100% FREE Updated: Apr 2026 Real Analysis Calculus of a Single Variable

Power Series

Comprehensive study notes on Power Series for CUET PG Mathematics preparation. This chapter covers key concepts, formulas, and examples needed for your exam.

Power Series

This chapter meticulously explores power series, detailing their convergence criteria and essential analytical properties. A thorough understanding of these concepts is paramount for the CUET PG MA examination, as power series form a fundamental cornerstone of Real Analysis and are consistently featured in problem-solving scenarios.

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Chapter Contents

| # | Topic |
|---|-------|
| 1 | Convergence of Power Series |
| 2 | Properties of Power Series |

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We begin with Convergence of Power Series.

Part 1: Convergence of Power Series

Power series are fundamental in analysis, offering a means to represent functions as infinite sums. Understanding their convergence properties is critical for their application in calculus, differential equations, and complex analysis, making it a recurring topic in competitive examinations. We investigate the methods for determining the domain over which such series converge.

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Core Concepts

1. Definition of a Power Series

A power series is an infinite series of the form βˆ‘n=0∞cn(xβˆ’a)n\sum_{n=0}^{\infty} c_n (x-a)^n, where cnc_n are coefficients, xx is a variable, and aa is the center of the series. For simplicity, we often consider series centered at a=0a=0, i.e., βˆ‘n=0∞cnxn\sum_{n=0}^{\infty} c_n x^n.

πŸ“– Power Series

A power series centered at aa is an expression of the form

βˆ‘n=0∞cn(xβˆ’a)n=c0+c1(xβˆ’a)+c2(xβˆ’a)2+…\sum_{n=0}^{\infty} c_n (x-a)^n = c_0 + c_1(x-a) + c_2(x-a)^2 + \dots

2. Radius of Convergence

For every power series, there exists a unique non-negative real number RR, called the radius of convergence, such that the series converges absolutely for ∣xβˆ’a∣<R|x-a| < R and diverges for ∣xβˆ’a∣>R|x-a| > R. At the endpoints, ∣xβˆ’a∣=R|x-a|=R, the series may converge or diverge.

πŸ“ Radius of Convergence using Ratio Test

Let the power series be βˆ‘n=0∞cn(xβˆ’a)n\sum_{n=0}^{\infty} c_n (x-a)^n. If

L=lim⁑nβ†’βˆžβˆ£cn+1cn∣L = \lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right|

exists, then the radius of convergence RR is given by:
R=1LR = \frac{1}{L}

If L=0L=0, then R=∞R=\infty (series converges for all xx). If L=∞L=\infty, then R=0R=0 (series converges only at x=ax=a).
When to use: When cnc_n involves factorials or products.

Quick Example: Ratio Test

We determine the radius of convergence for the series βˆ‘n=1∞n22nxn\sum_{n=1}^{\infty} \frac{n^2}{2^n} x^n.

Step 1: Identify the coefficient cnc_n.
>

cn=n22nc_n = \frac{n^2}{2^n}

Step 2: Compute the limit L=lim⁑nβ†’βˆžβˆ£cn+1cn∣L = \lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right|.
>

L=lim⁑nβ†’βˆžβˆ£(n+1)2/2n+1n2/2n∣=lim⁑nβ†’βˆžβˆ£(n+1)22n+1β‹…2nn2∣=lim⁑nβ†’βˆžβˆ£(n+1)22n2∣=lim⁑nβ†’βˆž12(n+1n)2=12(1)2=12\begin{aligned} L & = \lim_{n \to \infty} \left| \frac{(n+1)^2 / 2^{n+1}}{n^2 / 2^n} \right| \\ & = \lim_{n \to \infty} \left| \frac{(n+1)^2}{2^{n+1}} \cdot \frac{2^n}{n^2} \right| \\ & = \lim_{n \to \infty} \left| \frac{(n+1)^2}{2n^2} \right| \\ & = \lim_{n \to \infty} \frac{1}{2} \left( \frac{n+1}{n} \right)^2 \\ & = \frac{1}{2} (1)^2 = \frac{1}{2} \end{aligned}

Step 3: Calculate R=1LR = \frac{1}{L}.
>

R=11/2=2R = \frac{1}{1/2} = 2

Answer: 2\boxed{2}

:::question type="MCQ" question="The radius of convergence of the power series βˆ‘n=1∞(n!)2(2n)!xn\sum_{n=1}^{\infty} \frac{(n!)^2}{(2n)!} x^n is:" options=["1/41/4","22","44","∞\infty"] answer="44" hint="Apply the Ratio Test. Recall that

(2(n+1))!=(2n+2)!=(2n+2)(2n+1)(2n)!(2(n+1))! = (2n+2)! = (2n+2)(2n+1)(2n)!
" solution="Step 1: Identify cnc_n.
>
cn=(n!)2(2n)!c_n = \frac{(n!)^2}{(2n)!}

Step 2: Compute L=lim⁑nβ†’βˆžβˆ£cn+1cn∣L = \lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right|.
>

L=lim⁑nβ†’βˆžβˆ£((n+1)!)2/(2(n+1))!(n!)2/(2n)!∣=lim⁑nβ†’βˆžβˆ£((n+1)!)2(2n+2)!β‹…(2n)!(n!)2∣=lim⁑nβ†’βˆžβˆ£(n+1)2(n!)2(2n+2)(2n+1)(2n)!β‹…(2n)!(n!)2∣=lim⁑nβ†’βˆž(n+1)2(2n+2)(2n+1)=lim⁑nβ†’βˆžn2+2n+14n2+6n+2=lim⁑nβ†’βˆž1+2/n+1/n24+6/n+2/n2=14\begin{aligned} L & = \lim_{n \to \infty} \left| \frac{((n+1)!)^2 / (2(n+1))!}{(n!)^2 / (2n)!} \right| \\ & = \lim_{n \to \infty} \left| \frac{((n+1)!)^2}{(2n+2)!} \cdot \frac{(2n)!}{(n!)^2} \right| \\ & = \lim_{n \to \infty} \left| \frac{(n+1)^2 (n!)^2}{(2n+2)(2n+1)(2n)!} \cdot \frac{(2n)!}{(n!)^2} \right| \\ & = \lim_{n \to \infty} \frac{(n+1)^2}{(2n+2)(2n+1)} \\ & = \lim_{n \to \infty} \frac{n^2+2n+1}{4n^2+6n+2} \\ & = \lim_{n \to \infty} \frac{1+2/n+1/n^2}{4+6/n+2/n^2} \\ & = \frac{1}{4} \end{aligned}

Step 3: Calculate R=1LR = \frac{1}{L}.
>

R=11/4=4R = \frac{1}{1/4} = 4

Answer: 4\boxed{4}
"
:::

πŸ“ Radius of Convergence using Root Test

Let the power series be βˆ‘n=0∞cn(xβˆ’a)n\sum_{n=0}^{\infty} c_n (x-a)^n. If

L=lim⁑nβ†’βˆžβˆ£cn∣nL = \lim_{n \to \infty} \sqrt[n]{|c_n|}

exists, then the radius of convergence RR is given by:
R=1LR = \frac{1}{L}

If L=0L=0, then R=∞R=\infty. If L=∞L=\infty, then R=0R=0.
When to use: When cnc_n involves nn-th powers.

Quick Example: Root Test

We find the radius of convergence for the series βˆ‘n=1∞(n+1n)nxn\sum_{n=1}^{\infty} \left(\frac{n+1}{n}\right)^n x^n.

