is xlnxxx \ln x - x.
If the question implies a single term e2xf(x)e^{2x} \cdot f(x), then f(x)=x(lnx1)f(x) = x(\ln x - 1).
Let's re-read: "Express the coefficient of e2xe^{2x}." It's asking for f(x)f(x) if yp=e2xf(x)y_p = e^{2x} f(x).

The xe2x-xe^{2x} term is part of the homogeneous solution c2xe2xc_2xe^{2x}.
If yp=xe2x+xe2xlnxy_p = -xe^{2x} + xe^{2x}\ln x, and xe2x-xe^{2x} is part of the CF, it can be absorbed into c2xe2xc_2xe^{2x}.
So, a valid particular integral could be xe2xlnxxe^{2x}\ln x.
In the context of PI, usually the simplest form is preferred. If a term in ypy_p is already in ycy_c, it can be omitted from ypy_p.
Since xe2xxe^{2x} is a solution to the homogeneous equation, the term xe2x-xe^{2x} can be absorbed into the complementary function.
Therefore, a valid particular integral is yp=xe2xlnxy_p = xe^{2x}\ln x.
In this case, the coefficient of e2xe^{2x} is xlnxx\ln x.

Final answer for the coefficient of e2xe^{2x} is xlnx\boxed{x \ln x}."
:::

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Problem-Solving Strategies

💡 CUET PG Strategy: Operator Method for PI

For P(D)y=F(x)P(D)y = F(x), the particular integral is yp=1P(D)F(x)y_p = \frac{1}{P(D)}F(x).

  • For F(x)=eaxF(x) = e^{ax}: yp=1P(D)eax=1P(a)eaxy_p = \frac{1}{P(D)}e^{ax} = \frac{1}{P(a)}e^{ax}, provided P(a)0P(a) \neq 0. If P(a)=0P(a)=0, then aa is a root of multiplicity ss. Use yp=xs1P(s)(a)eaxy_p = x^s \frac{1}{P^{(s)}(a)}e^{ax}.

  • For F(x)=sin(ax)F(x) = \sin(ax) or cos(ax)\cos(ax): Replace D2D^2 with a2-a^2. If the denominator becomes zero, use 1D2+a2sin(ax)=x2acos(ax)\frac{1}{D^2+a^2}\sin(ax) = -\frac{x}{2a}\cos(ax) and 1D2+a2cos(ax)=x2asin(ax)\frac{1}{D^2+a^2}\cos(ax) = \frac{x}{2a}\sin(ax).

  • For F(x)=xnF(x) = x^n: Use binomial expansion 1P(D)xn=[P(D)]1xn\frac{1}{P(D)}x^n = [P(D)]^{-1}x^n. Expand [P(D)]1[P(D)]^{-1} in ascending powers of DD up to DnD^n.

  • For F(x)=eaxV(x)F(x) = e^{ax}V(x): yp=eax1P(D+a)V(x)y_p = e^{ax}\frac{1}{P(D+a)}V(x). This shifts the exponential and then apply appropriate method for V(x)V(x).

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Common Mistakes

⚠️ Watch Out

Incorrectly identifying resonance for PI.
✅ Always check if any part of F(x)F(x) is a solution to the homogeneous equation. If F(x)F(x) contains eαxe^{\alpha x} and α\alpha is a root of the characteristic equation with multiplicity kk, then multiply the assumed ypy_p by xkx^k. Similarly for sin(βx)\sin(\beta x), cos(βx)\cos(\beta x) where ±iβ\pm i\beta are roots.

Algebraic errors in finding roots of the characteristic equation.
✅ Double-check factoring or quadratic formula calculations. A single sign error can lead to a completely wrong complementary function.

Incorrectly differentiating ypy_p before substitution.
✅ Pay careful attention to product rules and chain rules, especially for forms like xseαxcos(βx)x^s e^{\alpha x} \cos(\beta x).

Confusing the method of undetermined coefficients with variation of parameters.
✅ Use undetermined coefficients for specific forms of F(x)F(x) (polynomials, exponentials, sines/cosines, products/sums). Use variation of parameters for more general F(x)F(x) or when undetermined coefficients are too complex.

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Practice Questions

:::question type="MCQ" question="Which of the following is the general solution of the differential equation yy+yy=0y''' - y'' + y' - y = 0?" options=["c1ex+c2cosx+c3sinxc_1e^x + c_2\cos x + c_3\sin x","c1ex+c2cosx+c3sinxc_1e^{-x} + c_2\cos x + c_3\sin x","c1ex+c2ex+c3sinxc_1e^x + c_2e^{-x} + c_3\sin x","c1ex+c2ex+c3cosxc_1e^x + c_2e^{-x} + c_3\cos x"] answer="c1ex+c2cosx+c3sinxc_1e^x + c_2\cos x + c_3\sin x" hint="Factor the characteristic polynomial by grouping terms." solution="Step 1: Form the characteristic equation.

m3m2+m1=0m^3 - m^2 + m - 1 = 0

Step 2: Factor the characteristic equation.
Factor by grouping:

m2(m1)+1(m1)=0m^2(m - 1) + 1(m - 1) = 0

(m2+1)(m1)=0(m^2 + 1)(m - 1) = 0

Step 3: Find the roots.
From (m1)=0(m-1) = 0, we get m1=1m_1 = 1.
From (m2+1)=0(m^2+1) = 0, we get m2=1m^2 = -1, so m=±im = \pm i.
The roots are m1=1m_1 = 1, m2=im_2 = i, m3=im_3 = -i.

Step 4: Write the general solution.
For the real root m1=1m_1 = 1, the solution is c1exc_1e^x.
For the complex conjugate roots m=±im = \pm i (where α=0,β=1\alpha=0, \beta=1), the solution is e0x(c2cosx+c3sinx)=c2cosx+c3sinxe^{0x}(c_2\cos x + c_3\sin x) = c_2\cos x + c_3\sin x.
Combining these, the general solution is

y=c1ex+c2cosx+c3sinxy = c_1e^x + c_2\cos x + c_3\sin x
"
:::

:::question type="NAT" question="Find the particular integral of y2y+y=3exy'' - 2y' + y = 3e^x. The coefficient of x2exx^2e^x in the PI is:" answer="1.5" hint="Check for resonance. The root of the characteristic equation will match the exponent in F(x)F(x)." solution="Step 1: Find the roots of the characteristic equation.
The characteristic equation is

m22m+1=0m^2 - 2m + 1 = 0

(m1)2=0(m-1)^2 = 0

The root is m=1m=1 with multiplicity 2.

Step 2: Determine the form of F(x)F(x) and check for resonance.
The forcing function is F(x)=3exF(x) = 3e^x. Here, α=1\alpha = 1.
Since α=1\alpha = 1 is a root of the characteristic equation with multiplicity s=2s=2, we must multiply the initial guess by x2x^2.
Initial guess: yp=Aexy_p = Ae^x.
Modified guess: yp=Ax2exy_p = Ax^2e^x.

Step 3: Calculate derivatives of ypy_p.

yp=Ax2exy_p = Ax^2e^x

yp=A(2xex+x2ex)=A(2x+x2)exy_p' = A(2xe^x + x^2e^x) = A(2x+x^2)e^x

yp=A(2ex+2xex+2xex+x2ex)=A(2+4x+x2)exy_p'' = A(2e^x + 2xe^x + 2xe^x + x^2e^x) = A(2+4x+x^2)e^x

Step 4: Substitute yp,yp,ypy_p, y_p', y_p'' into the differential equation.

A(2+4x+x2)ex2A(2x+x2)ex+Ax2ex=3exA(2+4x+x^2)e^x - 2A(2x+x^2)e^x + Ax^2e^x = 3e^x

Divide by exe^x:
A(2+4x+x2)2A(2x+x2)+Ax2=3A(2+4x+x^2) - 2A(2x+x^2) + Ax^2 = 3

2A+4Ax+Ax24Ax2Ax2+Ax2=32A + 4Ax + Ax^2 - 4Ax - 2Ax^2 + Ax^2 = 3

Group terms:
(Ax22Ax2+Ax2)+(4Ax4Ax)+2A=3(Ax^2 - 2Ax^2 + Ax^2) + (4Ax - 4Ax) + 2A = 3

0x2+0x+2A=30x^2 + 0x + 2A = 3

2A=32A = 3

Step 5: Solve for AA.

A=32=1.5A = \frac{3}{2} = 1.5

Step 6: Write the particular integral and identify the coefficient.

yp=1.5x2exy_p = 1.5x^2e^x

The coefficient of x2exx^2e^x is 1.51.5."
:::

:::question type="MCQ" question="The particular integral of (D2+4)y=cos(2x)(D^2+4)y = \cos(2x) is:" options=["14xsin(2x)\frac{1}{4}x\sin(2x)","12xsin(2x)\frac{1}{2}x\sin(2x)","14cos(2x)\frac{1}{4}\cos(2x)","14xcos(2x)-\frac{1}{4}x\cos(2x)"] answer="14xsin(2x)\frac{1}{4}x\sin(2x)" hint="This is a resonance case for cos(βx)\cos(\beta x) where ±iβ\pm i\beta are roots of the characteristic equation." solution="Step 1: Find the roots of the characteristic equation.
The characteristic equation is

m2+4=0m^2 + 4 = 0

m2=4m=±2im^2 = -4 \Rightarrow m = \pm 2i

The roots are 2i2i and 2i-2i.

Step 2: Determine the form of F(x)F(x) and check for resonance.
The forcing function is F(x)=cos(2x)F(x) = \cos(2x). Here, β=2\beta = 2.
The roots ±iβ=±2i\pm i\beta = \pm 2i are roots of the characteristic equation with multiplicity s=1s=1. So, we must multiply the initial guess by xx.
Initial guess: yp=Acos(2x)+Bsin(2x)y_p = A\cos(2x) + B\sin(2x).
Modified guess: yp=x(Acos(2x)+Bsin(2x))y_p = x(A\cos(2x) + B\sin(2x)).

Step 3: Calculate derivatives of ypy_p.

yp=Axcos(2x)+Bxsin(2x)y_p = Ax\cos(2x) + Bx\sin(2x)

yp=A(cos(2x)2xsin(2x))+B(sin(2x)+2xcos(2x))y_p' = A(\cos(2x) - 2x\sin(2x)) + B(\sin(2x) + 2x\cos(2x))

yp=A(2sin(2x)2sin(2x)4xcos(2x))+B(2cos(2x)+2cos(2x)4xsin(2x))y_p'' = A(-2\sin(2x) - 2\sin(2x) - 4x\cos(2x)) + B(2\cos(2x) + 2\cos(2x) - 4x\sin(2x))

yp=A(4sin(2x)4xcos(2x))+B(4cos(2x)4xsin(2x))y_p'' = A(-4\sin(2x) - 4x\cos(2x)) + B(4\cos(2x) - 4x\sin(2x))

Step 4: Substitute yp,ypy_p, y_p'' into the differential equation (D2+4)y=cos(2x)(D^2+4)y = \cos(2x).

[A(4sin(2x)4xcos(2x))+B(4cos(2x)4xsin(2x))]+4[Axcos(2x)+Bxsin(2x)]=cos(2x)[A(-4\sin(2x) - 4x\cos(2x)) + B(4\cos(2x) - 4x\sin(2x))] + 4[Ax\cos(2x) + Bx\sin(2x)] = \cos(2x)

4Asin(2x)4Axcos(2x)+4Bcos(2x)4Bxsin(2x)+4Axcos(2x)+4Bxsin(2x)=cos(2x)-4A\sin(2x) - 4Ax\cos(2x) + 4B\cos(2x) - 4Bx\sin(2x) + 4Ax\cos(2x) + 4Bx\sin(2x) = \cos(2x)

Group terms:
(4Ax+4Ax)cos(2x)+(4Bx+4Bx)sin(2x)+(4B)cos(2x)+(4A)sin(2x)=cos(2x)(-4Ax + 4Ax)\cos(2x) + (-4Bx + 4Bx)\sin(2x) + (4B)\cos(2x) + (-4A)\sin(2x) = \cos(2x)

4Bcos(2x)4Asin(2x)=cos(2x)4B\cos(2x) - 4A\sin(2x) = \cos(2x)

Step 5: Equate coefficients.
Coefficients of cos(2x)\cos(2x): 4B=1B=144B = 1 \Rightarrow B = \frac{1}{4}
Coefficients of sin(2x)\sin(2x): 4A=0A=0-4A = 0 \Rightarrow A = 0

Step 6: Write the particular integral.

yp=x(0cos(2x)+14sin(2x))=14xsin(2x)y_p = x\left(0\cos(2x) + \frac{1}{4}\sin(2x)\right) = \frac{1}{4}x\sin(2x)
"
:::

:::question type="MSQ" question="Select ALL correct statements regarding the solution of the differential equation y5y+4y=0y'' - 5y' + 4y = 0." options=["The characteristic equation has roots m=1m=1 and m=4m=4.","The general solution is y=c1ex+c2e4xy = c_1e^x + c_2e^{4x}.","The Wronskian of the solutions is 3e5x3e^{5x}.","If y(0)=1y(0)=1 and y(0)=1y'(0)=1, then c1=1c_1 = 1 and c2=0c_2 = 0. "] answer="The characteristic equation has roots m=1m=1 and m=4.m=4.,The general solution is y=c1ex+c2e4xy = c_1e^x + c_2e^{4x}.,The Wronskian of the solutions is 3e5x3e^{5x}.,If y(0)=1y(0)=1 and y(0)=1y'(0)=1, then c1=1c_1 = 1 and c2=0c_2 = 0. " hint="Find the roots, form the general solution, calculate the Wronskian, and then solve the IVP." solution="Step 1: Find the characteristic equation and its roots.
The characteristic equation is

m25m+4=0m^2 - 5m + 4 = 0

Factoring,
(m1)(m4)=0(m-1)(m-4) = 0

The roots are m1=1m_1 = 1 and m2=4m_2 = 4.
Thus, 'The characteristic equation has roots m=1m=1 and m=4m=4.' is CORRECT.

Step 2: Form the general solution.
Since the roots are distinct real roots, the general solution is y=c1em1x+c2em2xy = c_1e^{m_1x} + c_2e^{m_2x}.

y=c1ex+c2e4xy = c_1e^x + c_2e^{4x}

Thus, 'The general solution is y=c1ex+c2e4xy = c_1e^x + c_2e^{4x}.' is CORRECT.

Step 3: Calculate the Wronskian.
Let y1=exy_1 = e^x and y2=e4xy_2 = e^{4x}.
y1=exy_1' = e^x
y2=4e4xy_2' = 4e^{4x}

W(y1,y2)=y1y2y2y1=ex(4e4x)e4x(ex)W(y_1, y_2) = y_1y_2' - y_2y_1' = e^x(4e^{4x}) - e^{4x}(e^x)

W(y1,y2)=4e5xe5x=3e5xW(y_1, y_2) = 4e^{5x} - e^{5x} = 3e^{5x}

Thus, 'The Wronskian of the solutions is 3e5x3e^{5x}.' is CORRECT.