Step 1: Identify the coefficient cnc_n.
>

cn=(n+1n)nc_n = \left(\frac{n+1}{n}\right)^n

Step 2: Compute the limit L=lim⁑nβ†’βˆžβˆ£cn∣nL = \lim_{n \to \infty} \sqrt[n]{|c_n|}.
>

L=lim⁑nβ†’βˆžβˆ£(n+1n)n∣n=lim⁑nβ†’βˆžn+1n=lim⁑nβ†’βˆž(1+1n)=1\begin{aligned} L & = \lim_{n \to \infty} \sqrt[n]{\left|\left(\frac{n+1}{n}\right)^n\right|} \\ & = \lim_{n \to \infty} \frac{n+1}{n} \\ & = \lim_{n \to \infty} \left(1 + \frac{1}{n}\right) \\ & = 1 \end{aligned}

Step 3: Calculate R=1LR = \frac{1}{L}.
>

R=11=1R = \frac{1}{1} = 1

Answer: 1\boxed{1}

:::question type="MCQ" question="The radius of convergence of the power series βˆ‘n=1∞(nn+1)n2zn\sum_{n=1}^{\infty} \left(\frac{n}{n+1}\right)^{n^2} z^n is:" options=["ee","1/e1/e","11","∞\infty"] answer="ee" hint="Use the Root Test. Recall that

lim⁑nβ†’βˆž(1+1n)n=e\lim_{n \to \infty} \left(1 + \frac{1}{n}\right)^n = e
" solution="Step 1: Identify cnc_n.
>
cn=(nn+1)n2c_n = \left(\frac{n}{n+1}\right)^{n^2}

Step 2: Compute L=lim⁑nβ†’βˆžβˆ£cn∣nL = \lim_{n \to \infty} \sqrt[n]{|c_n|}.
>

L=lim⁑nβ†’βˆžβˆ£(nn+1)n2∣n=lim⁑nβ†’βˆž(nn+1)n=lim⁑nβ†’βˆž(11+1/n)n=1lim⁑nβ†’βˆž(1+1/n)n=1e\begin{aligned} L & = \lim_{n \to \infty} \sqrt[n]{\left|\left(\frac{n}{n+1}\right)^{n^2}\right|} \\ & = \lim_{n \to \infty} \left(\frac{n}{n+1}\right)^n \\ & = \lim_{n \to \infty} \left(\frac{1}{1 + 1/n}\right)^n \\ & = \frac{1}{\lim_{n \to \infty} (1 + 1/n)^n} \\ & = \frac{1}{e} \end{aligned}

Step 3: Calculate R=1LR = \frac{1}{L}.
>

R=11/e=eR = \frac{1}{1/e} = e

Answer: e\boxed{e}
"
:::

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3. Interval of Convergence

The interval of convergence is the set of all xx values for which the power series converges. It is determined by the radius of convergence RR and the behavior of the series at the endpoints x=aΒ±Rx = a \pm R.

For a series centered at aa:
* If R=0R=0, the interval is {a}\{a\}.
* If R=∞R=\infty, the interval is (βˆ’βˆž,∞)(-\infty, \infty).
* If 0<R<∞0 < R < \infty, the series converges absolutely on (aβˆ’R,a+R)(a-R, a+R). We must test the endpoints x=aβˆ’Rx=a-R and x=a+Rx=a+R separately using appropriate convergence tests for series of constants.

πŸ’‘ Endpoint Tests

At the endpoints, the power series becomes a series of constants. We employ standard convergence tests:
p-series test: βˆ‘1np\sum \frac{1}{n^p} converges if p>1p>1, diverges if p≀1p \le 1.
Alternating Series Test: For βˆ‘(βˆ’1)nbn\sum (-1)^n b_n, converges if bnb_n is positive, decreasing, and lim⁑nβ†’βˆžbn=0\lim_{n \to \infty} b_n = 0.
Comparison Test/Limit Comparison Test: Compare with a known convergent or divergent series.
Divergence Test: If lim⁑nβ†’βˆžanβ‰ 0\lim_{n \to \infty} a_n \neq 0, the series diverges.

Quick Example: Interval of Convergence

We find the interval of convergence for the series βˆ‘n=1∞xnn\sum_{n=1}^{\infty} \frac{x^n}{n}.

Step 1: Find the radius of convergence using the Ratio Test.
> cn=1nc_n = \frac{1}{n}
>

L=lim⁑nβ†’βˆžβˆ£1/(n+1)1/n∣=lim⁑nβ†’βˆžnn+1=1L = \lim_{n \to \infty} \left| \frac{1/(n+1)}{1/n} \right| = \lim_{n \to \infty} \frac{n}{n+1} = 1

>
R=1L=1R = \frac{1}{L} = 1

Step 2: Determine the interval of absolute convergence.
Since a=0a=0 and R=1R=1, the series converges absolutely on (βˆ’1,1)(-1, 1).

Step 3: Test the endpoints.
* At x=1x=1: The series becomes βˆ‘n=1∞1nn=βˆ‘n=1∞1n\sum_{n=1}^{\infty} \frac{1^n}{n} = \sum_{n=1}^{\infty} \frac{1}{n}. This is the harmonic series (a p-series with p=1p=1), which diverges.
* At x=βˆ’1x=-1: The series becomes βˆ‘n=1∞(βˆ’1)nn\sum_{n=1}^{\infty} \frac{(-1)^n}{n}. This is an alternating series.
* bn=1nb_n = \frac{1}{n} is positive.
* bnb_n is decreasing.
* lim⁑nβ†’βˆž1n=0\lim_{n \to \infty} \frac{1}{n} = 0.
By the Alternating Series Test, this series converges.

Step 4: Combine results for the interval of convergence.
The series converges on [βˆ’1,1)[-1, 1).

Answer: The interval of convergence is [βˆ’1,1)[-1, 1).

:::question type="MCQ" question="The series βˆ‘n=1∞xnnβ‹…2n\sum_{n=1}^{\infty} \frac{x^n}{n \cdot 2^n} is convergent in the interval:" options=["[βˆ’2,2)[-2, 2)","(0,2](0, 2]","(0,2)(0, 2)","(βˆ’βˆž,∞)(-\infty, \infty)"] answer="[βˆ’2,2)[-2, 2)" hint="First find the radius of convergence using the Ratio Test, then check the endpoints carefully." solution="Step 1: Find the radius of convergence.
> cn=1nβ‹…2nc_n = \frac{1}{n \cdot 2^n}
>

L=lim⁑nβ†’βˆžβˆ£1/((n+1)2n+1)1/(nβ‹…2n)∣=lim⁑nβ†’βˆžβˆ£nβ‹…2n(n+1)2n+1∣=lim⁑nβ†’βˆžn2(n+1)=12\begin{aligned} L & = \lim_{n \to \infty} \left| \frac{1/((n+1)2^{n+1})}{1/(n \cdot 2^n)} \right| \\ & = \lim_{n \to \infty} \left| \frac{n \cdot 2^n}{(n+1)2^{n+1}} \right| \\ & = \lim_{n \to \infty} \frac{n}{2(n+1)} \\ & = \frac{1}{2} \end{aligned}

>
R=1L=2R = \frac{1}{L} = 2

Step 2: Determine the interval of absolute convergence.
Since a=0a=0 and R=2R=2, the series converges absolutely on (βˆ’2,2)(-2, 2).

Step 3: Test the endpoints.
* At x=2x=2: The series becomes βˆ‘n=1∞2nnβ‹…2n=βˆ‘n=1∞1n\sum_{n=1}^{\infty} \frac{2^n}{n \cdot 2^n} = \sum_{n=1}^{\infty} \frac{1}{n}. This is the harmonic series (a p-series with p=1p=1), which diverges.
* At x=βˆ’2x=-2: The series becomes βˆ‘n=1∞(βˆ’2)nnβ‹…2n=βˆ‘n=1∞(βˆ’1)n2nnβ‹…2n=βˆ‘n=1∞(βˆ’1)nn\sum_{n=1}^{\infty} \frac{(-2)^n}{n \cdot 2^n} = \sum_{n=1}^{\infty} \frac{(-1)^n 2^n}{n \cdot 2^n} = \sum_{n=1}^{\infty} \frac{(-1)^n}{n}. This is the alternating harmonic series, which converges by the Alternating Series Test.

Step 4: Combine results for the interval of convergence.
The series converges on [βˆ’2,2)[-2, 2). The interval is [βˆ’2,2)[-2, 2).
Answer: \boxed{[-2, 2)}
"
:::

4. Differentiation and Integration of Power Series

Within its interval of convergence, a power series can be differentiated and integrated term by term. The radius of convergence remains unchanged, though the interval of convergence may change at the endpoints.

πŸ“ Term-by-Term Differentiation

If f(x)=βˆ‘n=0∞cn(xβˆ’a)nf(x) = \sum_{n=0}^{\infty} c_n (x-a)^n has radius of convergence R>0R > 0, then:

fβ€²(x)=βˆ‘n=1∞ncn(xβˆ’a)nβˆ’1f'(x) = \sum_{n=1}^{\infty} n c_n (x-a)^{n-1}

The radius of convergence for fβ€²(x)f'(x) is also RR.