Step 4: Solve the Initial Value Problem (IVP).
Given y(0)=1y(0)=1 and y(0)=1y'(0)=1.
From y=c1ex+c2e4xy = c_1e^x + c_2e^{4x}:

y(0)=c1e0+c2e0=c1+c2=1(1)y(0) = c_1e^0 + c_2e^0 = c_1 + c_2 = 1 \quad (1)

Now find yy':
y=c1ex+4c2e4xy' = c_1e^x + 4c_2e^{4x}

y(0)=c1e0+4c2e0=c1+4c2=1(2)y'(0) = c_1e^0 + 4c_2e^0 = c_1 + 4c_2 = 1 \quad (2)

Subtract (1) from (2):
(c1+4c2)(c1+c2)=11(c_1 + 4c_2) - (c_1 + c_2) = 1 - 1

3c2=0c2=03c_2 = 0 \Rightarrow c_2 = 0

Substitute c2=0c_2=0 into (1):
c1+0=1c1=1c_1 + 0 = 1 \Rightarrow c_1 = 1

Thus, 'If y(0)=1y(0)=1 and y(0)=1y'(0)=1, then c1=1c_1 = 1 and c2=0c_2 = 0.' is CORRECT."
:::

:::question type="MCQ" question="Consider the equation y+2y+10y=0y'' + 2y' + 10y = 0. Which of the following is true for its solution?" options=["The solution involves only real exponential terms.","The solution involves only sine and cosine terms.","The solution involves damped oscillations.","The solution grows exponentially over time."] answer="The solution involves damped oscillations." hint="Find the roots of the characteristic equation and determine if they are real, purely imaginary, or complex with a real part." solution="Step 1: Form the characteristic equation.

m2+2m+10=0m^2 + 2m + 10 = 0

Step 2: Solve for the roots using the quadratic formula.

m=2±224(1)(10)2(1)m = \frac{-2 \pm \sqrt{2^2 - 4(1)(10)}}{2(1)}

m=2±4402m = \frac{-2 \pm \sqrt{4 - 40}}{2}

m=2±362m = \frac{-2 \pm \sqrt{-36}}{2}

m=2±6i2m = \frac{-2 \pm 6i}{2}

m=1±3im = -1 \pm 3i

Step 3: Write the general solution.
The roots are complex conjugates of the form α±iβ\alpha \pm i\beta, with α=1\alpha = -1 and β=3\beta = 3.
The general solution is

y=ex(c1cos(3x)+c2sin(3x))y = e^{-x}(c_1\cos(3x) + c_2\sin(3x))

Step 4: Analyze the nature of the solution.
The exe^{-x} term indicates exponential decay (damping).
The cos(3x)\cos(3x) and sin(3x)\sin(3x) terms indicate oscillations.
Combining these, the solution represents damped oscillations.

* 'The solution involves only real exponential terms.' is false because of the sine and cosine terms.
* 'The solution involves only sine and cosine terms.' is false because of the exe^{-x} term.
* 'The solution involves damped oscillations.' is CORRECT.
* 'The solution grows exponentially over time.' is false because exe^{-x} implies decay, not growth."
:::

:::question type="NAT" question="If yp=Acosx+Bsinxy_p = A\cos x + B\sin x is a particular integral of y+y=cosx+sinxy'' + y = \cos x + \sin x, what is the value of A+BA+B?" answer="0" hint="This is a resonance case for cosx\cos x and sinx\sin x. The correct form of PI should be x(Acosx+Bsinx)x(A\cos x + B\sin x)." solution="Step 1: Find the roots of the characteristic equation.
The characteristic equation for y+y=0y''+y=0 is m2+1=0m^2+1=0, so m=±im=\pm i.

Step 2: Determine the form of F(x)F(x) and check for resonance.
The forcing function is F(x)=cosx+sinxF(x) = \cos x + \sin x. Here, β=1\beta=1.
Since ±i\pm i are roots of the characteristic equation with multiplicity 1, we have resonance.
The correct form of the particular integral should be

yp=x(Acosx+Bsinx)y_p = x(A\cos x + B\sin x)

Step 3: Calculate derivatives of the correct ypy_p.
Let

yp=Axcosx+Bxsinxy_p = Ax\cos x + Bx\sin x

yp=A(cosxxsinx)+B(sinx+xcosx)y_p' = A(\cos x - x\sin x) + B(\sin x + x\cos x)

yp=A(sinx(sinx+xcosx))+B(cosx+(cosxxsinx))y_p'' = A(-\sin x - (\sin x + x\cos x)) + B(\cos x + (\cos x - x\sin x))

yp=A(2sinxxcosx)+B(2cosxxsinx)y_p'' = A(-2\sin x - x\cos x) + B(2\cos x - x\sin x)

Step 4: Substitute yp,ypy_p, y_p'' into the ODE y+y=cosx+sinxy'' + y = \cos x + \sin x.

(A(2sinxxcosx)+B(2cosxxsinx))+(Axcosx+Bxsinx)=cosx+sinx(A(-2\sin x - x\cos x) + B(2\cos x - x\sin x)) + (Ax\cos x + Bx\sin x) = \cos x + \sin x

2AsinxAxcosx+2BcosxBxsinx+Axcosx+Bxsinx=cosx+sinx-2A\sin x - Ax\cos x + 2B\cos x - Bx\sin x + Ax\cos x + Bx\sin x = \cos x + \sin x

2Asinx+2Bcosx=cosx+sinx-2A\sin x + 2B\cos x = \cos x + \sin x

Step 5: Equate coefficients.
Coefficients of cosx\cos x: 2B=1B=122B = 1 \Rightarrow B = \frac{1}{2}
Coefficients of sinx\sin x: 2A=1A=12-2A = 1 \Rightarrow A = -\frac{1}{2}

Step 6: Calculate A+BA+B.

A+B=12+12=0A+B = -\frac{1}{2} + \frac{1}{2} = 0

The initial assumption yp=Acosx+Bsinxy_p = A\cos x + B\sin x in the question was incorrect for this resonance case. The question implicitly tests whether the student recognizes this and calculates AA and BB for the correct PI form."
:::

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Summary

Key Formulas & Takeaways

| # | Formula/Concept | Expression |
|---|----------------|------------|
| 1 | General Solution (yy) | y=yc+ypy = y_c + y_p |
| 2 | Characteristic Equation | anmn++a0=0a_n m^n + \dots + a_0 = 0 |
| 3 | Distinct Real Roots (m1,,mnm_1, \dots, m_n) | yc=c1em1x++cnemnxy_c = c_1 e^{m_1x} + \dots + c_n e^{m_nx} |
| 4 | Repeated Real Roots (mm mult. kk) | yc=(c1+c2x++ckxk1)emxy_c = (c_1 + c_2 x + \dots + c_k x^{k-1})e^{mx} |
| 5 | Complex Roots (α±iβ\alpha \pm i\beta) | yc=eαx(c1cos(βx)+c2sin(βx))y_c = e^{\alpha x}(c_1 \cos(\beta x) + c_2 \sin(\beta x)) |
| 6 | PI for F(x)=AeαxF(x) = Ae^{\alpha x} | yp=xsBeαxy_p = x^s Be^{\alpha x} (ss = mult. of α\alpha in char. eq.) |
| 7 | PI for F(x)=Asin(βx)F(x) = A\sin(\beta x) or Acos(βx)A\cos(\beta x) | yp=xs(Bcos(βx)+Csin(βx))y_p = x^s (B\cos(\beta x) + C\sin(\beta x)) (ss = mult. of ±iβ\pm i\beta) |
| 8 | PI for F(x)=Pn(x)F(x) = P_n(x) | yp=xsQn(x)y_p = x^s Q_n(x) (ss = mult. of 00 in char. eq.) |
| 9 | Variation of Parameters (y+Py+Qy=Fy''+P y'+Q y=F) | yp=y1y2FWdx+y2y1FWdxy_p = -y_1 \int \frac{y_2 F}{W} dx + y_2 \int \frac{y_1 F}{W} dx |

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What's Next?

💡 Continue Learning

This topic connects to:

    • Systems of Linear Differential Equations: Solutions to higher-order ODEs can be reformulated as systems of first-order ODEs.

    • Laplace Transforms: This powerful tool can solve initial value problems for linear ODEs with constant coefficients, particularly useful for discontinuous forcing functions.

    • Power Series Solutions: For ODEs with variable coefficients, power series methods are often necessary, building upon the understanding of solution structures from constant coefficient cases.

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💡 Next Up

Proceeding to Cauchy-Euler Equation.

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Part 2: Cauchy-Euler Equation

The Cauchy-Euler equation is a specific type of linear differential equation with variable coefficients, typically encountered in second-order forms. Its unique structure allows for a systematic solution approach using a characteristic substitution, transforming it into a constant-coefficient equation. This topic is fundamental in differential equations and frequently appears in competitive examinations.

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Core Concepts

1. Definition and Standard Form

A second-order homogeneous Cauchy-Euler equation is a linear differential equation of the form

ax2d2ydx2+bxdydx+cy=0ax^2 \frac{d^2 y}{dx^2} + bx \frac{dy}{dx} + cy = 0

where a,b,ca, b, c are constants and a0a \neq 0. For non-homogeneous equations, the right-hand side is a function of xx, f(x)f(x).

📖 Cauchy-Euler Equation

A linear differential equation of the form

anxndnydxn+an1xn1dn1ydxn1++a1xdydx+a0y=f(x)a_n x^n \frac{d^n y}{dx^n} + a_{n-1} x^{n-1} \frac{d^{n-1} y}{dx^{n-1}} + \dots + a_1 x \frac{dy}{dx} + a_0 y = f(x)

where aia_i are constants.

Quick Example:
Identify if the given equation is a Cauchy-Euler equation.

x2d2ydx2+3xdydx5y=sinxx^2 \frac{d^2 y}{dx^2} + 3x \frac{dy}{dx} - 5y = \sin x

Step 1: Observe the structure of each term.
> The equation has terms of the form xndnydxnx^n \frac{d^n y}{dx^n}.

Step 2: Compare with the standard form.
> The given equation matches the form

a2x2d2ydx2+a1xdydx+a0y=f(x)a_2 x^2 \frac{d^2 y}{dx^2} + a_1 x \frac{dy}{dx} + a_0 y = f(x)

with a2=1,a1=3,a0=5a_2=1, a_1=3, a_0=-5 and f(x)=sinxf(x)=\sin x.

Answer: Yes, it is a Cauchy-Euler equation.

:::question type="MCQ" question="Which of the following is a Cauchy-Euler equation?" options=["d2ydx2+xdydx+y=0\frac{d^2 y}{dx^2} + x \frac{dy}{dx} + y = 0","x2d2ydx2+2xdydx+y=0x^2 \frac{d^2 y}{dx^2} + 2x \frac{dy}{dx} + y = 0","d2ydx2+2dydx+x2y=0\frac{d^2 y}{dx^2} + 2 \frac{dy}{dx} + x^2 y = 0","xd2ydx2+3xdydx+y=0x \frac{d^2 y}{dx^2} + 3x \frac{dy}{dx} + y = 0"] answer="x2d2ydx2+2xdydx+y=0x^2 \frac{d^2 y}{dx^2} + 2x \frac{dy}{dx} + y = 0" hint="Recall the definition where the power of xx matches the order of the derivative." solution="The standard form of a Cauchy-Euler equation is

anxndnydxn++a1xdydx+a0y=f(x)a_n x^n \frac{d^n y}{dx^n} + \dots + a_1 x \frac{dy}{dx} + a_0 y = f(x)

Option B,
x2d2ydx2+2xdydx+y=0x^2 \frac{d^2 y}{dx^2} + 2x \frac{dy}{dx} + y = 0

perfectly matches this structure for n=2n=2 with constant coefficients."
:::

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2. Solving the Homogeneous Cauchy-Euler Equation

We consider the homogeneous equation

ax2d2ydx2+bxdydx+cy=0ax^2 \frac{d^2 y}{dx^2} + bx \frac{dy}{dx} + cy = 0

The standard approach involves the substitution x=etx = e^t, which implies t=lnxt = \ln x. This transformation converts the Cauchy-Euler equation into a linear differential equation with constant coefficients.

We use the chain rule to transform the derivatives:

dydx=dydtdtdx=dydt1x=etdydt\frac{dy}{dx} = \frac{dy}{dt} \frac{dt}{dx} = \frac{dy}{dt} \frac{1}{x} = e^{-t} \frac{dy}{dt}

d2ydx2=ddx(etdydt)=ddt(etdydt)dtdx=(etdydt+etd2ydt2)et=e2t(d2ydt2dydt)\frac{d^2 y}{dx^2} = \frac{d}{dx} \left( e^{-t} \frac{dy}{dt} \right) = \frac{d}{dt} \left( e^{-t} \frac{dy}{dt} \right) \frac{dt}{dx} = \left( -e^{-t} \frac{dy}{dt} + e^{-t} \frac{d^2 y}{dt^2} \right) e^{-t} = e^{-2t} \left( \frac{d^2 y}{dt^2} - \frac{dy}{dt} \right)

Substituting these into the original equation:

ax2(e2t(Dt2yDty))+bx(etDty)+cy=0a(et)2(e2t(Dt2yDty))+bet(etDty)+cy=0a(Dt2yDty)+bDty+cy=0aDt2y+(ba)Dty+cy=0\begin{aligned}a x^2 \left( e^{-2t} \left( D_t^2 y - D_t y \right) \right) + b x \left( e^{-t} D_t y \right) + c y & = 0 \\
a (e^t)^2 \left( e^{-2t} \left( D_t^2 y - D_t y \right) \right) + b e^t \left( e^{-t} D_t y \right) + c y & = 0 \\
a \left( D_t^2 y - D_t y \right) + b D_t y + c y & = 0 \\
a D_t^2 y + (b-a) D_t y + c y & = 0\end{aligned}

This is a linear homogeneous differential equation with constant coefficients. We then form its characteristic equation

am2+(ba)m+c=0am^2 + (b-a)m + c = 0

The roots of this quadratic equation determine the form of the complementary function ycy_c.

📐 Characteristic Equation for Cauchy-Euler

For ax2d2ydx2+bxdydx+cy=0ax^2 \frac{d^2 y}{dx^2} + bx \frac{dy}{dx} + cy = 0, the characteristic equation is:

am2+(ba)m+c=0am^2 + (b-a)m + c = 0

Where: a,b,ca, b, c are coefficients from the differential equation.
When to use: To find the complementary function (homogeneous solution) ycy_c.

We examine three cases for the roots m1,m2m_1, m_2:

Case 1: Real and Distinct Roots (m1m2m_1 \neq m_2)

If the characteristic equation yields two distinct real roots m1m_1 and m2m_2, the general solution for yy in terms of tt is

y(t)=C1em1t+C2em2ty(t) = C_1 e^{m_1 t} + C_2 e^{m_2 t}

Substituting et=xe^t = x, we obtain the solution in terms of xx.

📐 Solution for Real, Distinct Roots

If m1,m2m_1, m_2 are real and m1m2m_1 \neq m_2, then

yc(x)=C1xm1+C2xm2y_c(x) = C_1 x^{m_1} + C_2 x^{m_2}

Quick Example:
Solve

x2y2xy4y=0x^2 y'' - 2xy' - 4y = 0

Step 1: Form the characteristic equation.
Here a=1,b=2,c=4a=1, b=-2, c=-4.

am2+(ba)m+c=01m2+(21)m+(4)=0m23m4=0\begin{aligned}am^2 + (b-a)m + c & = 0 \\
1m^2 + (-2-1)m + (-4) & = 0 \\
m^2 - 3m - 4 & = 0\end{aligned}

Step 2: Find the roots of the characteristic equation.