πŸ“ Term-by-Term Integration

If f(x)=βˆ‘n=0∞cn(xβˆ’a)nf(x) = \sum_{n=0}^{\infty} c_n (x-a)^n has radius of convergence R>0R > 0, then:

∫f(x) dx=C+βˆ‘n=0∞cnn+1(xβˆ’a)n+1\int f(x) \, dx = C + \sum_{n=0}^{\infty} \frac{c_n}{n+1} (x-a)^{n+1}

The radius of convergence for ∫f(x) dx\int f(x) \, dx is also RR.

Quick Example: Differentiation of Power Series

Consider the geometric series βˆ‘n=0∞xn=11βˆ’x\sum_{n=0}^{\infty} x^n = \frac{1}{1-x} for ∣x∣<1|x|<1. We find the power series for 1(1βˆ’x)2\frac{1}{(1-x)^2}.

Step 1: Recall the known power series for 11βˆ’x\frac{1}{1-x}.
>

11βˆ’x=βˆ‘n=0∞xn=1+x+x2+x3+…\frac{1}{1-x} = \sum_{n=0}^{\infty} x^n = 1 + x + x^2 + x^3 + \dots

Step 2: Differentiate both sides with respect to xx.
>

ddx(11βˆ’x)=ddx(βˆ‘n=0∞xn)\frac{d}{dx} \left( \frac{1}{1-x} \right) = \frac{d}{dx} \left( \sum_{n=0}^{\infty} x^n \right)

>
1(1βˆ’x)2=βˆ‘n=1∞nxnβˆ’1\frac{1}{(1-x)^2} = \sum_{n=1}^{\infty} n x^{n-1}

Step 3: Adjust the index for standard form (optional, but good practice).
Let k=nβˆ’1k = n-1, so n=k+1n=k+1. When n=1n=1, k=0k=0.
>

1(1βˆ’x)2=βˆ‘k=0∞(k+1)xk\frac{1}{(1-x)^2} = \sum_{k=0}^{\infty} (k+1) x^k

or, using nn as the index again:
>
1(1βˆ’x)2=βˆ‘n=0∞(n+1)xn=1+2x+3x2+4x3+…\frac{1}{(1-x)^2} = \sum_{n=0}^{\infty} (n+1) x^n = 1 + 2x + 3x^2 + 4x^3 + \dots

Answer: The power series for 1(1βˆ’x)2\frac{1}{(1-x)^2} is βˆ‘n=0∞(n+1)xn\sum_{n=0}^{\infty} (n+1) x^n. Its radius of convergence is R=1R=1, same as the original series.

:::question type="MCQ" question="The power series representation for ln⁑(1βˆ’x)\ln(1-x) for ∣x∣<1|x|<1 is:" options=["βˆ‘n=0∞xn+1n+1\sum_{n=0}^{\infty} \frac{x^{n+1}}{n+1}","βˆ‘n=1∞xnn\sum_{n=1}^{\infty} \frac{x^n}{n}","βˆ’βˆ‘n=0∞xn+1n+1-\sum_{n=0}^{\infty} \frac{x^{n+1}}{n+1}","βˆ’βˆ‘n=1∞xnn-\sum_{n=1}^{\infty} \frac{x^n}{n}"] answer="βˆ’βˆ‘n=1∞xnn-\sum_{n=1}^{\infty} \frac{x^n}{n}" hint="Consider the integral of the geometric series 11βˆ’x\frac{1}{1-x}." solution="Step 1: Recall the geometric series.
>

11βˆ’x=βˆ‘n=0∞xnfor ∣x∣<1\frac{1}{1-x} = \sum_{n=0}^{\infty} x^n \quad \text{for } |x|<1

Step 2: Integrate both sides from 00 to xx.
>

∫0x11βˆ’tdt=∫0x(βˆ‘n=0∞tn)dt\int_0^x \frac{1}{1-t} dt = \int_0^x \left( \sum_{n=0}^{\infty} t^n \right) dt

>
[βˆ’ln⁑(1βˆ’t)]0x=βˆ‘n=0∞∫0xtndt[-\ln(1-t)]_0^x = \sum_{n=0}^{\infty} \int_0^x t^n dt

>
βˆ’ln⁑(1βˆ’x)βˆ’(βˆ’ln⁑(1βˆ’0))=βˆ‘n=0∞[tn+1n+1]0x-\ln(1-x) - (-\ln(1-0)) = \sum_{n=0}^{\infty} \left[ \frac{t^{n+1}}{n+1} \right]_0^x

Step 3: Express ln⁑(1βˆ’x)\ln(1-x) and adjust index.
>

ln⁑(1βˆ’x)=βˆ’βˆ‘n=0∞xn+1n+1\ln(1-x) = -\sum_{n=0}^{\infty} \frac{x^{n+1}}{n+1}

Let k=n+1k=n+1. When n=0n=0, k=1k=1.
>
ln⁑(1βˆ’x)=βˆ’βˆ‘k=1∞xkk\ln(1-x) = -\sum_{k=1}^{\infty} \frac{x^k}{k}

Using nn as the index again:
>
ln⁑(1βˆ’x)=βˆ’βˆ‘n=1∞xnn\ln(1-x) = -\sum_{n=1}^{\infty} \frac{x^n}{n}

Answer: \boxed{βˆ’βˆ‘n=1∞xnn-\sum_{n=1}^{\infty} \frac{x^n}{n}}
"
:::

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Advanced Applications

Combining the techniques for radius and interval of convergence allows us to analyze more complex series. We observe that careful application of convergence tests at endpoints is crucial.

Worked Example:

We determine the interval of convergence for the series βˆ‘n=1∞(xβˆ’3)nnβ‹…4n\sum_{n=1}^{\infty} \frac{(x-3)^n}{n \cdot 4^n}.

Step 1: Find the radius of convergence.
The series is centered at a=3a=3. cn=1nβ‹…4nc_n = \frac{1}{n \cdot 4^n}.
>

L=lim⁑nβ†’βˆžβˆ£1/((n+1)4n+1)1/(nβ‹…4n)∣=lim⁑nβ†’βˆžβˆ£nβ‹…4n(n+1)4n+1∣=lim⁑nβ†’βˆžn4(n+1)=14\begin{aligned} L & = \lim_{n \to \infty} \left| \frac{1/((n+1)4^{n+1})}{1/(n \cdot 4^n)} \right| \\ & = \lim_{n \to \infty} \left| \frac{n \cdot 4^n}{(n+1)4^{n+1}} \right| \\ & = \lim_{n \to \infty} \frac{n}{4(n+1)} \\ & = \frac{1}{4} \end{aligned}

>
R=1L=4R = \frac{1}{L} = 4

Step 2: Determine the interval of absolute convergence.
With a=3a=3 and R=4R=4, the series converges absolutely for ∣xβˆ’3∣<4|x-3| < 4.
>

βˆ’4<xβˆ’3<4-4 < x-3 < 4

>
βˆ’1<x<7-1 < x < 7

The interval of absolute convergence is (βˆ’1,7)(-1, 7).

Step 3: Test the endpoints.
* At x=3βˆ’R=3βˆ’4=βˆ’1x = 3-R = 3-4 = -1:
The series becomes βˆ‘n=1∞(βˆ’1βˆ’3)nnβ‹…4n=βˆ‘n=1∞(βˆ’4)nnβ‹…4n=βˆ‘n=1∞(βˆ’1)n4nnβ‹…4n=βˆ‘n=1∞(βˆ’1)nn\sum_{n=1}^{\infty} \frac{(-1-3)^n}{n \cdot 4^n} = \sum_{n=1}^{\infty} \frac{(-4)^n}{n \cdot 4^n} = \sum_{n=1}^{\infty} \frac{(-1)^n 4^n}{n \cdot 4^n} = \sum_{n=1}^{\infty} \frac{(-1)^n}{n}.
This is the alternating harmonic series, which converges by the Alternating Series Test.
* At x=3+R=3+4=7x = 3+R = 3+4 = 7:
The series becomes βˆ‘n=1∞(7βˆ’3)nnβ‹…4n=βˆ‘n=1∞4nnβ‹…4n=βˆ‘n=1∞1n\sum_{n=1}^{\infty} \frac{(7-3)^n}{n \cdot 4^n} = \sum_{n=1}^{\infty} \frac{4^n}{n \cdot 4^n} = \sum_{n=1}^{\infty} \frac{1}{n}.
This is the harmonic series (p-series with p=1p=1), which diverges.

Step 4: Combine results for the interval of convergence.
The series converges on [βˆ’1,7)[-1, 7).

Answer: The interval of convergence is [βˆ’1,7)[-1, 7).

:::question type="NAT" question="The series βˆ‘n=1∞(x+1)nn2\sum_{n=1}^{\infty} \frac{(x+1)^n}{n^2} has an interval of convergence [A,B][A, B]. What is the value of A+BA+B?" answer="βˆ’2-2" hint="Find the radius of convergence, then check the endpoints. The interval of convergence will be closed at both ends." solution="Step 1: Find the radius of convergence.
The series is centered at a=βˆ’1a=-1. cn=1n2c_n = \frac{1}{n^2}.
>

L=lim⁑nβ†’βˆžβˆ£1/(n+1)21/n2∣=lim⁑nβ†’βˆžβˆ£n2(n+1)2∣=lim⁑nβ†’βˆž(nn+1)2=12=1\begin{aligned} L & = \lim_{n \to \infty} \left| \frac{1/(n+1)^2}{1/n^2} \right| \\ & = \lim_{n \to \infty} \left| \frac{n^2}{(n+1)^2} \right| \\ & = \lim_{n \to \infty} \left( \frac{n}{n+1} \right)^2 \\ & = 1^2 = 1 \end{aligned}

>
R=1L=1R = \frac{1}{L} = 1

Step 2: Determine the interval of absolute convergence.
With a=βˆ’1a=-1 and R=1R=1, the series converges absolutely for ∣xβˆ’(βˆ’1)∣<1|x-(-1)| < 1, i.e., ∣x+1∣<1|x+1| < 1.
>

βˆ’1<x+1<1-1 < x+1 < 1

>
βˆ’2<x<0-2 < x < 0

The interval of absolute convergence is (βˆ’2,0)(-2, 0).

Step 3: Test the endpoints.
* At x=βˆ’1βˆ’R=βˆ’1βˆ’1=βˆ’2x = -1-R = -1-1 = -2:
The series becomes βˆ‘n=1∞(βˆ’2+1)nn2=βˆ‘n=1∞(βˆ’1)nn2\sum_{n=1}^{\infty} \frac{(-2+1)^n}{n^2} = \sum_{n=1}^{\infty} \frac{(-1)^n}{n^2}.
Consider the absolute values: βˆ‘n=1∞∣(βˆ’1)nn2∣=βˆ‘n=1∞1n2\sum_{n=1}^{\infty} \left| \frac{(-1)^n}{n^2} \right| = \sum_{n=1}^{\infty} \frac{1}{n^2}. This is a p-series with p=2>1p=2 > 1, which converges. Since the series of absolute values converges, the original series converges absolutely at x=βˆ’2x=-2.
* At x=βˆ’1+R=βˆ’1+1=0x = -1+R = -1+1 = 0:
The series becomes βˆ‘n=1∞(0+1)nn2=βˆ‘n=1∞1n2\sum_{n=1}^{\infty} \frac{(0+1)^n}{n^2} = \sum_{n=1}^{\infty} \frac{1}{n^2}.
This is a p-series with p=2>1p=2 > 1, which converges.

Step 4: Combine results for the interval of convergence.
The series converges on [βˆ’2,0][-2, 0].
Thus, A=βˆ’2A = -2 and B=0B = 0.
A+B=βˆ’2+0=βˆ’2A+B = -2+0 = -2.
Answer: \boxed{-2}
"
:::

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Problem-Solving Strategies

πŸ’‘ CUET PG Strategy

When encountering power series problems:

  • Identify the center (aa) and coefficients (cnc_n). This sets up the problem correctly.

  • Choose the appropriate test for RR. Use the Ratio Test for factorials or products. Use the Root Test for nn-th powers. If neither applies cleanly, revert to the definition of RR via the limit superior or other series tests.

  • Calculate RR carefully. Algebraic simplification is key, especially with limits involving nβ†’βˆžn \to \infty.

  • Determine the open interval (aβˆ’R,a+R)(a-R, a+R). This gives the region of absolute convergence.

  • Critically examine the endpoints. Substitute x=aβˆ’Rx=a-R and x=a+Rx=a+R into the series and apply standard convergence tests for series of constants. This is often where students make errors.

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Common Mistakes

⚠️ Watch Out

❌ Students often forget to test the endpoints of the interval of convergence.
βœ… Always substitute the endpoint values into the original series and apply a suitable convergence test (e.g., p-series, Alternating Series Test, Comparison Test).

❌ Incorrectly applying the Ratio or Root Test, especially with complex expressions for cnc_n.
βœ… Ensure all algebraic simplifications are correct, particularly when dealing with n+1n+1 terms and limits. Remember lim⁑nβ†’βˆž(1+k/n)n=ek\lim_{n \to \infty} (1+k/n)^n = e^k.

❌ Confusing radius of convergence with interval of convergence.
βœ… RR is a single non-negative number. The interval is a set of xx values, which may be open, closed, or half-open.

❌ Misinterpreting the result of the Ratio/Root Test when L=0L=0 or L=∞L=\infty.
βœ… L=0β€…β€ŠβŸΉβ€…β€ŠR=∞L=0 \implies R=\infty (converges everywhere). L=βˆžβ€…β€ŠβŸΉβ€…β€ŠR=0L=\infty \implies R=0 (converges only at center).

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Practice Questions

:::question type="MCQ" question="The radius of convergence of the power series βˆ‘n=0∞nnn!xn\sum_{n=0}^{\infty} \frac{n^n}{n!} x^n is:" options=["ee","1/e1/e","11","∞\infty"] answer="1/e1/e" hint="Use the Ratio Test. Recall that lim⁑nβ†’βˆž(1+1/n)n=e\lim_{n \to \infty} (1 + 1/n)^n = e." solution="Step 1: Identify cnc_n.
>

cn=nnn!c_n = \frac{n^n}{n!}

Step 2: Compute L=lim⁑nβ†’βˆžβˆ£cn+1cn∣L = \lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right|.
>

L=lim⁑nβ†’βˆžβˆ£(n+1)n+1/(n+1)!nn/n!∣=lim⁑nβ†’βˆžβˆ£(n+1)n+1(n+1)!β‹…n!nn∣=lim⁑nβ†’βˆžβˆ£(n+1)n+1(n+1)n!β‹…n!nn∣=lim⁑nβ†’βˆžβˆ£(n+1)nnn∣=lim⁑nβ†’βˆž(n+1n)n=lim⁑nβ†’βˆž(1+1n)n=e\begin{aligned} L & = \lim_{n \to \infty} \left| \frac{(n+1)^{n+1}/(n+1)!}{n^n/n!} \right| \\ & = \lim_{n \to \infty} \left| \frac{(n+1)^{n+1}}{(n+1)!} \cdot \frac{n!}{n^n} \right| \\ & = \lim_{n \to \infty} \left| \frac{(n+1)^{n+1}}{(n+1)n!} \cdot \frac{n!}{n^n} \right| \\ & = \lim_{n \to \infty} \left| \frac{(n+1)^n}{n^n} \right| \\ & = \lim_{n \to \infty} \left( \frac{n+1}{n} \right)^n \\ & = \lim_{n \to \infty} \left( 1 + \frac{1}{n} \right)^n \\ & = e \end{aligned}

Step 3: Calculate R=1LR = \frac{1}{L}.
>

R=1eR = \frac{1}{e}

Answer: \boxed{1/e}"
:::

:::question type="MCQ" question="The interval of convergence for the series βˆ‘n=1∞(xβˆ’5)nnln⁑n\sum_{n=1}^{\infty} \frac{(x-5)^n}{n \ln n} is:" options=["[4,6)[4, 6)","(4,6](4, 6]","(4,6)(4, 6)","[4,6][4, 6]"] answer="[4,6)[4, 6)" hint="Find R using the Ratio Test, then test endpoints. For x=4x=4, use the Alternating Series Test. For x=6x=6, use the Integral Test or Comparison Test with a known divergent series." solution="Step 1: Find the radius of convergence.
The series is centered at a=5a=5. cn=1nln⁑nc_n = \frac{1}{n \ln n}.
>