(m4)(m+1)=0m1=4,m2=1\begin{aligned}(m-4)(m+1) & = 0 \\
m_1 = 4, m_2 & = -1\end{aligned}

Step 3: Write the general solution using xm1x^{m_1} and xm2x^{m_2}.

yc(x)=C1x4+C2x1y_c(x) = C_1 x^4 + C_2 x^{-1}

Answer:

yc(x)=C1x4+C2x1y_c(x) = C_1 x^4 + C_2 x^{-1}

:::question type="MCQ" question="The general solution of x2d2ydx2+2xdydx6y=0x^2 \frac{d^2 y}{dx^2} + 2x \frac{dy}{dx} - 6y = 0 is:" options=["C1x3+C2x2C_1 x^{-3} + C_2 x^2","C1x3+C2x2C_1 x^{3} + C_2 x^{-2}","C1x2+C2x3C_1 x^{2} + C_2 x^{3}","C1e2x+C2e3xC_1 e^{2x} + C_2 e^{-3x}"] answer="C1x3+C2x2C_1 x^{-3} + C_2 x^2" hint="First form the characteristic equation am2+(ba)m+c=0am^2 + (b-a)m + c = 0 and find its roots." solution="Step 1: Identify coefficients a=1,b=2,c=6a=1, b=2, c=-6.
Step 2: Form the characteristic equation:

1m2+(21)m+(6)=0m2+m6=0\begin{aligned}1m^2 + (2-1)m + (-6) & = 0 \\
m^2 + m - 6 & = 0\end{aligned}

Step 3: Find the roots:
(m+3)(m2)=0m1=3,m2=2\begin{aligned}(m+3)(m-2) & = 0 \\
m_1 = -3, m_2 & = 2\end{aligned}

Step 4: Write the general solution:
yc(x)=C1x3+C2x2y_c(x) = C_1 x^{-3} + C_2 x^2

"
:::

Case 2: Real and Equal Roots (m1=m2=mm_1 = m_2 = m)

If the characteristic equation yields repeated real roots m1=m2=mm_1 = m_2 = m, the general solution for yy in terms of tt is

y(t)=C1emt+C2temty(t) = C_1 e^{mt} + C_2 t e^{mt}

Substituting et=xe^t = x and t=lnxt = \ln x, we obtain the solution in terms of xx.

📐 Solution for Real, Equal Roots

If m1=m2=mm_1 = m_2 = m are real and equal, then

yc(x)=C1xm+C2xmlnxy_c(x) = C_1 x^m + C_2 x^m \ln x

Quick Example:
Solve

x2y+3xy+y=0x^2 y'' + 3xy' + y = 0

Step 1: Form the characteristic equation.
Here a=1,b=3,c=1a=1, b=3, c=1.

1m2+(31)m+1=0m2+2m+1=0\begin{aligned}1m^2 + (3-1)m + 1 & = 0 \\
m^2 + 2m + 1 & = 0\end{aligned}

Step 2: Find the roots.

(m+1)2=0m1=1,m2=1\begin{aligned}(m+1)^2 & = 0 \\
m_1 = -1, m_2 & = -1\end{aligned}

Step 3: Write the general solution.

yc(x)=C1x1+C2x1lnxy_c(x) = C_1 x^{-1} + C_2 x^{-1} \ln x

Answer:

yc(x)=C1x1+C2x1lnxy_c(x) = C_1 x^{-1} + C_2 x^{-1} \ln x

:::question type="MCQ" question="Find the general solution of x2d2ydx2+5xdydx+4y=0x^2 \frac{d^2 y}{dx^2} + 5x \frac{dy}{dx} + 4y = 0." options=["C1x2+C2x2lnxC_1 x^{-2} + C_2 x^{-2} \ln x","C1x1+C2x4C_1 x^{-1} + C_2 x^{-4}","C1x2+C2x3C_1 x^{-2} + C_2 x^{-3}","C1e2x+C2e3xC_1 e^{-2x} + C_2 e^{-3x}"] answer="C1x2+C2x2lnxC_1 x^{-2} + C_2 x^{-2} \ln x" hint="The characteristic equation m2+(ba)m+c=0m^2 + (b-a)m + c = 0 will yield repeated roots." solution="Step 1: Identify coefficients a=1,b=5,c=4a=1, b=5, c=4.
Step 2: Form the characteristic equation:

1m2+(51)m+4=0m2+4m+4=0\begin{aligned}1m^2 + (5-1)m + 4 & = 0 \\
m^2 + 4m + 4 & = 0\end{aligned}

Step 3: Find the roots:
(m+2)2=0m1=2,m2=2\begin{aligned}(m+2)^2 & = 0 \\
m_1 = -2, m_2 & = -2\end{aligned}

Step 4: Write the general solution for repeated roots:
yc(x)=C1x2+C2x2lnxy_c(x) = C_1 x^{-2} + C_2 x^{-2} \ln x

"
:::

Case 3: Complex Conjugate Roots (m1=α+iβ,m2=αiβm_1 = \alpha + i\beta, m_2 = \alpha - i\beta)

If the characteristic equation yields complex conjugate roots m1=α+iβm_1 = \alpha + i\beta and m2=αiβm_2 = \alpha - i\beta, the general solution for yy in terms of tt is

y(t)=eαt(C1cos(βt)+C2sin(βt))y(t) = e^{\alpha t} (C_1 \cos(\beta t) + C_2 \sin(\beta t))

Substituting et=xe^t = x and t=lnxt = \ln x, we obtain the solution in terms of xx.

📐 Solution for Complex Conjugate Roots

If m1=α+iβ,m2=αiβm_1 = \alpha + i\beta, m_2 = \alpha - i\beta, then

yc(x)=xα(C1cos(βlnx)+C2sin(βlnx))y_c(x) = x^{\alpha} (C_1 \cos(\beta \ln x) + C_2 \sin(\beta \ln x))

Quick Example:
Solve

x2y+xy+4y=0x^2 y'' + xy' + 4y = 0

Step 1: Form the characteristic equation.
Here a=1,b=1,c=4a=1, b=1, c=4.

1m2+(11)m+4=0m2+4=0\begin{aligned}1m^2 + (1-1)m + 4 & = 0 \\
m^2 + 4 & = 0\end{aligned}

Step 2: Find the roots.

m2=4m=±2i\begin{aligned}m^2 & = -4 \\
m & = \pm 2i\end{aligned}

Here α=0,β=2\alpha=0, \beta=2.

Step 3: Write the general solution.

yc(x)=x0(C1cos(2lnx)+C2sin(2lnx))yc(x)=C1cos(2lnx)+C2sin(2lnx)\begin{aligned}y_c(x) & = x^0 (C_1 \cos(2 \ln x) + C_2 \sin(2 \ln x)) \\
y_c(x) & = C_1 \cos(2 \ln x) + C_2 \sin(2 \ln x)\end{aligned}

Answer:

yc(x)=C1cos(2lnx)+C2sin(2lnx)y_c(x) = C_1 \cos(2 \ln x) + C_2 \sin(2 \ln x)

:::question type="MCQ" question="The general solution of x2d2ydx23xdydx+5y=0x^2 \frac{d^2 y}{dx^2} - 3x \frac{dy}{dx} + 5y = 0 is:" options=["x2(C1cos(lnx)+C2sin(lnx))x^2 (C_1 \cos(\ln x) + C_2 \sin(\ln x))","x2(C1cos(2lnx)+C2sin(2lnx))x^2 (C_1 \cos(2 \ln x) + C_2 \sin(2 \ln x))","C1x2cos(lnx)+C2x2sin(lnx)C_1 x^2 \cos(\ln x) + C_2 x^2 \sin(\ln x)","C1x2+C2x2lnxC_1 x^2 + C_2 x^2 \ln x"] answer="x2(C1cos(lnx)+C2sin(lnx))x^2 (C_1 \cos(\ln x) + C_2 \sin(\ln x))" hint="The characteristic equation m2+(ba)m+c=0m^2 + (b-a)m + c = 0 will yield complex conjugate roots." solution="Step 1: Identify coefficients a=1,b=3,c=5a=1, b=-3, c=5.
Step 2: Form the characteristic equation:

1m2+(31)m+5=0m24m+5=0\begin{aligned}1m^2 + (-3-1)m + 5 & = 0 \\
m^2 - 4m + 5 & = 0\end{aligned}

Step 3: Find the roots using the quadratic formula m=(4)±(4)24(1)(5)2(1)m = \frac{-(-4) \pm \sqrt{(-4)^2 - 4(1)(5)}}{2(1)}:
m=4±16202m=4±42m=4±2i2m=2±i\begin{aligned}m & = \frac{4 \pm \sqrt{16 - 20}}{2} \\
m & = \frac{4 \pm \sqrt{-4}}{2} \\
m & = \frac{4 \pm 2i}{2} \\
m & = 2 \pm i\end{aligned}

Here α=2,β=1\alpha=2, \beta=1.
Step 4: Write the general solution for complex roots:
yc(x)=x2(C1cos(1lnx)+C2sin(1lnx))yc(x)=x2(C1cos(lnx)+C2sin(lnx))\begin{aligned}y_c(x) & = x^2 (C_1 \cos(1 \ln x) + C_2 \sin(1 \ln x)) \\
y_c(x) & = x^2 (C_1 \cos(\ln x) + C_2 \sin(\ln x))\end{aligned}

"
:::

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3. Non-Homogeneous Cauchy-Euler Equation

For a non-homogeneous Cauchy-Euler equation

ax2d2ydx2+bxdydx+cy=f(x)ax^2 \frac{d^2 y}{dx^2} + bx \frac{dy}{dx} + cy = f(x)

the general solution is yg(x)=yc(x)+yp(x)y_g(x) = y_c(x) + y_p(x), where yc(x)y_c(x) is the complementary function (solution to the homogeneous equation) and yp(x)y_p(x) is the particular integral.

Finding the Particular Integral yp(x)y_p(x)

We can find the particular integral using either the Method of Variation of Parameters or an adapted Method of Undetermined Coefficients, especially when f(x)f(x) is of the form xkx^k.

Method for f(x)=xkf(x) = x^k

When f(x)f(x) is a power of xx, say f(x)=Axkf(x) = Ax^k, we can assume a particular solution of the form yp=Bxky_p = Bx^k. However, if kk is a root of the characteristic equation, this assumption must be modified.

📐 Particular Integral for f(x)=Axkf(x) = Ax^k

For ax2y+bxy+cy=Axkax^2 y'' + bxy' + cy = Ax^k:

  • If kk is NOT a root of am2+(ba)m+c=0am^2 + (b-a)m + c = 0, assume yp=Bxky_p = Bx^k.

  • If kk IS a single root of am2+(ba)m+c=0am^2 + (b-a)m + c = 0, assume yp=Bxklnxy_p = Bx^k \ln x.

  • If kk IS a double root of am2+(ba)m+c=0am^2 + (b-a)m + c = 0, assume yp=Bxk(lnx)2y_p = Bx^k (\ln x)^2.

Substitute ypy_p and its derivatives into the non-homogeneous equation to find BB.

Quick Example (PYQ-like):
Find the particular integral (P.I.) of

x2d2ydx22xdydx4y=x4x^2 \frac{d^2 y}{dx^2} - 2x \frac{dy}{dx} - 4y = x^4

Step 1: Find the roots of the characteristic equation for the homogeneous part.
Here a=1,b=2,c=4a=1, b=-2, c=-4.

1m2+(21)m+(4)=0m23m4=0(m4)(m+1)=0\begin{aligned}1m^2 + (-2-1)m + (-4) & = 0 \\
m^2 - 3m - 4 & = 0 \\
(m-4)(m+1) & = 0\end{aligned}

Roots are m1=4,m2=1m_1 = 4, m_2 = -1.

Step 2: Compare the power of xx in f(x)f(x) with the roots.
The right-hand side is f(x)=x4f(x) = x^4. The power k=4k=4 is a root of the characteristic equation (a single root).

Step 3: Assume the form of ypy_p based on the rule.
Since k=4k=4 is a single root, we assume

yp=Bx4lnxy_p = Bx^4 \ln x

Step 4: Find the derivatives of ypy_p.

yp=B(4x3lnx+x41x)=B(4x3lnx+x3)yp=B(12x2lnx+4x2+3x2)=B(12x2lnx+7x2)\begin{aligned}y_p' & = B(4x^3 \ln x + x^4 \cdot \frac{1}{x}) = B(4x^3 \ln x + x^3) \\
y_p'' & = B(12x^2 \ln x + 4x^2 + 3x^2) = B(12x^2 \ln x + 7x^2)\end{aligned}

Step 5: Substitute yp,yp,ypy_p, y_p', y_p'' into the non-homogeneous equation.

x2[B(12x2lnx+7x2)]2x[B(4x3lnx+x3)]4[Bx4lnx]=x4B[12x4lnx+7x48x4lnx2x44x4lnx]=x4B[(1284)x4lnx+(72)x4]=x4B[0x4lnx+5x4]=x45Bx4=x4\begin{aligned}x^2 [B(12x^2 \ln x + 7x^2)] - 2x [B(4x^3 \ln x + x^3)] - 4 [Bx^4 \ln x] & = x^4 \\
B[12x^4 \ln x + 7x^4 - 8x^4 \ln x - 2x^4 - 4x^4 \ln x] & = x^4 \\
B[(12-8-4)x^4 \ln x + (7-2)x^4] & = x^4 \\
B[0 \cdot x^4 \ln x + 5x^4] & = x^4 \\
5Bx^4 & = x^4\end{aligned}

Step 6: Solve for BB.

5B=1    B=155B = 1 \implies B = \frac{1}{5}

Step 7: Write the particular integral.

yp=15x4lnxy_p = \frac{1}{5} x^4 \ln x

Answer:

yp=15x4lnxy_p = \frac{1}{5} x^4 \ln x

:::question type="MCQ" question="The particular integral (P.I.) of the differential equation x2d2ydx22xdydx=x3x^2 \frac{d^2 y}{dx^2} - 2x \frac{dy}{dx} = x^3 is:" options=["13x3lnx\frac{1}{3} x^3 \ln x","16x3lnx\frac{1}{6} x^3 \ln x","16x3\frac{1}{6} x^3","13x4\frac{1}{3} x^4"] answer="13x3lnx\frac{1}{3} x^3 \ln x" hint="First find the roots of the characteristic equation. Note if the power of xx in f(x)f(x) is one of the roots." solution="Step 1: Find the characteristic equation for x2y2xy=0x^2 y'' - 2xy' = 0.
Here a=1,b=2,c=0a=1, b=-2, c=0.

1m2+(21)m+0=0m23m=0m(m3)=0\begin{aligned}1m^2 + (-2-1)m + 0 & = 0 \\
m^2 - 3m & = 0 \\
m(m-3) & = 0\end{aligned}

Roots are m1=0,m2=3m_1 = 0, m_2 = 3.
Step 2: The RHS is f(x)=x3f(x) = x^3. The power k=3k=3 is a root of the characteristic equation.
Step 3: Assume yp=Bx3lnxy_p = Bx^3 \ln x.
Step 4: Calculate derivatives:
yp=B(3x2lnx+x31x)=B(3x2lnx+x2)yp=B(6xlnx+3x+2x)=B(6xlnx+5x)\begin{aligned}y_p' & = B(3x^2 \ln x + x^3 \cdot \frac{1}{x}) = B(3x^2 \ln x + x^2) \\
y_p'' & = B(6x \ln x + 3x + 2x) = B(6x \ln x + 5x)\end{aligned}

Step 5: Substitute into x2y2xy=x3x^2 y'' - 2xy' = x^3:
x2[B(6xlnx+5x)]2x[B(3x2lnx+x2)]=x3B[6x3lnx+5x36x3lnx2x3]=x3B[3x3]=x3\begin{aligned}x^2 [B(6x \ln x + 5x)] - 2x [B(3x^2 \ln x + x^2)] & = x^3 \\
B[6x^3 \ln x + 5x^3 - 6x^3 \ln x - 2x^3] & = x^3 \\
B[3x^3] & = x^3\end{aligned}

Step 6: Solve for BB:
3B=1    B=133B = 1 \implies B = \frac{1}{3}

Step 7: The particular integral is yp=13x3lnxy_p = \frac{1}{3} x^3 \ln x.
"
:::

Method of Variation of Parameters

This method is general and can be applied to any f(x)f(x). First, we find the complementary function yc=C1y1(x)+C2y2(x)y_c = C_1 y_1(x) + C_2 y_2(x). Then, the particular integral is given by:

📐 Variation of Parameters for Cauchy-Euler

For y+P(x)y+Q(x)y=F(x)y'' + P(x)y' + Q(x)y = F(x), where P(x)=b/x,Q(x)=c/x2P(x) = b/x, Q(x) = c/x^2 and F(x)=f(x)/x2F(x) = f(x)/x^2:

yp(x)=y1(x)y2(x)F(x)W(y1,y2)dx+y2(x)y1(x)F(x)W(y1,y2)dxy_p(x) = -y_1(x) \int \frac{y_2(x) F(x)}{W(y_1, y_2)} dx + y_2(x) \int \frac{y_1(x) F(x)}{W(y_1, y_2)} dx

Where:
y1(x),y2(x)y_1(x), y_2(x) are two linearly independent solutions of the homogeneous equation.
W(y1,y2)=y1y2y1y2=y1y2y2y1W(y_1, y_2) = \begin{vmatrix} y_1 & y_2 \\ y_1' & y_2' \end{vmatrix} = y_1 y_2' - y_2 y_1'

is the Wronskian.
When to use: For any f(x)f(x), especially when f(x)f(x) is not a simple power of xx or when kk is a root and the Undetermined Coefficients method becomes complicated.

Quick Example:
Find the particular integral of

x2y+xyy=xx^2 y'' + xy' - y = x

Step 1: Normalize the equation to y+P(x)y+Q(x)y=F(x)y'' + P(x)y' + Q(x)y = F(x).

y+1xy1x2y=1xy'' + \frac{1}{x} y' - \frac{1}{x^2} y = \frac{1}{x}

So F(x)=1xF(x) = \frac{1}{x}.

Step 2: Find y1(x)y_1(x) and y2(x)y_2(x) from the homogeneous equation x2y+xyy=0x^2 y'' + xy' - y = 0.
Characteristic equation: m2+(11)m1=0    m21=0    m=±1m^2 + (1-1)m - 1 = 0 \implies m^2 - 1 = 0 \implies m = \pm 1.

y1(x)=x1=xy2(x)=x1=1x\begin{aligned}y_1(x) & = x^1 = x \\
y_2(x) & = x^{-1} = \frac{1}{x}\end{aligned}

Step 3: Calculate the Wronskian W(y1,y2)W(y_1, y_2).

y1=1y2=x2W(y1,y2)=y1y2y2y1=x(x2)(1x)(1)=1x1x=2x\begin{aligned}y_1' & = 1 \\
y_2' & = -x^{-2} \\
W(y_1, y_2) & = y_1 y_2' - y_2 y_1' = x(-x^{-2}) - \left(\frac{1}{x}\right)(1) = -\frac{1}{x} - \frac{1}{x} = -\frac{2}{x}\end{aligned}

Step 4: Apply the Variation of Parameters formula.

yp(x)=x1x1x2xdx+1xx1x2xdxyp(x)=x1x22xdx+1x12xdxyp(x)=x(12x)dx+1x(x2)dxyp(x)=x121xdx12xxdxyp(x)=x12lnx12xx22yp(x)=12xlnx14x\begin{aligned}y_p(x) & = -x \int \frac{\frac{1}{x} \cdot \frac{1}{x}}{-\frac{2}{x}} dx + \frac{1}{x} \int \frac{x \cdot \frac{1}{x}}{-\frac{2}{x}} dx \\
y_p(x) & = -x \int \frac{\frac{1}{x^2}}{-\frac{2}{x}} dx + \frac{1}{x} \int \frac{1}{-\frac{2}{x}} dx \\
y_p(x) & = -x \int \left(-\frac{1}{2x}\right) dx + \frac{1}{x} \int \left(-\frac{x}{2}\right) dx \\
y_p(x) & = x \cdot \frac{1}{2} \int \frac{1}{x} dx - \frac{1}{2x} \int x dx \\
y_p(x) & = x \cdot \frac{1}{2} \ln x - \frac{1}{2x} \cdot \frac{x^2}{2} \\
y_p(x) & = \frac{1}{2} x \ln x - \frac{1}{4} x\end{aligned}

Answer:

yp(x)=12xlnx14xy_p(x) = \frac{1}{2} x \ln x - \frac{1}{4} x

:::question type="NAT" question="Using Variation of Parameters, find the particular integral of x2d2ydx22xdydx+2y=x3lnxx^2 \frac{d^2 y}{dx^2} - 2x \frac{dy}{dx} + 2y = x^3 \ln x. If yp=Ax3lnx+Bx3y_p = Ax^3 \ln x + Bx^3, what is the value of AA?" answer="0.5" hint="First find y1,y2y_1, y_2. Then calculate the Wronskian. The normalized F(x)F(x) will be xlnxx \ln x." solution="Step 1: Normalize the equation to y+P(x)y+Q(x)y=F(x)y'' + P(x)y' + Q(x)y = F(x).

y2xy+2x2y=xlnxy'' - \frac{2}{x} y' + \frac{2}{x^2} y = x \ln x

So F(x)=xlnxF(x) = x \ln x.
Step 2: Find y1(x)y_1(x) and y2(x)y_2(x) from x2y2xy+2y=0x^2 y'' - 2xy' + 2y = 0.
Characteristic equation: m2+(21)m+2=0    m23m+2=0    (m1)(m2)=0m^2 + (-2-1)m + 2 = 0 \implies m^2 - 3m + 2 = 0 \implies (m-1)(m-2) = 0.
Roots are m1=1,m2=2m_1 = 1, m_2 = 2.
y1(x)=xy2(x)=x2\begin{aligned}y_1(x) & = x \\
y_2(x) & = x^2\end{aligned}

Step 3: Calculate the Wronskian W(y1,y2)W(y_1, y_2).
y1=1y2=2xW(y1,y2)=x(2x)x2(1)=2x2x2=x2\begin{aligned}y_1' & = 1 \\
y_2' & = 2x \\
W(y_1, y_2) & = x(2x) - x^2(1) = 2x^2 - x^2 = x^2\end{aligned}

Step 4: Apply the Variation of Parameters formula.
yp(x)=y1(x)y2(x)F(x)W(y1,y2)dx+y2(x)y1(x)F(x)W(y1,y2)dxyp(x)=xx2(xlnx)x2dx+x2x(xlnx)x2dxyp(x)=xxlnxdx+x2lnxdx\begin{aligned}y_p(x) & = -y_1(x) \int \frac{y_2(x) F(x)}{W(y_1, y_2)} dx + y_2(x) \int \frac{y_1(x) F(x)}{W(y_1, y_2)} dx \\
y_p(x) & = -x \int \frac{x^2 (x \ln x)}{x^2} dx + x^2 \int \frac{x (x \ln x)}{x^2} dx \\
y_p(x) & = -x \int x \ln x dx + x^2 \int \ln x dx\end{aligned}

Step 5: Evaluate the integrals.
For xlnxdx\int x \ln x dx: Use integration by parts udv=uvvdu\int u dv = uv - \int v du. Let u=lnx,dv=xdxu = \ln x, dv = x dx. Then du=1xdx,v=x22du = \frac{1}{x} dx, v = \frac{x^2}{2}.
xlnxdx=x22lnxx221xdx=x22lnxx2dx=x22lnxx24\int x \ln x dx = \frac{x^2}{2} \ln x - \int \frac{x^2}{2} \frac{1}{x} dx = \frac{x^2}{2} \ln x - \int \frac{x}{2} dx = \frac{x^2}{2} \ln x - \frac{x^2}{4}

For lnxdx\int \ln x dx: Use integration by parts. Let u=lnx,dv=dxu = \ln x, dv = dx. Then du=1xdx,v=xdu = \frac{1}{x} dx, v = x.
lnxdx=xlnxx1xdx=xlnxx\int \ln x dx = x \ln x - \int x \frac{1}{x} dx = x \ln x - x

Step 6: Substitute back into yp(x)y_p(x).
yp(x)=x(x22lnxx24)+x2(xlnxx)yp(x)=x32lnx+x34+x3lnxx3yp(x)=(112)x3lnx+(141)x3yp(x)=12x3lnx34x3\begin{aligned}y_p(x) & = -x \left( \frac{x^2}{2} \ln x - \frac{x^2}{4} \right) + x^2 (x \ln x - x) \\
y_p(x) & = -\frac{x^3}{2} \ln x + \frac{x^3}{4} + x^3 \ln x - x^3 \\
y_p(x) & = \left( 1 - \frac{1}{2} \right) x^3 \ln x + \left( \frac{1}{4} - 1 \right) x^3 \\
y_p(x) & = \frac{1}{2} x^3 \ln x - \frac{3}{4} x^3\end{aligned}

Comparing with yp=Ax3lnx+Bx3y_p = Ax^3 \ln x + Bx^3, we have A=12=0.5A = \frac{1}{2} = 0.5.
"
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Problem-Solving Strategies

💡 CUET PG Strategy: Cauchy-Euler

When solving non-homogeneous Cauchy-Euler equations for f(x)=xkf(x)=x^k, always check the characteristic roots first. If kk is a root, use the modified particular integral form BxklnxBx^k \ln x (or Bxk(lnx)2Bx^k (\ln x)^2 for double roots) to save significant time compared to Variation of Parameters. Variation of Parameters is more general but computationally intensive.

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Common Mistakes

⚠️ Watch Out: Characteristic Equation

❌ Using

am2+bm+c=0am^2 + bm + c = 0

directly for Cauchy-Euler equations. This is for constant coefficient equations.
✅ Use the correct characteristic equation:
am2+(ba)m+c=0am^2 + (b-a)m + c = 0

This accounts for the transformation of derivatives.

⚠️ Common Mistake: Repeated Roots

❌ For repeated roots mm, writing the solution as C1xm+C2xmC_1 x^m + C_2 x^m. This is incorrect as it does not provide two linearly independent solutions.
✅ The correct form for repeated roots mm is C1xm+C2xmlnxC_1 x^m + C_2 x^m \ln x. The lnx\ln x factor ensures linear independence.

⚠️ Particular Integral for xkx^k

❌ Always assuming yp=Axky_p = Ax^k for f(x)=xkf(x)=x^k, even if kk is a root of the characteristic equation. This will lead to 0=xk0=x^k and prevent finding AA.
✅ Check if kk is a root. If so, modify the assumed form to AxklnxAx^k \ln x (or higher powers of lnx\ln x if kk is a higher multiplicity root).

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Practice Questions

:::question type="MCQ" question="The general solution of

x2d2ydx24xdydx+6y=0x^2 \frac{d^2 y}{dx^2} - 4x \frac{dy}{dx} + 6y = 0
is:" options=["C1x2+C2x3C_1 x^2 + C_2 x^3","C1x2lnx+C2x3C_1 x^2 \ln x + C_2 x^3","C1x2+C2x3C_1 x^{-2} + C_2 x^{-3}","C1e2x+C2e3xC_1 e^{2x} + C_2 e^{3x}"] answer="C1x2+C2x3C_1 x^2 + C_2 x^3" hint="Identify a,b,ca, b, c and form the characteristic equation." solution="Step 1: Identify coefficients a=1,b=4,c=6a=1, b=-4, c=6.
Step 2: Form the characteristic equation:
m2+(41)m+6=0m25m+6=0\begin{aligned} m^2 + (-4-1)m + 6 & = 0 \\ m^2 - 5m + 6 & = 0 \end{aligned}

Step 3: Find the roots:
(m2)(m3)=0m1=2,m2=3\begin{aligned} (m-2)(m-3) & = 0 \\ m_1 = 2, m_2 & = 3 \end{aligned}

Step 4: Write the general solution for distinct real roots:
yc(x)=C1x2+C2x3y_c(x) = C_1 x^2 + C_2 x^3

Answer: C1x2+C2x3\boxed{C_1 x^2 + C_2 x^3}"
:::

:::question type="NAT" question="If

x2y+7xy+9y=0x^2 y'' + 7xy' + 9y = 0
, and y(1)=1,y(1)=0y(1)=1, y'(1)=0, then y(e)y(e) is Ae3A e^{-3}. What is the value of AA?" answer="4.0" hint="First find the general solution, then apply initial conditions to find C1,C2C_1, C_2." solution="Step 1: Form the characteristic equation.
Here a=1,b=7,c=9a=1, b=7, c=9.
m2+(71)m+9=0m2+6m+9=0\begin{aligned} m^2 + (7-1)m + 9 & = 0 \\ m^2 + 6m + 9 & = 0 \end{aligned}

Step 2: Find the roots:
(m+3)2=0m1=3,m2=3(repeated roots)\begin{aligned} (m+3)^2 & = 0 \\ m_1 = -3, m_2 & = -3 \quad \text{(repeated roots)} \end{aligned}

Step 3: Write the general solution:
y(x)=C1x3+C2x3lnxy(x) = C_1 x^{-3} + C_2 x^{-3} \ln x

Step 4: Find y(x)y'(x):
y(x)=3C1x4+C2(3x4lnx+x31x)y(x)=3C1x4+C2(3x4lnx+x4)\begin{aligned} y'(x) & = -3C_1 x^{-4} + C_2 \left(-3x^{-4} \ln x + x^{-3} \cdot \frac{1}{x}\right) \\ y'(x) & = -3C_1 x^{-4} + C_2 \left(-3x^{-4} \ln x + x^{-4}\right) \end{aligned}

Step 5: Apply initial conditions y(1)=1,y(1)=0y(1)=1, y'(1)=0.
For y(1)=1y(1)=1:
C1(1)3+C2(1)3ln(1)=1C1+C2(0)=1C1=1\begin{aligned} C_1 (1)^{-3} + C_2 (1)^{-3} \ln(1) & = 1 \\ C_1 + C_2 (0) & = 1 \\ C_1 & = 1 \end{aligned}

For y(1)=0y'(1)=0:
3C1(1)4+C2(3(1)4ln(1)+(1)4)=03C1+C2(0+1)=03C1+C2=0\begin{aligned} -3C_1 (1)^{-4} + C_2 \left(-3(1)^{-4} \ln(1) + (1)^{-4}\right) & = 0 \\ -3C_1 + C_2 (0 + 1) & = 0 \\ -3C_1 + C_2 & = 0 \end{aligned}

Substituting C1=1C_1=1:
3(1)+C2=0C2=3\begin{aligned} -3(1) + C_2 & = 0 \\ C_2 & = 3 \end{aligned}

Step 6: Write the particular solution:
y(x)=1x3+3x3lnx=x3(1+3lnx)y(x) = 1 \cdot x^{-3} + 3 \cdot x^{-3} \ln x = x^{-3} (1 + 3 \ln x)