L=lim⁑nβ†’βˆžβˆ£1/((n+1)ln⁑(n+1))1/(nln⁑n)∣=lim⁑nβ†’βˆžβˆ£nln⁑n(n+1)ln⁑(n+1)∣=lim⁑nβ†’βˆž(nn+1)(ln⁑nln⁑(n+1))=1β‹…lim⁑nβ†’βˆž1/n1/(n+1)(L’Hopital’sΒ RuleΒ forΒ ln⁑n/ln⁑(n+1))=1β‹…lim⁑nβ†’βˆžn+1n=1\begin{aligned} L & = \lim_{n \to \infty} \left| \frac{1/((n+1)\ln(n+1))}{1/(n \ln n)} \right| \\ & = \lim_{n \to \infty} \left| \frac{n \ln n}{(n+1)\ln(n+1)} \right| \\ & = \lim_{n \to \infty} \left( \frac{n}{n+1} \right) \left( \frac{\ln n}{\ln(n+1)} \right) \\ & = 1 \cdot \lim_{n \to \infty} \frac{1/n}{1/(n+1)} \quad \text{(L'Hopital's Rule for } \ln n / \ln(n+1) \text{)} \\ & = 1 \cdot \lim_{n \to \infty} \frac{n+1}{n} \\ & = 1 \end{aligned}

>
R=1L=1R = \frac{1}{L} = 1

Step 2: Determine the interval of absolute convergence.
With a=5a=5 and R=1R=1, the series converges absolutely for ∣xβˆ’5∣<1|x-5| < 1.
>

βˆ’1<xβˆ’5<1-1 < x-5 < 1

>
4<x<64 < x < 6

The interval of absolute convergence is (4,6)(4, 6).

Step 3: Test the endpoints.
* At x=4x = 4: The series becomes
>

βˆ‘n=1∞(4βˆ’5)nnln⁑n=βˆ‘n=1∞(βˆ’1)nnln⁑n\sum_{n=1}^{\infty} \frac{(4-5)^n}{n \ln n} = \sum_{n=1}^{\infty} \frac{(-1)^n}{n \ln n}

This is an alternating series. Let bn=1nln⁑nb_n = \frac{1}{n \ln n}.
1. bn>0b_n > 0 for nβ‰₯2n \ge 2.
2. bnb_n is decreasing for nβ‰₯2n \ge 2.
3. lim⁑nβ†’βˆž1nln⁑n=0\lim_{n \to \infty} \frac{1}{n \ln n} = 0.
By the Alternating Series Test, the series converges at x=4x=4.
* At x=6x = 6: The series becomes
>
βˆ‘n=1∞(6βˆ’5)nnln⁑n=βˆ‘n=1∞1nln⁑n\sum_{n=1}^{\infty} \frac{(6-5)^n}{n \ln n} = \sum_{n=1}^{\infty} \frac{1}{n \ln n}

We use the Integral Test. Let f(x)=1xln⁑xf(x) = \frac{1}{x \ln x}. This function is positive, continuous, and decreasing for xβ‰₯2x \ge 2.
>
∫2∞1xln⁑xdx=lim⁑bβ†’βˆž[ln⁑(ln⁑x)]2b=lim⁑bβ†’βˆž(ln⁑(ln⁑b)βˆ’ln⁑(ln⁑2))=∞\int_2^\infty \frac{1}{x \ln x} dx = \lim_{b \to \infty} [\ln(\ln x)]_2^b = \lim_{b \to \infty} (\ln(\ln b) - \ln(\ln 2)) = \infty

Since the integral diverges, the series diverges at x=6x=6.

Step 4: Combine results for the interval of convergence.
The series converges on [4,6)[4, 6).
Answer: \boxed{[4, 6)}"
:::

:::question type="NAT" question="If the series βˆ‘n=0∞(n!)k(kn)!xn\sum_{n=0}^{\infty} \frac{(n!)^k}{(kn)!} x^n has a radius of convergence RR, then for k=2k=2, RR is:" answer="4" hint="Apply the Ratio Test. Be careful with factorials." solution="Step 1: Identify cnc_n for k=2k=2.
>

cn=(n!)2(2n)!c_n = \frac{(n!)^2}{(2n)!}

Step 2: Compute L=lim⁑nβ†’βˆžβˆ£cn+1cn∣L = \lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right|.
>

L=lim⁑nβ†’βˆžβˆ£((n+1)!)2/(2(n+1))!(n!)2/(2n)!∣=lim⁑nβ†’βˆžβˆ£((n+1)!)2(2n+2)!β‹…(2n)!(n!)2∣=lim⁑nβ†’βˆž(n+1)2(n!)2(2n+2)(2n+1)(2n)!β‹…(2n)!(n!)2=lim⁑nβ†’βˆž(n+1)2(2n+2)(2n+1)=lim⁑nβ†’βˆžn2+2n+14n2+6n+2=lim⁑nβ†’βˆž1+2/n+1/n24+6/n+2/n2=14\begin{aligned} L & = \lim_{n \to \infty} \left| \frac{((n+1)!)^2 / (2(n+1))!}{(n!)^2 / (2n)!} \right| \\ & = \lim_{n \to \infty} \left| \frac{((n+1)!)^2}{(2n+2)!} \cdot \frac{(2n)!}{(n!)^2} \right| \\ & = \lim_{n \to \infty} \frac{(n+1)^2 (n!)^2}{(2n+2)(2n+1)(2n)!} \cdot \frac{(2n)!}{(n!)^2} \\ & = \lim_{n \to \infty} \frac{(n+1)^2}{(2n+2)(2n+1)} \\ & = \lim_{n \to \infty} \frac{n^2+2n+1}{4n^2+6n+2} \\ & = \lim_{n \to \infty} \frac{1+2/n+1/n^2}{4+6/n+2/n^2} \\ & = \frac{1}{4} \end{aligned}

Step 3: Calculate R=1LR = \frac{1}{L}.
>

R=11/4=4R = \frac{1}{1/4} = 4

Answer: \boxed{4}"
:::

:::question type="MSQ" question="Which of the following statements about the power series βˆ‘n=1∞(βˆ’1)nn(xβˆ’1)n\sum_{n=1}^{\infty} \frac{(-1)^n}{n} (x-1)^n are correct?" options=["The radius of convergence is 11.","The series converges at x=0x=0.","The series converges at x=2x=2.","The interval of convergence is (0,2)(0, 2)."] answer="The radius of convergence is 11,The series converges at x=2x=2" hint="First find R. Then test endpoints x=0x=0 and x=2x=2." solution="Step 1: Find the radius of convergence.
The series is centered at a=1a=1. cn=(βˆ’1)nnc_n = \frac{(-1)^n}{n}.
>

L=lim⁑nβ†’βˆžβˆ£cn+1cn∣=lim⁑nβ†’βˆžβˆ£(βˆ’1)n+1/(n+1)(βˆ’1)n/n∣=lim⁑nβ†’βˆžβˆ£nn+1β‹…(βˆ’1)n+1(βˆ’1)n∣=lim⁑nβ†’βˆžβˆ£nn+1β‹…(βˆ’1)∣=lim⁑nβ†’βˆžnn+1=1\begin{aligned} L & = \lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right| \\ & = \lim_{n \to \infty} \left| \frac{(-1)^{n+1}/(n+1)}{(-1)^n/n} \right| \\ & = \lim_{n \to \infty} \left| \frac{n}{n+1} \cdot \frac{(-1)^{n+1}}{(-1)^n} \right| \\ & = \lim_{n \to \infty} \left| \frac{n}{n+1} \cdot (-1) \right| \\ & = \lim_{n \to \infty} \frac{n}{n+1} \\ & = 1 \end{aligned}

>
R=1L=1R = \frac{1}{L} = 1

Thus, Statement 1: 'The radius of convergence is 11' is correct.

Step 2: Determine the interval of absolute convergence.
With a=1a=1 and R=1R=1, the series converges absolutely for ∣xβˆ’1∣<1|x-1| < 1, which means 0<x<20 < x < 2.