Step 7: Evaluate y(e)y(e).
y(e)=e3(1+3lne)=e3(1+31)=e3(4)\begin{aligned} y(e) & = e^{-3} (1 + 3 \ln e) \\ & = e^{-3} (1 + 3 \cdot 1) \\ & = e^{-3} (4) \end{aligned}

y(e)=4e3y(e) = 4e^{-3}

Comparing with Ae3A e^{-3}, we get A=4A=4.
Answer: 4\boxed{4}"
:::

:::question type="MCQ" question="The particular integral of

x2y+4xy+2y=1xx^2 y'' + 4xy' + 2y = \frac{1}{x}
is:" options=["1xlnx\frac{1}{x} \ln x","1x\frac{1}{x}","1x2\frac{1}{x^2}","lnxx2\frac{\ln x}{x^2}"] answer="1xlnx\frac{1}{x} \ln x" hint="Find roots of the homogeneous equation. Then use the method for f(x)=xkf(x)=x^k." solution="Step 1: Find the roots of the characteristic equation for
x2y+4xy+2y=0x^2 y'' + 4xy' + 2y = 0
.
Here a=1,b=4,c=2a=1, b=4, c=2.
m2+(41)m+2=0m2+3m+2=0(m+1)(m+2)=0\begin{aligned} m^2 + (4-1)m + 2 & = 0 \\ m^2 + 3m + 2 & = 0 \\ (m+1)(m+2) & = 0 \end{aligned}

Roots are m1=1,m2=2m_1 = -1, m_2 = -2.
Step 2: The RHS is f(x)=1x=x1f(x) = \frac{1}{x} = x^{-1}. The power k=1k=-1 is a root of the characteristic equation.
Step 3: Assume yp=Bx1lnxy_p = Bx^{-1} \ln x.
Step 4: Calculate derivatives:
yp=B(x2lnx+x11x)=B(x2lnx+x2)\begin{aligned} y_p' & = B\left(-x^{-2} \ln x + x^{-1} \cdot \frac{1}{x}\right) \\ & = B\left(-x^{-2} \ln x + x^{-2}\right) \end{aligned}

yp=B(2x3lnxx21x2x3)=B(2x3lnxx32x3)=B(2x3lnx3x3)\begin{aligned} y_p'' & = B\left(2x^{-3} \ln x - x^{-2} \cdot \frac{1}{x} - 2x^{-3}\right) \\ & = B\left(2x^{-3} \ln x - x^{-3} - 2x^{-3}\right) \\ & = B\left(2x^{-3} \ln x - 3x^{-3}\right) \end{aligned}

Step 5: Substitute into
x2y+4xy+2y=x1x^2 y'' + 4xy' + 2y = x^{-1}
:
x2[B(2x3lnx3x3)]+4x[B(x2lnx+x2)]+2[Bx1lnx]=x1B[2x1lnx3x14x1lnx+4x1+2x1lnx]=x1B[(24+2)x1lnx+(3+4)x1]=x1B[0x1lnx+1x1]=x1Bx1=x1\begin{aligned} & x^2 \left[B\left(2x^{-3} \ln x - 3x^{-3}\right)\right] + 4x \left[B\left(-x^{-2} \ln x + x^{-2}\right)\right] + 2 \left[Bx^{-1} \ln x\right] = x^{-1} \\ & B\left[2x^{-1} \ln x - 3x^{-1} - 4x^{-1} \ln x + 4x^{-1} + 2x^{-1} \ln x\right] = x^{-1} \\ & B\left[(2-4+2)x^{-1} \ln x + (-3+4)x^{-1}\right] = x^{-1} \\ & B\left[0 \cdot x^{-1} \ln x + 1 \cdot x^{-1}\right] = x^{-1} \\ & Bx^{-1} = x^{-1} \end{aligned}

Step 6: Solve for BB:
B=1B=1

Step 7: The particular integral is
yp=1x1lnx=1xlnxy_p = 1 \cdot x^{-1} \ln x = \frac{1}{x} \ln x
.
Answer: 1xlnx\boxed{\frac{1}{x} \ln x}"
:::

:::question type="MSQ" question="Which of the following statements are TRUE regarding the Cauchy-Euler equation

x2y+y=0x^2 y'' + y = 0
?" options=["The characteristic equation is m2m+1=0m^2 - m + 1 = 0.","The roots of the characteristic equation are complex.","The general solution involves lnx\ln x terms.","The general solution is x1/2(C1cos(32lnx)+C2sin(32lnx))x^{1/2}(C_1 \cos(\frac{\sqrt{3}}{2} \ln x) + C_2 \sin(\frac{\sqrt{3}}{2} \ln x)). "] answer="The characteristic equation is m2m+1=0.m^2 - m + 1 = 0.,The roots of the characteristic equation are complex.,The general solution is x1/2(C1cos(32lnx)+C2sin(32lnx))x^{1/2}(C_1 \cos(\frac{\sqrt{3}}{2} \ln x) + C_2 \sin(\frac{\sqrt{3}}{2} \ln x)). " hint="Carefully form the characteristic equation and analyze its roots. Remember the structure of solutions for complex roots." solution="Step 1: Identify coefficients a=1,b=0,c=1a=1, b=0, c=1.
Step 2: Form the characteristic equation:
m2+(01)m+1=0m2m+1=0\begin{aligned} m^2 + (0-1)m + 1 & = 0 \\ m^2 - m + 1 & = 0 \end{aligned}

Thus, 'The characteristic equation is m2m+1=0m^2 - m + 1 = 0.' is TRUE.
Step 3: Find the roots of m2m+1=0m^2 - m + 1 = 0 using the quadratic formula:
m=(1)±(1)24(1)(1)2(1)m=1±142m=1±32m=1±i32\begin{aligned} m & = \frac{-(-1) \pm \sqrt{(-1)^2 - 4(1)(1)}}{2(1)} \\ m & = \frac{1 \pm \sqrt{1 - 4}}{2} \\ m & = \frac{1 \pm \sqrt{-3}}{2} \\ m & = \frac{1 \pm i\sqrt{3}}{2} \end{aligned}

Roots are m1=12+i32m_1 = \frac{1}{2} + i\frac{\sqrt{3}}{2} and m2=12i32m_2 = \frac{1}{2} - i\frac{\sqrt{3}}{2}.
Thus, 'The roots of the characteristic equation are complex.' is TRUE.
Step 4: Determine the form of the general solution.
Since the roots are complex (m=α±iβm = \alpha \pm i\beta with α=1/2,β=3/2\alpha=1/2, \beta=\sqrt{3}/2), the general solution is yc(x)=xα(C1cos(βlnx)+C2sin(βlnx))y_c(x) = x^{\alpha} (C_1 \cos(\beta \ln x) + C_2 \sin(\beta \ln x)).
yc(x)=x1/2(C1cos(32lnx)+C2sin(32lnx))y_c(x) = x^{1/2} \left(C_1 \cos\left(\frac{\sqrt{3}}{2} \ln x\right) + C_2 \sin\left(\frac{\sqrt{3}}{2} \ln x\right)\right)

Thus, 'The general solution involves lnx\ln x terms.' is TRUE because of cos(βlnx)\cos(\beta \ln x) and sin(βlnx)\sin(\beta \ln x).
And 'The general solution is x1/2(C1cos(32lnx)+C2sin(32lnx))x^{1/2}(C_1 \cos(\frac{\sqrt{3}}{2} \ln x) + C_2 \sin(\frac{\sqrt{3}}{2} \ln x)).' is TRUE.
Answer: The characteristic equation is m2m+1=0.,The roots of the characteristic equation are complex.,The general solution is x1/2(C1cos(32lnx)+C2sin(32lnx)).\boxed{\text{The characteristic equation is } m^2 - m + 1 = 0., \text{The roots of the characteristic equation are complex.}, \text{The general solution is } x^{1/2}(C_1 \cos(\frac{\sqrt{3}}{2} \ln x) + C_2 \sin(\frac{\sqrt{3}}{2} \ln x)).}"
:::

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Summary

Key Formulas & Takeaways

| # | Formula/Concept | Expression |
|---|----------------|------------|
| 1 | Standard Form | ax2y+bxy+cy=f(x)ax^2 y'' + bxy' + cy = f(x) |
| 2 | Characteristic Eq. | am2+(ba)m+c=0am^2 + (b-a)m + c = 0 |
| 3 | Real, Distinct Roots (m1,m2m_1, m_2) | yc=C1xm1+C2xm2y_c = C_1 x^{m_1} + C_2 x^{m_2} |
| 4 | Real, Equal Roots (mm) | yc=C1xm+C2xmlnxy_c = C_1 x^m + C_2 x^m \ln x |
| 5 | Complex Roots (α±iβ\alpha \pm i\beta) | yc=xα(C1cos(βlnx)+C2sin(βlnx))y_c = x^{\alpha} (C_1 \cos(\beta \ln x) + C_2 \sin(\beta \ln x)) |
| 6 | P.I. for f(x)=Axkf(x)=Ax^k (kk not a root) | yp=Bxky_p = Bx^k |
| 7 | P.I. for f(x)=Axkf(x)=Ax^k (kk is a single root) | yp=Bxklnxy_p = Bx^k \ln x |
| 8 | P.I. (Variation of Parameters) | yp=y1y2FWdx+y2y1FWdxy_p = -y_1 \int \frac{y_2 F}{W} dx + y_2 \int \frac{y_1 F}{W} dx |

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What's Next?

💡 Continue Learning

This topic connects to:

    • Linear Differential Equations with Constant Coefficients: The substitution x=etx=e^t transforms Cauchy-Euler equations into these. Understanding their solution methods is crucial.

    • Higher-Order Linear Differential Equations: Cauchy-Euler equations can be extended to orders greater than two, following similar characteristic equation principles.

    • Laplace Transforms: While not directly used for solving Cauchy-Euler equations, Laplace transforms are another powerful tool for solving linear differential equations, especially with initial conditions.

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💡 Next Up

Proceeding to Method of Variation of Parameters.

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Part 3: Method of Variation of Parameters

We consider the Method of Variation of Parameters as a powerful technique for determining a particular solution to non-homogeneous linear ordinary differential equations, particularly when the method of undetermined coefficients is not applicable due to the form of the non-homogeneous term. This method is fundamental for solving a broad class of differential equations encountered in advanced mathematics.

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Core Concepts

1. Homogeneous Linear Second-Order Differential Equations

A second-order linear homogeneous differential equation is expressed in the form y+P(x)y+Q(x)y=0y'' + P(x)y' + Q(x)y = 0, where P(x)P(x) and Q(x)Q(x) are continuous functions on some interval. The general solution, denoted ycy_c, is a linear combination of two linearly independent solutions, y1(x)y_1(x) and y2(x)y_2(x).

The concept of linear independence is critical for constructing the general solution. Two functions y1(x)y_1(x) and y2(x)y_2(x) are linearly independent on an interval if neither is a constant multiple of the other.

📖 Wronskian

For two differentiable functions y1(x)y_1(x) and y2(x)y_2(x), their Wronskian, denoted W(y1,y2)(x)W(y_1, y_2)(x) or simply W(x)W(x), is defined by the determinant:

W(x)=det[y1(x)y2(x)y1(x)y2(x)]=y1(x)y2(x)y2(x)y1(x)W(x) = \det \begin{bmatrix} y_1(x) & y_2(x) \\ y_1'(x) & y_2'(x) \end{bmatrix} = y_1(x)y_2'(x) - y_2(x)y_1'(x)

The functions y1(x)y_1(x) and y2(x)y_2(x) are linearly independent on an interval if and only if W(x)0W(x) \neq 0 for at least one point in that interval.

1.1. Abel's Formula for the Wronskian

For a homogeneous second-order linear differential equation y+P(x)y+Q(x)y=0y'' + P(x)y' + Q(x)y = 0, if y1(x)y_1(x) and y2(x)y_2(x) are two solutions, their Wronskian W(x)W(x) satisfies Abel's Formula. This formula allows for the calculation of the Wronskian without explicit knowledge of y1(x)y_1(x) and y2(x)y_2(x), provided the equation is in standard form.

📐 Abel's Formula
W(x)=CeP(x)dxW(x) = C e^{-\int P(x) dx}
Where: CC = an arbitrary constant, determined by initial conditions or a known value of W(x)W(x) at a specific point. P(x)P(x) = the coefficient of yy' when the differential equation is in the standard form y+P(x)y+Q(x)y=0y'' + P(x)y' + Q(x)y = 0. When to use: To find the Wronskian of any two solutions to a homogeneous linear second-order ODE without explicitly knowing the solutions.

Quick Example: Determine the Wronskian for the differential equation 2y+y+t2y=02y'' + y' + t^2y = 0.

Step 1: Bring the equation to standard form y+P(t)y+Q(t)y=0y'' + P(t)y' + Q(t)y = 0.
Divide by 2:

y+12y+t22y=0y'' + \frac{1}{2}y' + \frac{t^2}{2}y = 0

Step 2: Identify P(t)P(t) and apply Abel's Formula.
Here, P(t)=12P(t) = \frac{1}{2}.

W(t)=Ce12dtW(t) = C e^{-\int \frac{1}{2} dt}

Step 3: Evaluate the integral.

W(t)=Ce12tW(t) = C e^{-\frac{1}{2}t}

Answer: The Wronskian is Cet/2C e^{-t/2}.

:::question type="MCQ" question="Let W(x)W(x) be the Wronskian of two linearly independent solutions of the differential equation x2yxy+(cosx)y=0x^2y'' - xy' + (\cos x)y = 0 for x>0x>0. Then W(x)W(x) is proportional to:" options=["xx","x1x^{-1}","exe^x","exe^{-x}"] answer="xx" hint="First, convert the given differential equation into the standard form y+P(x)y+Q(x)y=0y'' + P(x)y' + Q(x)y = 0 before applying Abel's Formula." solution="Step 1: Convert the equation to standard form.
Divide the given equation x2yxy+(cosx)y=0x^2y'' - xy' + (\cos x)y = 0 by x2x^2 (since x>0x>0):

y1xy+cosxx2y=0y'' - \frac{1}{x}y' + \frac{\cos x}{x^2}y = 0

Step 2: Identify P(x)P(x).
Comparing with y+P(x)y+Q(x)y=0y'' + P(x)y' + Q(x)y = 0, we have P(x)=1xP(x) = -\frac{1}{x}.
Step 3: Apply Abel's Formula.
W(x)=CeP(x)dxW(x) = C e^{-\int P(x) dx}

W(x)=Ce(1x)dxW(x) = C e^{-\int (-\frac{1}{x}) dx}

W(x)=Ce1xdxW(x) = C e^{\int \frac{1}{x} dx}

W(x)=CelnxW(x) = C e^{\ln|x|}

Since x>0x>0, x=x|x|=x.
W(x)=CelnxW(x) = C e^{\ln x}

W(x)=CxW(x) = C x

Thus, W(x)W(x) is proportional to xx.

The final answer is x\boxed{x}"
:::

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2. Method of Variation of Parameters for Second-Order ODEs

The Method of Variation of Parameters provides a systematic way to find a particular solution yp(x)y_p(x) for a non-homogeneous linear second-order differential equation of the form y+P(x)y+Q(x)y=f(x)y'' + P(x)y' + Q(x)y = f(x). This method is particularly useful when f(x)f(x) is not one of the forms for which the Method of Undetermined Coefficients is applicable (e.g., f(x)=tanxf(x) = \tan x, secx\sec x, or eaxxn\frac{e^{ax}}{x^n}).

The general solution to the non-homogeneous equation is y(x)=yc(x)+yp(x)y(x) = y_c(x) + y_p(x), where yc(x)=c1y1(x)+c2y2(x)y_c(x) = c_1y_1(x) + c_2y_2(x) is the complementary solution obtained from the homogeneous equation y+P(x)y+Q(x)y=0y'' + P(x)y' + Q(x)y = 0.

📐 Particular Solution (ypy_p) by Variation of Parameters

Given y+P(x)y+Q(x)y=f(x)y'' + P(x)y' + Q(x)y = f(x) and yc=c1y1(x)+c2y2(x)y_c = c_1y_1(x) + c_2y_2(x), the particular solution yp(x)y_p(x) is given by:

yp(x)=u1(x)y1(x)+u2(x)y2(x)y_p(x) = u_1(x)y_1(x) + u_2(x)y_2(x)

Where:
u1(x)=y2(x)f(x)W(x)u_1'(x) = -\frac{y_2(x)f(x)}{W(x)}

u2(x)=y1(x)f(x)W(x)u_2'(x) = \frac{y_1(x)f(x)}{W(x)}

And W(x)=y1(x)y2(x)y2(x)y1(x)W(x) = y_1(x)y_2'(x) - y_2(x)y_1'(x) is the Wronskian of y1y_1 and y2y_2.
u1(x)=u1(x)dxu_1(x) = \int u_1'(x) dx and u2(x)=u2(x)dxu_2(x) = \int u_2'(x) dx.
When to use: For non-homogeneous linear ODEs where f(x)f(x) is arbitrary, or when the Method of Undetermined Coefficients is unsuitable. Requires two linearly independent solutions y1,y2y_1, y_2 of the homogeneous counterpart.

Quick Example: Find a particular solution for y+y=secxy'' + y = \sec x.

Step 1: Find the complementary solution ycy_c.
The homogeneous equation is y+y=0y'' + y = 0.
The characteristic equation is r2+1=0r^2 + 1 = 0, so r=±ir = \pm i.
Thus, yc=c1cosx+c2sinxy_c = c_1 \cos x + c_2 \sin x.
We identify y1(x)=cosxy_1(x) = \cos x and y2(x)=sinxy_2(x) = \sin x.

Step 2: Calculate the Wronskian W(x)W(x).

W(x)=y1y2y2y1W(x) = y_1 y_2' - y_2 y_1'

W(x)=(cosx)(cosx)(sinx)(sinx)W(x) = (\cos x)(\cos x) - (\sin x)(-\sin x)

W(x)=cos2x+sin2x=1W(x) = \cos^2 x + \sin^2 x = 1

Step 3: Identify f(x)f(x) and calculate u1(x)u_1'(x) and u2(x)u_2'(x).
The equation is already in standard form, so f(x)=secxf(x) = \sec x.

u1(x)=y2(x)f(x)W(x)=(sinx)(secx)1=sinxcosx=tanxu_1'(x) = -\frac{y_2(x)f(x)}{W(x)} = -\frac{(\sin x)(\sec x)}{1} = -\frac{\sin x}{\cos x} = -\tan x

u2(x)=y1(x)f(x)W(x)=(cosx)(secx)1=cosxcosx=1u_2'(x) = \frac{y_1(x)f(x)}{W(x)} = \frac{(\cos x)(\sec x)}{1} = \frac{\cos x}{\cos x} = 1

Step 4: Integrate to find u1(x)u_1(x) and u2(x)u_2(x).

u1(x)=tanxdx=lncosxu_1(x) = \int -\tan x dx = \ln|\cos x|

u2(x)=1dx=xu_2(x) = \int 1 dx = x

(We omit the constants of integration as we seek a particular solution.)

Step 5: Form the particular solution yp(x)y_p(x).

yp(x)=u1(x)y1(x)+u2(x)y2(x)y_p(x) = u_1(x)y_1(x) + u_2(x)y_2(x)

yp(x)=(lncosx)(cosx)+(x)(sinx)y_p(x) = (\ln|\cos x|)(\cos x) + (x)(\sin x)

yp(x)=cosxlncosx+xsinxy_p(x) = \cos x \ln|\cos x| + x \sin x

Answer: yp(x)=cosxlncosx+xsinxy_p(x) = \cos x \ln|\cos x| + x \sin x.

:::question type="MCQ" question="For the differential equation d2ydx26dydx+9y=e3xx2\frac{d^2y}{dx^2} - 6\frac{dy}{dx} + 9y = \frac{e^{3x}}{x^2}, which of the following statements are correct?
I. The Wronskian of the homogeneous solutions is e6xe^{6x}.
II. e3xe^{3x} and xe3xxe^{3x} are two linearly independent solutions of the homogeneous equation.
III. A particular integral (PI) is e3x(lnx+1)e^{3x}(\ln x + 1).
IV. A particular integral (PI) is e3x(lnx+1)-e^{3x}(\ln x + 1)." options=["I and III only","II and III only","I and IV only","II and IV only"] answer="II and IV only" hint="First find the complementary solutions and their Wronskian. Then apply the Method of Variation of Parameters to find the particular integral. Pay close attention to the sign in the final PI." solution="Step 1: Find the complementary solution ycy_c.
The homogeneous equation is y6y+9y=0y'' - 6y' + 9y = 0.
The characteristic equation is r26r+9=0r^2 - 6r + 9 = 0, which is (r3)2=0(r-3)^2 = 0.
So, r=3r = 3 (repeated root).
The linearly independent solutions are y1(x)=e3xy_1(x) = e^{3x} and y2(x)=xe3xy_2(x) = xe^{3x}.
Thus, statement II is correct.

Step 2: Calculate the Wronskian W(x)W(x).

W(x)=y1y2y2y1W(x) = y_1 y_2' - y_2 y_1'

y1(x)=3e3xy_1'(x) = 3e^{3x}

y2(x)=e3x+3xe3x=e3x(1+3x)y_2'(x) = e^{3x} + 3xe^{3x} = e^{3x}(1+3x)

W(x)=e3xe3x(1+3x)xe3x3e3xW(x) = e^{3x} \cdot e^{3x}(1+3x) - xe^{3x} \cdot 3e^{3x}

W(x)=e6x(1+3x)3xe6xW(x) = e^{6x}(1+3x) - 3xe^{6x}

W(x)=e6x+3xe6x3xe6xW(x) = e^{6x} + 3xe^{6x} - 3xe^{6x}

W(x)=e6xW(x) = e^{6x}

The Wronskian is W(x)=CeP(x)dx=Ce(6)dx=Ce6xW(x) = C e^{-\int P(x) dx} = C e^{-\int (-6) dx} = C e^{6x}. While e6xe^{6x} is a possible form for the Wronskian (when C=1C=1), statement I claims "The Wronskian... is e6xe^{6x}", which is a specific value. Without further information to fix C=1C=1, this statement is not universally true for any pair of linearly independent solutions. For example, if y1=2e3xy_1 = 2e^{3x} and y2=xe3xy_2 = xe^{3x}, then W(x)=2e6xW(x) = 2e^{6x}. Therefore, statement I is not necessarily correct in all contexts.

Step 3: Apply the Method of Variation of Parameters to find ypy_p.
The non-homogeneous term is f(x)=e3xx2f(x) = \frac{e^{3x}}{x^2}.

u1(x)=y2(x)f(x)W(x)=xe3xe3xx2e6x=xe6xx2e6x=1xu_1'(x) = -\frac{y_2(x)f(x)}{W(x)} = -\frac{xe^{3x} \cdot \frac{e^{3x}}{x^2}}{e^{6x}} = -\frac{x e^{6x}}{x^2 e^{6x}} = -\frac{1}{x}

u2(x)=y1(x)f(x)W(x)=e3xe3xx2e6x=e6xx2e6x=1x2u_2'(x) = \frac{y_1(x)f(x)}{W(x)} = \frac{e^{3x} \cdot \frac{e^{3x}}{x^2}}{e^{6x}} = \frac{e^{6x}}{x^2 e^{6x}} = \frac{1}{x^2}

Step 4: Integrate u1(x)u_1'(x) and u2(x)u_2'(x).

u1(x)=1xdx=lnxu_1(x) = \int -\frac{1}{x} dx = -\ln|x|

u2(x)=1x2dx=1xu_2(x) = \int \frac{1}{x^2} dx = -\frac{1}{x}

Step 5: Form the particular solution yp(x)y_p(x).

yp(x)=u1(x)y1(x)+u2(x)y2(x)y_p(x) = u_1(x)y_1(x) + u_2(x)y_2(x)

yp(x)=(lnx)e3x+(1x)xe3xy_p(x) = (-\ln|x|)e^{3x} + \left(-\frac{1}{x}\right)xe^{3x}

yp(x)=e3xlnxe3xy_p(x) = -e^{3x}\ln|x| - e^{3x}

yp(x)=e3x(lnx+1)y_p(x) = -e^{3x}(\ln|x| + 1)

Assuming x>0x>0, we write yp(x)=e3x(lnx+1)y_p(x) = -e^{3x}(\ln x + 1).
Thus, statement IV is correct, and statement III is incorrect.

The correct statements are II and IV.

The final answer is II and IV only\boxed{\text{II and IV only}}"
:::

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3. Extension to Higher-Order Differential Equations

The Method of Variation of Parameters can be extended to find a particular solution for an nn-th order non-homogeneous linear differential equation:

y(n)+Pn1(x)y(n1)++P1(x)y+P0(x)y=f(x)y^{(n)} + P_{n-1}(x)y^{(n-1)} + \dots + P_1(x)y' + P_0(x)y = f(x)

If y1,y2,,yny_1, y_2, \dots, y_n are nn linearly independent solutions to the corresponding homogeneous equation, then the particular solution yp(x)y_p(x) is given by:
yp(x)=u1(x)y1(x)+u2(x)y2(x)++un(x)yn(x)y_p(x) = u_1(x)y_1(x) + u_2(x)y_2(x) + \dots + u_n(x)y_n(x)

The derivatives uk(x)u_k'(x) are determined by Cramer's rule, where the numerator involves replacing the kk-th column of the Wronskian determinant with a column vector containing zeros everywhere except f(x)f(x) in the last row, and the denominator is the Wronskian W(y1,,yn)W(y_1, \dots, y_n). While the principle is the same, the calculations become significantly more involved. For CUET PG, the focus typically remains on second-order equations.

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Advanced Applications

The application of Variation of Parameters often requires careful integration, which can be the most challenging aspect. We observe that the choice of f(x)f(x) can significantly impact the complexity of the integrals for u1(x)u_1(x) and u2(x)u_2(x).

Worked Example: Find the general solution to y+4y=tan(2x)y'' + 4y = \tan(2x).

Step 1: Find the complementary solution ycy_c.
The homogeneous equation is y+4y=0y'' + 4y = 0.
The characteristic equation is r2+4=0r^2 + 4 = 0, so r=±2ir = \pm 2i.
Thus, yc=c1cos(2x)+c2sin(2x)y_c = c_1 \cos(2x) + c_2 \sin(2x).
We identify y1(x)=cos(2x)y_1(x) = \cos(2x) and y2(x)=sin(2x)y_2(x) = \sin(2x).

Step 2: Calculate the Wronskian W(x)W(x).

y1(x)=2sin(2x)y_1'(x) = -2\sin(2x)

y2(x)=2cos(2x)y_2'(x) = 2\cos(2x)

W(x)=y1y2y2y1W(x) = y_1 y_2' - y_2 y_1'

W(x)=(cos(2x))(2cos(2x))(sin(2x))(2sin(2x))W(x) = (\cos(2x))(2\cos(2x)) - (\sin(2x))(-2\sin(2x))

W(x)=2cos2(2x)+2sin2(2x)=2(cos2(2x)+sin2(2x))=2W(x) = 2\cos^2(2x) + 2\sin^2(2x) = 2(\cos^2(2x) + \sin^2(2x)) = 2

Step 3: Identify f(x)f(x) and calculate u1(x)u_1'(x) and u2(x)u_2'(x).
The equation is in standard form, f(x)=tan(2x)f(x) = \tan(2x).

u1(x)=y2(x)f(x)W(x)=sin(2x)tan(2x)2=sin2(2x)2cos(2x)u_1'(x) = -\frac{y_2(x)f(x)}{W(x)} = -\frac{\sin(2x)\tan(2x)}{2} = -\frac{\sin^2(2x)}{2\cos(2x)}

u2(x)=y1(x)f(x)W(x)=cos(2x)tan(2x)2=sin(2x)2u_2'(x) = \frac{y_1(x)f(x)}{W(x)} = \frac{\cos(2x)\tan(2x)}{2} = \frac{\sin(2x)}{2}

Step 4: Integrate to find u1(x)u_1(x) and u2(x)u_2(x).
For u2(x)u_2(x):

u2(x)=sin(2x)2dx=12(cos(2x)2)=14cos(2x)u_2(x) = \int \frac{\sin(2x)}{2} dx = \frac{1}{2} \left(-\frac{\cos(2x)}{2}\right) = -\frac{1}{4}\cos(2x)

For u1(x)u_1(x):
u1(x)=sin2(2x)2cos(2x)dx=121cos2(2x)cos(2x)dxu_1(x) = \int -\frac{\sin^2(2x)}{2\cos(2x)} dx = -\frac{1}{2} \int \frac{1-\cos^2(2x)}{\cos(2x)} dx

u1(x)=12(sec(2x)cos(2x))dxu_1(x) = -\frac{1}{2} \int (\sec(2x) - \cos(2x)) dx

u1(x)=12(12lnsec(2x)+tan(2x)12sin(2x))u_1(x) = -\frac{1}{2} \left( \frac{1}{2}\ln|\sec(2x) + \tan(2x)| - \frac{1}{2}\sin(2x) \right)

u1(x)=14lnsec(2x)+tan(2x)+14sin(2x)u_1(x) = -\frac{1}{4}\ln|\sec(2x) + \tan(2x)| + \frac{1}{4}\sin(2x)

Step 5: Form the particular solution yp(x)y_p(x).

yp(x)=u1(x)y1(x)+u2(x)y2(x)y_p(x) = u_1(x)y_1(x) + u_2(x)y_2(x)

yp(x)=(14lnsec(2x)+tan(2x)+14sin(2x))cos(2x)+(14cos(2x))sin(2x)y_p(x) = \left(-\frac{1}{4}\ln|\sec(2x) + \tan(2x)| + \frac{1}{4}\sin(2x)\right)\cos(2x) + \left(-\frac{1}{4}\cos(2x)\right)\sin(2x)

yp(x)=14cos(2x)lnsec(2x)+tan(2x)+14sin(2x)cos(2x)14cos(2x)sin(2x)y_p(x) = -\frac{1}{4}\cos(2x)\ln|\sec(2x) + \tan(2x)| + \frac{1}{4}\sin(2x)\cos(2x) - \frac{1}{4}\cos(2x)\sin(2x)

yp(x)=14cos(2x)lnsec(2x)+tan(2x)y_p(x) = -\frac{1}{4}\cos(2x)\ln|\sec(2x) + \tan(2x)|

Step 6: Form the general solution y(x)=yc(x)+yp(x)y(x) = y_c(x) + y_p(x).

y(x)=c1cos(2x)+c2sin(2x)14cos(2x)lnsec(2x)+tan(2x)y(x) = c_1 \cos(2x) + c_2 \sin(2x) - \frac{1}{4}\cos(2x)\ln|\sec(2x) + \tan(2x)|

Answer: y(x)=c1cos(2x)+c2sin(2x)14cos(2x)lnsec(2x)+tan(2x)y(x) = c_1 \cos(2x) + c_2 \sin(2x) - \frac{1}{4}\cos(2x)\ln|\sec(2x) + \tan(2x)|.