Step 3: Test the endpoints.
* At x=0x=0: Substitute x=0x=0 into the series:
>

βˆ‘n=1∞(βˆ’1)nn(0βˆ’1)n=βˆ‘n=1∞(βˆ’1)nn(βˆ’1)n=βˆ‘n=1∞(βˆ’1)2nn=βˆ‘n=1∞1n\sum_{n=1}^{\infty} \frac{(-1)^n}{n} (0-1)^n = \sum_{n=1}^{\infty} \frac{(-1)^n}{n} (-1)^n = \sum_{n=1}^{\infty} \frac{(-1)^{2n}}{n} = \sum_{n=1}^{\infty} \frac{1}{n}

This is the harmonic series, which diverges.
Thus, Statement 2: 'The series converges at x=0x=0' is incorrect.
* At x=2x=2: Substitute x=2x=2 into the series:
>
βˆ‘n=1∞(βˆ’1)nn(2βˆ’1)n=βˆ‘n=1∞(βˆ’1)nn(1)n=βˆ‘n=1∞(βˆ’1)nn\sum_{n=1}^{\infty} \frac{(-1)^n}{n} (2-1)^n = \sum_{n=1}^{\infty} \frac{(-1)^n}{n} (1)^n = \sum_{n=1}^{\infty} \frac{(-1)^n}{n}

This is the alternating harmonic series. It satisfies the conditions of the Alternating Series Test (bn=1/nb_n = 1/n is positive, decreasing, and lim⁑nβ†’βˆž1/n=0\lim_{n \to \infty} 1/n = 0). Therefore, this series converges.
Thus, Statement 3: 'The series converges at x=2x=2' is correct.

Step 4: Determine the full interval of convergence.
The series converges for x∈(0,2]x \in (0, 2] (from step 2 and endpoint tests).
Thus, Statement 4: 'The interval of convergence is (0,2)(0, 2)' is incorrect.

Answer: \boxed{\text{The radius of convergence is } 1 \text{, The series converges at } x=2}}"
:::

:::question type="MCQ" question="The series βˆ‘n=0∞x2n2n\sum_{n=0}^{\infty} \frac{x^{2n}}{2^n} has an interval of convergence:" options=["(βˆ’2,2)(-2, 2)","(βˆ’2,2)(-\sqrt{2}, \sqrt{2})","(βˆ’βˆž,∞)(-\infty, \infty)","(βˆ’1,1)(-1, 1)"] answer="(βˆ’2,2)(-\sqrt{2}, \sqrt{2})" hint="Treat y=x2y=x^2 and find the convergence for yy. Or apply the Ratio Test carefully to x2nx^{2n}." solution="Method 1: Using Ratio Test for x2nx^{2n}
Step 1: Identify cnc_n for the term xnx^n. Here, the series is βˆ‘n=0∞cnxn\sum_{n=0}^{\infty} c_n x^n where cn=0c_n = 0 for odd nn, and cn=1/2n/2c_n = 1/2^{n/2} for even nn. This makes the standard Ratio/Root Test slightly awkward.

Instead, we apply the Ratio Test to the form βˆ‘n=0∞an\sum_{n=0}^{\infty} a_n, where an=x2n2na_n = \frac{x^{2n}}{2^n}.
>

Lβ€²=lim⁑nβ†’βˆžβˆ£an+1an∣=lim⁑nβ†’βˆžβˆ£x2(n+1)/2n+1x2n/2n∣=lim⁑nβ†’βˆžβˆ£x2n+22n+1β‹…2nx2n∣=lim⁑nβ†’βˆžβˆ£x22∣=∣x2∣2\begin{aligned} L' & = \lim_{n \to \infty} \left| \frac{a_{n+1}}{a_n} \right| \\ & = \lim_{n \to \infty} \left| \frac{x^{2(n+1)}/2^{n+1}}{x^{2n}/2^n} \right| \\ & = \lim_{n \to \infty} \left| \frac{x^{2n+2}}{2^{n+1}} \cdot \frac{2^n}{x^{2n}} \right| \\ & = \lim_{n \to \infty} \left| \frac{x^2}{2} \right| \\ & = \frac{|x^2|}{2} \end{aligned}

For convergence, we require Lβ€²<1L' < 1.
>
∣x2∣2<1\frac{|x^2|}{2} < 1

>
∣x2∣<2|x^2| < 2

>
x2<2x^2 < 2

>
βˆ’2<x<2-\sqrt{2} < x < \sqrt{2}

Step 2: Test endpoints.
* At x=2x = \sqrt{2}: The series becomes
>

βˆ‘n=0∞(2)2n2n=βˆ‘n=0∞2n2n=βˆ‘n=0∞1\sum_{n=0}^{\infty} \frac{(\sqrt{2})^{2n}}{2^n} = \sum_{n=0}^{\infty} \frac{2^n}{2^n} = \sum_{n=0}^{\infty} 1

This series diverges.
* At x=βˆ’2x = -\sqrt{2}: The series becomes
>
βˆ‘n=0∞(βˆ’2)2n2n=βˆ‘n=0∞(2)2n2n=βˆ‘n=0∞1\sum_{n=0}^{\infty} \frac{(-\sqrt{2})^{2n}}{2^n} = \sum_{n=0}^{\infty} \frac{(\sqrt{2})^{2n}}{2^n} = \sum_{n=0}^{\infty} 1

This series diverges.

Step 3: Combine results.
The interval of convergence is (βˆ’2,2)(-\sqrt{2}, \sqrt{2}).

Method 2: Substitution
Let y=x2y = x^2. The series becomes βˆ‘n=0∞yn2n=βˆ‘n=0∞(y2)n\sum_{n=0}^{\infty} \frac{y^n}{2^n} = \sum_{n=0}^{\infty} \left(\frac{y}{2}\right)^n.
This is a geometric series with ratio r=y/2r = y/2. It converges if ∣r∣<1|r| < 1.
>

∣y2∣<1\left|\frac{y}{2}\right| < 1

>
∣y∣<2|y| < 2

Substitute back y=x2y=x^2:
>
∣x2∣<2|x^2| < 2

>
x2<2x^2 < 2

>
βˆ’2<x<2-\sqrt{2} < x < \sqrt{2}

At the endpoints x=Β±2x=\pm\sqrt{2}, y=x2=2y=x^2=2. The series becomes βˆ‘n=0∞(2/2)n=βˆ‘n=0∞1\sum_{n=0}^{\infty} (2/2)^n = \sum_{n=0}^{\infty} 1, which diverges.
The interval of convergence is (βˆ’2,2)(-\sqrt{2}, \sqrt{2}).
Answer: \boxed{(-\sqrt{2}, \sqrt{2})}"
:::

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Summary

❗ Key Formulas & Takeaways

| # | Formula/Concept | Expression |
|---|----------------|------------|
| 1 | Power Series | βˆ‘n=0∞cn(xβˆ’a)n\sum_{n=0}^{\infty} c_n (x-a)^n |
| 2 | Radius of Conv. (Ratio Test) |

R=1/lim⁑nβ†’βˆžβˆ£cn+1cn∣R = 1 / \lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right|
|
| 3 | Radius of Conv. (Root Test) |
R=1/lim⁑nβ†’βˆžβˆ£cn∣nR = 1 / \lim_{n \to \infty} \sqrt[n]{|c_n|}
|
| 4 | Interval of Convergence | Determined by RR and endpoint tests at aΒ±Ra \pm R |
| 5 | Term-by-Term Differentiation |
ddxβˆ‘cn(xβˆ’a)n=βˆ‘ncn(xβˆ’a)nβˆ’1\frac{d}{dx} \sum c_n (x-a)^n = \sum n c_n (x-a)^{n-1}
(same RR) |
| 6 | Term-by-Term Integration |
βˆ«βˆ‘cn(xβˆ’a)ndx=C+βˆ‘cnn+1(xβˆ’a)n+1\int \sum c_n (x-a)^n dx = C + \sum \frac{c_n}{n+1} (x-a)^{n+1}
(same RR) |

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What's Next?

πŸ’‘ Continue Learning

This topic connects to:

    • Taylor and Maclaurin Series: Power series are the foundation for these function representations, crucial for approximations and solving differential equations.

    • Fourier Series: While distinct, Fourier series also represent functions as infinite sums (of sines and cosines), extending the idea of infinite series representations to periodic functions.

    • Complex Analysis: The concept of power series extends naturally to complex variables, forming the basis for analytic functions and complex differentiation.

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πŸ’‘ Next Up

Proceeding to Properties of Power Series.

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Part 2: Properties of Power Series

Power series are fundamental in real analysis, providing a means to represent functions as infinite sums of powers. We utilize them for function approximation, solving differential equations, and evaluating integrals, making them a recurring topic in competitive examinations.

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Core Concepts

1. Definition of a Power Series

A power series is an infinite series of the form βˆ‘n=0∞cn(xβˆ’a)n\sum_{n=0}^{\infty} c_n (x-a)^n, where aa is the center of the series, xx is a variable, and cnc_n are constants known as the coefficients. When a=0a=0, the series is a Maclaurin series.