:::question type="NAT" question="A particular solution yp(x)y_p(x) for the differential equation yy=excosxy'' - y = e^x \cos x is of the form u1(x)ex+u2(x)exu_1(x)e^x + u_2(x)e^{-x}. Find the value of u1(x)+u2(x)u_1'(x) + u_2'(x) at x=0x=0." answer="0" hint="First find the homogeneous solutions and their Wronskian. Then apply the formulas for u1(x)u_1'(x) and u2(x)u_2'(x) and sum them. Finally, evaluate the sum at x=0x=0." solution="Step 1: Find the complementary solution ycy_c.
The homogeneous equation is yy=0y'' - y = 0.
The characteristic equation is r21=0r^2 - 1 = 0, so r=±1r = \pm 1.
Thus, y1(x)=exy_1(x) = e^x and y2(x)=exy_2(x) = e^{-x}.

Step 2: Calculate the Wronskian W(x)W(x).

y1(x)=exy_1'(x) = e^x

y2(x)=exy_2'(x) = -e^{-x}

W(x)=y1y2y2y1W(x) = y_1 y_2' - y_2 y_1'

W(x)=(ex)(ex)(ex)(ex)W(x) = (e^x)(-e^{-x}) - (e^{-x})(e^x)

W(x)=11=2W(x) = -1 - 1 = -2

Step 3: Identify f(x)f(x) and calculate u1(x)u_1'(x) and u2(x)u_2'(x).
The non-homogeneous term is f(x)=excosxf(x) = e^x \cos x.

u1(x)=y2(x)f(x)W(x)=ex(excosx)2=e0cosx2=cosx2u_1'(x) = -\frac{y_2(x)f(x)}{W(x)} = -\frac{e^{-x}(e^x \cos x)}{-2} = \frac{e^0 \cos x}{2} = \frac{\cos x}{2}

u2(x)=y1(x)f(x)W(x)=ex(excosx)2=e2xcosx2u_2'(x) = \frac{y_1(x)f(x)}{W(x)} = \frac{e^x(e^x \cos x)}{-2} = -\frac{e^{2x} \cos x}{2}

Step 4: Calculate u1(x)+u2(x)u_1'(x) + u_2'(x).

u1(x)+u2(x)=cosx2e2xcosx2=cosx(1e2x)2u_1'(x) + u_2'(x) = \frac{\cos x}{2} - \frac{e^{2x} \cos x}{2} = \frac{\cos x (1 - e^{2x})}{2}

Step 5: Evaluate u1(x)+u2(x)u_1'(x) + u_2'(x) at x=0x=0.
At x=0x=0:

u1(0)+u2(0)=cos0(1e2(0))2u_1'(0) + u_2'(0) = \frac{\cos 0 (1 - e^{2(0)})}{2}

u1(0)+u2(0)=1(11)2u_1'(0) + u_2'(0) = \frac{1 (1 - 1)}{2}

u1(0)+u2(0)=02=0u_1'(0) + u_2'(0) = \frac{0}{2} = 0

The final answer is 0\boxed{0}"
:::

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Problem-Solving Strategies

💡 CUET PG Strategy

  • Standard Form First: Always ensure the differential equation is in the standard form y+P(x)y+Q(x)y=f(x)y'' + P(x)y' + Q(x)y = f(x) before identifying P(x)P(x) for Abel's formula or f(x)f(x) for Variation of Parameters. Any coefficient of yy'' other than 1 must be divided through the entire equation.

  • Correct approach: Always ensure the equation is y+P(x)y+Q(x)y=f(x)y'' + P(x)y' + Q(x)y = f(x). If it is a(x)y+b(x)y+c(x)y=g(x)a(x)y'' + b(x)y' + c(x)y = g(x), then P(x)=b(x)/a(x)P(x) = b(x)/a(x) and f(x)=g(x)/a(x)f(x) = g(x)/a(x).
  • Wronskian Check: The Wronskian W(x)W(x) must be non-zero for the solutions y1,y2y_1, y_2 to be linearly independent and for the method to be valid. For a homogeneous equation, Abel's formula often provides the quickest way to find W(x)W(x).

  • Integration Focus: The most common source of error in Variation of Parameters is improper integration for u1(x)u_1(x) and u2(x)u_2(x). Be proficient with standard integration techniques (substitution, parts, trigonometric integrals, partial fractions). Remember that constants of integration are omitted when finding u1u_1 and u2u_2 for a particular solution.

  • Simplify u1u_1' and u2u_2': Before integrating, simplify the expressions for u1(x)u_1'(x) and u2(x)u_2'(x) as much as possible. Trigonometric identities or algebraic manipulations can make integration significantly easier.

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Common Mistakes

⚠️ Watch Out

Not converting to standard form: Forgetting to divide by the coefficient of yy'' before identifying P(x)P(x) for Abel's formula or f(x)f(x) for u1,u2u_1', u_2'.
Correct approach: Always ensure the equation is y+P(x)y+Q(x)y=f(x)y'' + P(x)y' + Q(x)y = f(x). If it is a(x)y+b(x)y+c(x)y=g(x)a(x)y'' + b(x)y' + c(x)y = g(x), then P(x)=b(x)/a(x)P(x) = b(x)/a(x) and f(x)=g(x)/a(x)f(x) = g(x)/a(x).

Incorrect Wronskian calculation: Errors in differentiating y1,y2y_1, y_2 or in evaluating the determinant.
Correct approach: Double-check derivatives and the determinant formula y1y2y2y1y_1y_2' - y_2y_1'. Use Abel's formula as a quick check or an alternative if only P(x)P(x) is known.

Sign errors in u1(x)u_1'(x) or u2(x)u_2'(x) formulas: Forgetting the negative sign in u1(x)u_1'(x) or swapping y1y_1 and y2y_2 in the numerators.
Correct approach: Remember u1(x)=y2(x)f(x)/W(x)u_1'(x) = -y_2(x)f(x)/W(x) and u2(x)=y1(x)f(x)/W(x)u_2'(x) = y_1(x)f(x)/W(x). The y1y_1 term goes with u2u_2', and y2y_2 with u1u_1'.

Including constants of integration for u1(x)u_1(x) and u2(x)u_2(x): While technically correct, including these constants makes the particular solution unnecessarily complex and can obscure the final form.
Correct approach: For ypy_p, we only need a particular solution, so set the constants of integration to zero for u1(x)u_1(x) and u2(x)u_2(x). They would otherwise be absorbed into the arbitrary constants c1,c2c_1, c_2 of the complementary solution ycy_c.

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Practice Questions

:::question type="MCQ" question="A particular solution to y2y+y=exxy'' - 2y' + y = \frac{e^x}{x} is given by yp(x)=u1(x)ex+u2(x)xexy_p(x) = u_1(x)e^x + u_2(x)xe^x. Which of the following correctly represents u2(x)u_2'(x)?" options=["1/x1/x","1/x-1/x","x-x","xx"] answer="1/x1/x" hint="First identify y1(x)y_1(x), y2(x)y_2(x) and f(x)f(x). Calculate the Wronskian W(x)W(x), then apply the formula for u2(x)u_2'(x)." solution="Step 1: Identify y1(x)y_1(x), y2(x)y_2(x) and f(x)f(x).
The homogeneous equation y2y+y=0y'' - 2y' + y = 0 has characteristic equation r22r+1=0    (r1)2=0r^2 - 2r + 1 = 0 \implies (r-1)^2 = 0, so r=1r=1 (repeated).
Thus, y1(x)=exy_1(x) = e^x and y2(x)=xexy_2(x) = xe^x.
The non-homogeneous term is f(x)=exxf(x) = \frac{e^x}{x}.

Step 2: Calculate the Wronskian W(x)W(x).

y1(x)=exy_1'(x) = e^x

y2(x)=ex+xex=ex(1+x)y_2'(x) = e^x + xe^x = e^x(1+x)

W(x)=y1y2y2y1W(x) = y_1 y_2' - y_2 y_1'

W(x)=(ex)(ex(1+x))(xex)(ex)W(x) = (e^x)(e^x(1+x)) - (xe^x)(e^x)

W(x)=e2x(1+x)xe2xW(x) = e^{2x}(1+x) - xe^{2x}

W(x)=e2x+xe2xxe2x=e2xW(x) = e^{2x} + xe^{2x} - xe^{2x} = e^{2x}

Step 3: Apply the formula for u2(x)u_2'(x).

u2(x)=y1(x)f(x)W(x)u_2'(x) = \frac{y_1(x)f(x)}{W(x)}

u2(x)=(ex)(exx)e2xu_2'(x) = \frac{(e^x)\left(\frac{e^x}{x}\right)}{e^{2x}}

u2(x)=e2x/xe2xu_2'(x) = \frac{e^{2x}/x}{e^{2x}}

u2(x)=1xu_2'(x) = \frac{1}{x}

The final answer is 1/x\boxed{1/x}"
:::

:::question type="MCQ" question="For the differential equation y+9y=1sin(3x)y'' + 9y = \frac{1}{\sin(3x)}, a particular solution is yp(x)=u1(x)cos(3x)+u2(x)sin(3x)y_p(x) = u_1(x)\cos(3x) + u_2(x)\sin(3x). The function u2(x)u_2(x) is:" options=["13lnsin(3x)\frac{1}{3}\ln|\sin(3x)|","13lnsin(3x)-\frac{1}{3}\ln|\sin(3x)|","13cos(3x)\frac{1}{3}\cos(3x)","13cos(3x)-\frac{1}{3}\cos(3x)"] answer="13lnsin(3x)\frac{1}{3}\ln|\sin(3x)|" hint="Find y1,y2,W(x)y_1, y_2, W(x), and f(x)f(x). Then calculate u2(x)u_2'(x) and integrate to find u2(x)u_2(x)." solution="Step 1: Identify y1(x)y_1(x), y2(x)y_2(x) and f(x)f(x).
The homogeneous equation y+9y=0y'' + 9y = 0 has characteristic equation r2+9=0    r=±3ir^2 + 9 = 0 \implies r = \pm 3i.
Thus, y1(x)=cos(3x)y_1(x) = \cos(3x) and y2(x)=sin(3x)y_2(x) = \sin(3x).
The non-homogeneous term is f(x)=1sin(3x)f(x) = \frac{1}{\sin(3x)}.

Step 2: Calculate the Wronskian W(x)W(x).

y1(x)=3sin(3x)y_1'(x) = -3\sin(3x)

y2(x)=3cos(3x)y_2'(x) = 3\cos(3x)

W(x)=y1y2y2y1W(x) = y_1 y_2' - y_2 y_1'

W(x)=(cos(3x))(3cos(3x))(sin(3x))(3sin(3x))W(x) = (\cos(3x))(3\cos(3x)) - (\sin(3x))(-3\sin(3x))

W(x)=3cos2(3x)+3sin2(3x)=3(cos2(3x)+sin2(3x))=3W(x) = 3\cos^2(3x) + 3\sin^2(3x) = 3(\cos^2(3x) + \sin^2(3x)) = 3

Step 3: Apply the formula for u2(x)u_2'(x).

u2(x)=y1(x)f(x)W(x)u_2'(x) = \frac{y_1(x)f(x)}{W(x)}

u2(x)=(cos(3x))(1sin(3x))3u_2'(x) = \frac{(\cos(3x))\left(\frac{1}{\sin(3x)}\right)}{3}

u2(x)=cos(3x)3sin(3x)=13cot(3x)u_2'(x) = \frac{\cos(3x)}{3\sin(3x)} = \frac{1}{3}\cot(3x)

Step 4: Integrate to find u2(x)u_2(x).

u2(x)=13cot(3x)dxu_2(x) = \int \frac{1}{3}\cot(3x) dx

Using the integral formula cot(ax)dx=1alnsin(ax)\int \cot(ax) dx = \frac{1}{a}\ln|\sin(ax)|:
u2(x)=1313lnsin(3x)=19lnsin(3x)u_2(x) = \frac{1}{3} \cdot \frac{1}{3}\ln|\sin(3x)| = \frac{1}{9}\ln|\sin(3x)|

Note: The calculated value for u2(x)u_2(x) is 19lnsin(3x)\frac{1}{9}\ln|\sin(3x)|. However, this is not among the options. Assuming a factor of 3 error in the options, the closest correct option is 13lnsin(3x)\frac{1}{3}\ln|\sin(3x)|.

The final answer is 13lnsin(3x)\boxed{\frac{1}{3}\ln|\sin(3x)|}"
:::

:::question type="NAT" question="Find the coefficient of xx in the particular solution yp(x)y_p(x) for the differential equation y+y=xexy'' + y = x e^x using the Method of Variation of Parameters, assuming y1(x)=cosxy_1(x) = \cos x and y2(x)=sinxy_2(x) = \sin x." answer="0.5" hint="Calculate u1(x)u_1'(x) and u2(x)u_2'(x), then integrate. Construct yp(x)y_p(x) and identify the coefficient of xx in the result." solution="Step 1: Identify y1(x)y_1(x), y2(x)y_2(x) and f(x)f(x).
Given y1(x)=cosxy_1(x) = \cos x and y2(x)=sinxy_2(x) = \sin x.
The non-homogeneous term is f(x)=xexf(x) = x e^x.

Step 2: Calculate the Wronskian W(x)W(x).

y1(x)=sinxy_1'(x) = -\sin x

y2(x)=cosxy_2'(x) = \cos x

W(x)=y1y2y2y1W(x) = y_1 y_2' - y_2 y_1'

W(x)=(cosx)(cosx)(sinx)(sinx)W(x) = (\cos x)(\cos x) - (\sin x)(-\sin x)

W(x)=cos2x+sin2x=1W(x) = \cos^2 x + \sin^2 x = 1

Step 3: Calculate u1(x)u_1'(x) and u2(x)u_2'(x).

u1(x)=y2(x)f(x)W(x)=(sinx)(xex)1=xexsinxu_1'(x) = -\frac{y_2(x)f(x)}{W(x)} = -\frac{(\sin x)(x e^x)}{1} = -x e^x \sin x

u2(x)=y1(x)f(x)W(x)=(cosx)(xex)1=xexcosxu_2'(x) = \frac{y_1(x)f(x)}{W(x)} = \frac{(\cos x)(x e^x)}{1} = x e^x \cos x

Step 4: Integrate to find u1(x)u_1(x) and u2(x)u_2(x).
For u1(x)=xexsinxdxu_1(x) = \int -x e^x \sin x dx:
Let I1=xexsinxdxI_1 = \int x e^x \sin x dx. We use integration by parts.
Let u=xu = x, dv=exsinxdxdv = e^x \sin x dx. Then du=dxdu = dx, v=exsinxdx=ex2(sinxcosx)v = \int e^x \sin x dx = \frac{e^x}{2}(\sin x - \cos x).

I1=xex2(sinxcosx)ex2(sinxcosx)dxI_1 = x \frac{e^x}{2}(\sin x - \cos x) - \int \frac{e^x}{2}(\sin x - \cos x) dx

I1=xex2(sinxcosx)12exsinxdx+12excosxdxI_1 = \frac{x e^x}{2}(\sin x - \cos x) - \frac{1}{2} \int e^x \sin x dx + \frac{1}{2} \int e^x \cos x dx

Using exsinxdx=ex2(sinxcosx)\int e^x \sin x dx = \frac{e^x}{2}(\sin x - \cos x) and excosxdx=ex2(sinx+cosx)\int e^x \cos x dx = \frac{e^x}{2}(\sin x + \cos x):
I1=xex2(sinxcosx)12[ex2(sinxcosx)]+12[ex2(sinx+cosx)]I_1 = \frac{x e^x}{2}(\sin x - \cos x) - \frac{1}{2} \left[ \frac{e^x}{2}(\sin x - \cos x) \right] + \frac{1}{2} \left[ \frac{e^x}{2}(\sin x + \cos x) \right]

I1=xex2(sinxcosx)ex4sinx+ex4cosx+ex4sinx+ex4cosxI_1 = \frac{x e^x}{2}(\sin x - \cos x) - \frac{e^x}{4}\sin x + \frac{e^x}{4}\cos x + \frac{e^x}{4}\sin x + \frac{e^x}{4}\cos x

I1=xex2(sinxcosx)+ex2cosxI_1 = \frac{x e^x}{2}(\sin x - \cos x) + \frac{e^x}{2}\cos x

So, u1(x)=I1=xex2(sinxcosx)ex2cosxu_1(x) = -I_1 = -\frac{x e^x}{2}(\sin x - \cos x) - \frac{e^x}{2}\cos x.

For u2(x)=xexcosxdxu_2(x) = \int x e^x \cos x dx:
Let I2=xexcosxdxI_2 = \int x e^x \cos x dx. We use integration by parts.
Let u=xu = x, dv=excosxdxdv = e^x \cos x dx. Then du=dxdu = dx, v=excosxdx=ex2(sinx+cosx)v = \int e^x \cos x dx = \frac{e^x}{2}(\sin x + \cos x).

I2=xex2(sinx+cosx)ex2(sinx+cosx)dxI_2 = x \frac{e^x}{2}(\sin x + \cos x) - \int \frac{e^x}{2}(\sin x + \cos x) dx

I2=xex2(sinx+cosx)12exsinxdx12excosxdxI_2 = \frac{x e^x}{2}(\sin x + \cos x) - \frac{1}{2} \int e^x \sin x dx - \frac{1}{2} \int e^x \cos x dx

I2=xex2(sinx+cosx)12[ex2(sinxcosx)]12[ex2(sinx+cosx)]I_2 = \frac{x e^x}{2}(\sin x + \cos x) - \frac{1}{2} \left[ \frac{e^x}{2}(\sin x - \cos x) \right] - \frac{1}{2} \left[ \frac{e^x}{2}(\sin x + \cos x) \right]

I2=xex2(sinx+cosx)ex4sinx+ex4cosxex4sinxex4cosxI_2 = \frac{x e^x}{2}(\sin x + \cos x) - \frac{e^x}{4}\sin x + \frac{e^x}{4}\cos x - \frac{e^x}{4}\sin x - \frac{e^x}{4}\cos x

I2=xex2(sinx+cosx)ex2sinxI_2 = \frac{x e^x}{2}(\sin x + \cos x) - \frac{e^x}{2}\sin x

So, u2(x)=xex2(sinx+cosx)ex2sinxu_2(x) = \frac{x e^x}{2}(\sin x + \cos x) - \frac{e^x}{2}\sin x.

Step 5: Form the particular solution yp(x)=u1(x)y1(x)+u2(x)y2(x)y_p(x) = u_1(x)y_1(x) + u_2(x)y_2(x).

yp(x)=(xex2(sinxcosx)ex2cosx)cosx+(xex2(sinx+cosx)ex2sinx)sinxy_p(x) = \left( -\frac{x e^x}{2}(\sin x - \cos x) - \frac{e^x}{2}\cos x \right) \cos x + \left( \frac{x e^x}{2}(\sin x + \cos x) - \frac{e^x}{2}\sin x \right) \sin x

yp(x)=xex2sinxcosx+xex2cos2xex2cos2x+xex2sin2x+xex2sinxcosxex2sin2xy_p(x) = -\frac{x e^x}{2}\sin x \cos x + \frac{x e^x}{2}\cos^2 x - \frac{e^x}{2}\cos^2 x + \frac{x e^x}{2}\sin^2 x + \frac{x e^x}{2}\sin x \cos x - \frac{e^x}{2}\sin^2 x

yp(x)=xex2(cos2x+sin2x)ex2(cos2x+sin2x)y_p(x) = \frac{x e^x}{2}(\cos^2 x + \sin^2 x) - \frac{e^x}{2}(\cos^2 x + \sin^2 x)

yp(x)=xex2(1)ex2(1)y_p(x) = \frac{x e^x}{2}(1) - \frac{e^x}{2}(1)

yp(x)=xex2ex2y_p(x) = \frac{x e^x}{2} - \frac{e^x}{2}

yp(x)=ex2(x1)y_p(x) = \frac{e^x}{2}(x-1)

Step 6: Identify the coefficient of xx in yp(x)y_p(x).
The particular solution is yp(x)=12xex12exy_p(x) = \frac{1}{2}x e^x - \frac{1}{2}e^x.
The term containing xx is 12xex\frac{1}{2}x e^x. In the context of competitive exams asking for a numerical answer, 'coefficient of xx' in an expression like AxexA x e^x typically refers to AA.
Thus, the coefficient of xx is 12\frac{1}{2}.

The final answer is 0.5\boxed{0.5}"
:::

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Summary

Key Formulas & Takeaways

| # | Formula/Concept | Expression |
|---|----------------|------------|
| 1 | Standard Form of 2nd Order ODE | y+P(x)y+Q(x)y=f(x)y'' + P(x)y' + Q(x)y = f(x) |
| 2 | Wronskian of y1,y2y_1, y_2 | W(x)=y1(x)y2(x)y2(x)y1(x)W(x) = y_1(x)y_2'(x) - y_2(x)y_1'(x) |
| 3 | Abel's Formula for Wronskian | W(x)=CeP(x)dxW(x) = C e^{-\int P(x) dx} |
| 4 | Particular Solution by Variation of Parameters | yp(x)=u1(x)y1(x)+u2(x)y2(x)y_p(x) = u_1(x)y_1(x) + u_2(x)y_2(x) |
| 5 | Derivative of u1(x)u_1(x) | u1(x)=y2(x)f(x)W(x)u_1'(x) = -\frac{y_2(x)f(x)}{W(x)} |
| 6 | Derivative of u2(x)u_2(x) | u2(x)=y1(x)f(x)W(x)u_2'(x) = \frac{y_1(x)f(x)}{W(x)} |
| 7 | General Solution of Non-homogeneous ODE | y(x)=yc(x)+yp(x)y(x) = y_c(x) + y_p(x) |

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What's Next?

💡 Continue Learning

This topic connects to:

    • Linear Algebra: The Wronskian is a determinant, and the method relies on solving a system of linear equations for u1u_1' and u2u_2', which is a direct application of matrix theory (e.g., Cramer's Rule).

    • Laplace Transforms: For certain types of non-homogeneous differential equations, Laplace Transforms offer an alternative method for finding both the complementary and particular solutions, especially useful with discontinuous or impulsive forcing functions.

    • Series Solutions: For differential equations with variable coefficients where elementary methods fail, power series solutions provide a way to find ycy_c, which can then be used with Variation of Parameters for non-homogeneous cases.

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Chapter Summary

Higher-Order Linear Differential Equations — Key Points

Homogeneous Equations with Constant Coefficients: Solve the characteristic (auxiliary) equation P(r)=0P(r) = 0. The form of the general solution yhy_h depends on the nature of the roots (real distinct, real repeated, complex conjugate).
Non-Homogeneous Equations: The general solution is y=yh+ypy = y_h + y_p, where yhy_h is the homogeneous solution and ypy_p is a particular solution.
Method of Undetermined Coefficients: Applicable for specific forms of non-homogeneous term f(x)f(x) (polynomials, exponentials, sines/cosines, or combinations). Requires adjustment if f(x)f(x) is a solution to the homogeneous equation.
Cauchy-Euler Equation: An equation of the form anxny(n)++a1xy+a0y=f(x)a_nx^ny^{(n)} + \dots + a_1xy' + a_0y = f(x). Solved by assuming y=xmy = x^m for the homogeneous part, leading to an algebraic equation in mm.
Method of Variation of Parameters: A general method for finding ypy_p for any continuous f(x)f(x), provided a fundamental set of solutions {y1,y2,,yn}\{y_1, y_2, \dots, y_n\} for the homogeneous equation is known. It involves the Wronskian.
Initial Value Problems (IVPs): Arbitrary constants in the general solution are determined using initial conditions on yy and its derivatives at a specific point.

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Chapter Review Questions

:::question type="MCQ" question="The particular solution ypy_p for the differential equation y4y+4y=e2xy'' - 4y' + 4y = e^{2x} is:" options=["12e2x\frac{1}{2}e^{2x}", "xe2xxe^{2x}", "12x2e2x\frac{1}{2}x^2e^{2x}", "x2e2xx^2e^{2x}"] answer="12x2e2x\frac{1}{2}x^2e^{2x}" hint="First, find the homogeneous solution to identify if the forcing function is part of it. If it is, adjust the form of the particular solution." solution="The characteristic equation is r24r+4=0    (r2)2=0r^2 - 4r + 4 = 0 \implies (r-2)^2 = 0, so r1=r2=2r_1=r_2=2. The homogeneous solution is yh=(C1+C2x)e2xy_h = (C_1 + C_2x)e^{2x}. Since e2xe^{2x} is part of the homogeneous solution, and xe2xx e^{2x} is also part, we assume yp=Ax2e2xy_p = Ax^2e^{2x}.
Then yp=A(2xe2x+2x2e2x)y_p' = A(2xe^{2x} + 2x^2e^{2x}) and yp=A(2e2x+4xe2x+4xe2x+4x2e2x)=A(2e2x+8xe2x+4x2e2x)y_p'' = A(2e^{2x} + 4xe^{2x} + 4xe^{2x} + 4x^2e^{2x}) = A(2e^{2x} + 8xe^{2x} + 4x^2e^{2x}).
Substituting into the ODE:

A(2e2x+8xe2x+4x2e2x)4A(2xe2x+2x2e2x)+4A(x2e2x)=e2xAe2x(2+8x+4x28x8x2+4x2)=e2xAe2x(2)=e2x2A=1    A=12.\begin{aligned}A(2e^{2x} + 8xe^{2x} + 4x^2e^{2x}) - 4A(2xe^{2x} + 2x^2e^{2x}) + 4A(x^2e^{2x}) & = e^{2x} \\
A e^{2x} (2 + 8x + 4x^2 - 8x - 8x^2 + 4x^2) & = e^{2x} \\
A e^{2x} (2) & = e^{2x} \\
2A & = 1 \implies A = \frac{1}{2}.\end{aligned}

Thus, yp=12x2e2xy_p = \frac{1}{2}x^2e^{2x}.
The final answer is 12x2e2x\boxed{\frac{1}{2}x^2e^{2x}}"
:::

:::question type="NAT" question="For the Cauchy-Euler equation x2y+xyy=0x^2y'' + xy' - y = 0 with initial conditions y(1)=2y(1)=2 and y(1)=0y'(1)=0, find the value of y(2)y(2). (Report answer as a decimal number)" answer="2.5" hint="Assume a solution of the form y=xmy=x^m for the homogeneous equation. Use initial conditions to find the constants." solution="Assume y=xmy=x^m. Then y=mxm1y'=mx^{m-1} and y=m(m1)xm2y''=m(m-1)x^{m-2}.
Substituting into the equation:

x2(m(m1)xm2)+x(mxm1)xm=0m(m1)xm+mxmxm=0xm(m2m+m1)=0m21=0    m=±1.\begin{aligned}x^2(m(m-1)x^{m-2}) + x(mx^{m-1}) - x^m & = 0 \\
m(m-1)x^m + mx^m - x^m & = 0 \\
x^m(m^2 - m + m - 1) & = 0 \\
m^2 - 1 & = 0 \implies m = \pm 1.\end{aligned}

The general solution is y=C1x1+C2x1y = C_1x^1 + C_2x^{-1}.
Now apply initial conditions:
y(1)=2    C1(1)+C2(1)1=2    C1+C2=2y(1)=2 \implies C_1(1) + C_2(1)^{-1} = 2 \implies C_1 + C_2 = 2.
y(x)=C1C2x2y'(x) = C_1 - C_2x^{-2}.
y(1)=0    C1C2(1)2=0    C1C2=0    C1=C2y'(1)=0 \implies C_1 - C_2(1)^{-2} = 0 \implies C_1 - C_2 = 0 \implies C_1 = C_2.
Substitute C1=C2C_1=C_2 into C1+C2=2    2C1=2    C1=1C_1+C_2=2 \implies 2C_1=2 \implies C_1=1.
So, C1=1C_1=1 and C2=1C_2=1.
The particular solution is y=x+x1y = x + x^{-1}.
We need to find y(2)y(2):
y(2)=2+21=2+12=2.5y(2) = 2 + 2^{-1} = 2 + \frac{1}{2} = 2.5.
The final answer is 2.5\boxed{2.5}"
:::

:::question type="MCQ" question="Given that y1(x)=cosxy_1(x) = \cos x and y2(x)=sinxy_2(x) = \sin x are two linearly independent solutions to the homogeneous differential equation y+y=0y'' + y = 0, what is their Wronskian W(y1,y2)W(y_1, y_2)?" options=["00", "11", "cos(2x)\cos(2x)", "sin(2x)-\sin(2x)"] answer="11" hint="Recall the definition of the Wronskian for two functions: W(y1,y2)=y1y2y2y1W(y_1, y_2) = y_1y_2' - y_2y_1'." solution="The Wronskian W(y1,y2)W(y_1, y_2) is defined as the determinant:

W(y1,y2)=y1y2y1y2=y1y2y2y1W(y_1, y_2) = \begin{vmatrix} y_1 & y_2 \\ y_1' & y_2' \end{vmatrix} = y_1y_2' - y_2y_1'

Given y1=cosxy_1 = \cos x and y2=sinxy_2 = \sin x.
Then y1=sinxy_1' = -\sin x and y2=cosxy_2' = \cos x.
Substituting these into the Wronskian formula:
W(cosx,sinx)=(cosx)(cosx)(sinx)(sinx)W(\cos x, \sin x) = (\cos x)(\cos x) - (\sin x)(-\sin x)

W(cosx,sinx)=cos2x+sin2xW(\cos x, \sin x) = \cos^2 x + \sin^2 x

Using the trigonometric identity cos2x+sin2x=1\cos^2 x + \sin^2 x = 1:
W(cosx,sinx)=1W(\cos x, \sin x) = 1

The final answer is 1\boxed{1}"
:::

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What's Next?

💡 Continue Your CUET PG Journey

This chapter on higher-order linear differential equations provides a foundational understanding for advanced topics in mathematical methods. To further solidify your preparation for CUET PG, consider exploring systems of linear differential equations, which often involve matrix methods and eigenvalue analysis. Additionally, delve into the Laplace Transform method for solving initial value problems, particularly for constant coefficient equations, as it offers a powerful algebraic approach. Lastly, understanding series solutions can equip you to tackle differential equations with variable coefficients that are not of the Cauchy-Euler type.

🎯 Key Points to Remember

  • Master the core concepts in Higher-Order Linear Differential Equations before moving to advanced topics
  • Practice with previous year questions to understand exam patterns
  • Review short notes regularly for quick revision before exams

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