πŸ“– Power Series

A power series centered at aa is an expression of the form βˆ‘n=0∞cn(xβˆ’a)n=c0+c1(xβˆ’a)+c2(xβˆ’a)2+…\sum_{n=0}^{\infty} c_n (x-a)^n = c_0 + c_1(x-a) + c_2(x-a)^2 + \dots.

Quick Example:

Consider the power series βˆ‘n=0∞xnn!\sum_{n=0}^{\infty} \frac{x^n}{n!}.

Step 1: Identify the center and coefficients.

> The series is centered at a=0a=0.
>
> The coefficients are cn=1n!c_n = \frac{1}{n!}.

Step 2: Write out the first few terms.

>

c0+c1x+c2x2+c3x3+…=10!+11!x+12!x2+13!x3+…=1+x+x22+x36+…\begin{aligned}c_0 + c_1 x + c_2 x^2 + c_3 x^3 + \dots & = \frac{1}{0!} + \frac{1}{1!}x + \frac{1}{2!}x^2 + \frac{1}{3!}x^3 + \dots \\
& = 1 + x + \frac{x^2}{2} + \frac{x^3}{6} + \dots\end{aligned}

:::question type="MCQ" question="Which of the following is a power series centered at x=2x=2?" options=["βˆ‘n=0∞n!xn\sum_{n=0}^{\infty} n! x^n","βˆ‘n=0∞(xβˆ’2)nn\sum_{n=0}^{\infty} \frac{(x-2)^n}{n}","βˆ‘n=0∞xn2n\sum_{n=0}^{\infty} \frac{x^n}{2^n}","βˆ‘n=0∞(x+2)n\sum_{n=0}^{\infty} (x+2)^n"] answer="βˆ‘n=0∞(xβˆ’2)nn\sum_{n=0}^{\infty} \frac{(x-2)^n}{n}" hint="A power series centered at aa has the form βˆ‘cn(xβˆ’a)n\sum c_n (x-a)^n." solution="For a power series centered at aa, the term involving xx must be (xβˆ’a)(x-a). In this case, a=2a=2, so we look for (xβˆ’2)n(x-2)^n. Option B matches this form."
:::

---

2. Radius of Convergence (R)

The radius of convergence RR of a power series βˆ‘n=0∞cn(xβˆ’a)n\sum_{n=0}^{\infty} c_n (x-a)^n is a non-negative number (or ∞\infty) such that the series converges for ∣xβˆ’a∣<R|x-a| < R and diverges for ∣xβˆ’a∣>R|x-a| > R. The Ratio Test or Root Test are commonly employed to determine RR.

πŸ“ Ratio Test for Radius of Convergence

Let the power series be βˆ‘n=0∞cn(xβˆ’a)n\sum_{n=0}^{\infty} c_n (x-a)^n.
If L=lim⁑nβ†’βˆžβˆ£cn+1cn∣L = \lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right| exists, then:

    • If LL is a finite non-zero number, R=1LR = \frac{1}{L}.

    • If L=0L=0, then R=∞R=\infty.

    • If L=∞L=\infty, then R=0R=0.

Quick Example:

Determine the radius of convergence for the series βˆ‘n=1∞(xβˆ’3)nn\sum_{n=1}^{\infty} \frac{(x-3)^n}{n}.

Step 1: Identify cnc_n and aa.

> Here a=3a=3 and cn=1nc_n = \frac{1}{n}.

Step 2: Apply the Ratio Test.

> We calculate lim⁑nβ†’βˆžβˆ£cn+1cn∣\lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right|.
>
>

lim⁑nβ†’βˆžβˆ£1/(n+1)1/n∣=lim⁑nβ†’βˆžβˆ£nn+1∣=lim⁑nβ†’βˆž11+1/n=1\begin{aligned}\lim_{n \to \infty} \left| \frac{1/(n+1)}{1/n} \right| & = \lim_{n \to \infty} \left| \frac{n}{n+1} \right| \\
& = \lim_{n \to \infty} \frac{1}{1 + 1/n} = 1\end{aligned}

>
> Thus, L=1L=1.

Step 3: Determine RR.

> Since L=1L=1, R=1L=11=1R = \frac{1}{L} = \frac{1}{1} = 1.

Answer: The radius of convergence is R=1R=1.

:::question type="MCQ" question="Find the radius of convergence for the power series βˆ‘n=0∞n!2nxn\sum_{n=0}^{\infty} \frac{n!}{2^n} x^n." options=["00","11","22","∞\infty"] answer="00" hint="Use the Ratio Test. Pay attention to the limit value." solution="Step 1: Identify cnc_n.
> Here cn=n!2nc_n = \frac{n!}{2^n}.
>
> Step 2: Apply the Ratio Test.
>

lim⁑nβ†’βˆžβˆ£cn+1cn∣=lim⁑nβ†’βˆžβˆ£(n+1)!/2n+1n!/2n∣=lim⁑nβ†’βˆžβˆ£(n+1)!2n+1β‹…2nn!∣=lim⁑nβ†’βˆžβˆ£n+12∣=∞\begin{aligned}\lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right| & = \lim_{n \to \infty} \left| \frac{(n+1)!/2^{n+1}}{n!/2^n} \right| \\
& = \lim_{n \to \infty} \left| \frac{(n+1)!}{2^{n+1}} \cdot \frac{2^n}{n!} \right| \\
& = \lim_{n \to \infty} \left| \frac{n+1}{2} \right| = \infty\end{aligned}

>
> Step 3: Determine RR.
> Since L=∞L=\infty, the radius of convergence R=0R=0. The series only converges at its center x=0x=0."
:::

---

3. Interval of Convergence

The interval of convergence is the set of all xx values for which the power series converges. It is centered at aa and has length 2R2R. After finding RR, we must check the convergence at the endpoints x=aβˆ’Rx = a-R and x=a+Rx = a+R separately, as the Ratio Test is inconclusive at these points.

Quick Example:

Determine the interval of convergence for the series βˆ‘n=1∞(xβˆ’3)nn\sum_{n=1}^{\infty} \frac{(x-3)^n}{n}. (From previous example, R=1R=1 and a=3a=3).

Step 1: Establish the open interval of convergence.

> The series converges for ∣xβˆ’3∣<1|x-3| < 1, which means βˆ’1<xβˆ’3<1-1 < x-3 < 1.
> Adding 3 to all parts, we get 2<x<42 < x < 4.

Step 2: Check the left endpoint x=aβˆ’R=3βˆ’1=2x=a-R = 3-1=2.

> Substitute x=2x=2 into the series:
>

βˆ‘n=1∞(2βˆ’3)nn=βˆ‘n=1∞(βˆ’1)nn\sum_{n=1}^{\infty} \frac{(2-3)^n}{n} = \sum_{n=1}^{\infty} \frac{(-1)^n}{n}

> This is the alternating harmonic series, which converges by the Alternating Series Test.

Step 3: Check the right endpoint x=a+R=3+1=4x=a+R = 3+1=4.

> Substitute x=4x=4 into the series:
>

βˆ‘n=1∞(4βˆ’3)nn=βˆ‘n=1∞1nn=βˆ‘n=1∞1n\sum_{n=1}^{\infty} \frac{(4-3)^n}{n} = \sum_{n=1}^{\infty} \frac{1^n}{n} = \sum_{n=1}^{\infty} \frac{1}{n}

> This is the harmonic series, which diverges.

Step 4: State the interval of convergence.

> The series converges for x∈[2,4)x \in [2, 4).

Answer: The interval of convergence is [2,4)[2, 4).

:::question type="MCQ" question="Find the interval of convergence for the power series βˆ‘n=1∞(x+1)nnβ‹…2n\sum_{n=1}^{\infty} \frac{(x+1)^n}{n \cdot 2^n}." options=["(βˆ’3,1)(-3, 1)","(βˆ’3,1]( -3, 1 ]","[βˆ’3,1)[ -3, 1 )","[βˆ’3,1][ -3, 1 ]"] answer="[βˆ’3,1)[-3, 1)" hint="First find the radius of convergence using the Ratio Test, then check the endpoints. Remember to apply the appropriate convergence tests for the resulting series at the endpoints." solution="Step 1: Determine the radius of convergence.
> The series is centered at a=βˆ’1a=-1. Let cn=1nβ‹…2nc_n = \frac{1}{n \cdot 2^n}.
>

lim⁑nβ†’βˆžβˆ£cn+1cn∣=lim⁑nβ†’βˆžβˆ£1/((n+1)2n+1)1/(nβ‹…2n)∣=lim⁑nβ†’βˆžβˆ£nβ‹…2n(n+1)2n+1∣=lim⁑nβ†’βˆžn(n+1)2=12\begin{aligned}\lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right| & = \lim_{n \to \infty} \left| \frac{1/((n+1)2^{n+1})}{1/(n \cdot 2^n)} \right| \\
& = \lim_{n \to \infty} \left| \frac{n \cdot 2^n}{(n+1)2^{n+1}} \right| = \lim_{n \to \infty} \frac{n}{(n+1)2} = \frac{1}{2}\end{aligned}

> So, L=12L=\frac{1}{2}, which means R=1L=2R = \frac{1}{L} = 2.
>
> Step 2: Determine the open interval of convergence.
> The series converges for ∣xβˆ’(βˆ’1)∣<2|x - (-1)| < 2, i.e., ∣x+1∣<2|x+1| < 2.
> This implies βˆ’2<x+1<2-2 < x+1 < 2, so βˆ’3<x<1-3 < x < 1.
>
> Step 3: Check the left endpoint x=βˆ’3x = -3.
> Substitute x=βˆ’3x=-3 into the series:
>
βˆ‘n=1∞(βˆ’3+1)nnβ‹…2n=βˆ‘n=1∞(βˆ’2)nnβ‹…2n=βˆ‘n=1∞(βˆ’1)n2nnβ‹…2n=βˆ‘n=1∞(βˆ’1)nn\sum_{n=1}^{\infty} \frac{(-3+1)^n}{n \cdot 2^n} = \sum_{n=1}^{\infty} \frac{(-2)^n}{n \cdot 2^n} = \sum_{n=1}^{\infty} \frac{(-1)^n 2^n}{n \cdot 2^n} = \sum_{n=1}^{\infty} \frac{(-1)^n}{n}

> This is the alternating harmonic series, which converges by the Alternating Series Test. So x=βˆ’3x=-3 is included.
>
> Step 4: Check the right endpoint x=1x = 1.
> Substitute x=1x=1 into the series:
>
βˆ‘n=1∞(1+1)nnβ‹…2n=βˆ‘n=1∞2nnβ‹…2n=βˆ‘n=1∞1n\sum_{n=1}^{\infty} \frac{(1+1)^n}{n \cdot 2^n} = \sum_{n=1}^{\infty} \frac{2^n}{n \cdot 2^n} = \sum_{n=1}^{\infty} \frac{1}{n}

> This is the harmonic series, which diverges. So x=1x=1 is not included.
>
> Step 5: State the interval of convergence.
> Combining the results, the interval of convergence is [βˆ’3,1)[-3, 1)."
:::

---

4. Properties of Power Series

Power series behave much like polynomials within their interval of convergence, allowing for term-by-term operations.

4.1. Uniqueness of Power Series

If a function f(x)f(x) can be represented by a power series centered at aa, f(x)=βˆ‘n=0∞cn(xβˆ’a)nf(x) = \sum_{n=0}^{\infty} c_n (x-a)^n, then this representation is unique. That is, the coefficients cnc_n are uniquely determined by f(x)f(x).

❗ Uniqueness Theorem

If βˆ‘n=0∞cn(xβˆ’a)n=βˆ‘n=0∞dn(xβˆ’a)n\sum_{n=0}^{\infty} c_n (x-a)^n = \sum_{n=0}^{\infty} d_n (x-a)^n for all xx in some open interval containing aa, then cn=dnc_n = d_n for all nβ‰₯0n \ge 0.

4.2. Term-by-Term Differentiation

A power series can be differentiated term by term within its interval of convergence. The radius of convergence remains unchanged.

πŸ“ Differentiation of Power Series

If f(x)=βˆ‘n=0∞cn(xβˆ’a)nf(x) = \sum_{n=0}^{\infty} c_n (x-a)^n has radius of convergence R>0R > 0, then

fβ€²(x)=βˆ‘n=1∞ncn(xβˆ’a)nβˆ’1f'(x) = \sum_{n=1}^{\infty} n c_n (x-a)^{n-1}

and the radius of convergence for fβ€²(x)f'(x) is also RR.

Quick Example:

Given f(x)=βˆ‘n=0∞xn=11βˆ’xf(x) = \sum_{n=0}^{\infty} x^n = \frac{1}{1-x} for ∣x∣<1|x|<1. Find the power series for fβ€²(x)f'(x).

Step 1: Differentiate term by term.

>

>>fβ€²(x)=ddx(1+x+x2+x3+… )>=0+1+2x+3x2+…>=βˆ‘n=1∞nxnβˆ’1>>> \begin{aligned}> f'(x) & = \frac{d}{dx} (1 + x + x^2 + x^3 + \dots) \\
> & = 0 + 1 + 2x + 3x^2 + \dots \\
> & = \sum_{n=1}^{\infty} n x^{n-1}
> \end{aligned}
>

Step 2: Relate to the original function's derivative.

> We know fβ€²(x)=ddx(11βˆ’x)=1(1βˆ’x)2f'(x) = \frac{d}{dx} \left( \frac{1}{1-x} \right) = \frac{1}{(1-x)^2}.
>
> Thus, 1(1βˆ’x)2=βˆ‘n=1∞nxnβˆ’1\frac{1}{(1-x)^2} = \sum_{n=1}^{\infty} n x^{n-1} for ∣x∣<1|x|<1.

Answer: The power series for fβ€²(x)f'(x) is βˆ‘n=1∞nxnβˆ’1\sum_{n=1}^{\infty} n x^{n-1}.

:::question type="MCQ" question="If f(x)=βˆ‘n=0∞xnn!f(x) = \sum_{n=0}^{\infty} \frac{x^n}{n!} for all xx, what is the power series for fβ€²β€²(x)f''(x)?" options=["βˆ‘n=0∞xnn!\sum_{n=0}^{\infty} \frac{x^n}{n!}","βˆ‘n=1∞xnβˆ’1(nβˆ’1)!\sum_{n=1}^{\infty} \frac{x^{n-1}}{(n-1)!}","βˆ‘n=2∞xnβˆ’2(nβˆ’2)!\sum_{n=2}^{\infty} \frac{x^{n-2}}{(n-2)!}","βˆ‘n=0∞xn+2(n+2)!\sum_{n=0}^{\infty} \frac{x^{n+2}}{(n+2)!}"] answer="βˆ‘n=0∞xnn!\sum_{n=0}^{\infty} \frac{x^n}{n!}" hint="Differentiate twice term by term and adjust the summation index." solution="Step 1: Differentiate f(x)f(x) once.
>

>>f(x)=1+x+x22!+x33!+β‹―+xnn!+…>fβ€²(x)=0+1+2x2!+3x23!+β‹―+nxnβˆ’1n!+…>fβ€²(x)=1+x+x22!+β‹―+xnβˆ’1(nβˆ’1)!+β‹―=βˆ‘n=1∞xnβˆ’1(nβˆ’1)!>>> \begin{aligned}> f(x) & = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \dots + \frac{x^n}{n!} + \dots \\
> f'(x) & = 0 + 1 + \frac{2x}{2!} + \frac{3x^2}{3!} + \dots + \frac{nx^{n-1}}{n!} + \dots \\
> f'(x) & = 1 + x + \frac{x^2}{2!} + \dots + \frac{x^{n-1}}{(n-1)!} + \dots = \sum_{n=1}^{\infty} \frac{x^{n-1}}{(n-1)!}
> \end{aligned}
>

> Let k=nβˆ’1k=n-1. When n=1n=1, k=0k=0.
>
fβ€²(x)=βˆ‘k=0∞xkk!f'(x) = \sum_{k=0}^{\infty} \frac{x^k}{k!}

>
> Step 2: Differentiate fβ€²(x)f'(x) (which is f(x)f(x) again) once more.
>
>>fβ€²β€²(x)=ddx(βˆ‘k=0∞xkk!)=βˆ‘k=1∞kxkβˆ’1k!=βˆ‘k=1∞xkβˆ’1(kβˆ’1)!>>> \begin{aligned}> f''(x) & = \frac{d}{dx} \left( \sum_{k=0}^{\infty} \frac{x^k}{k!} \right) = \sum_{k=1}^{\infty} \frac{kx^{k-1}}{k!} = \sum_{k=1}^{\infty} \frac{x^{k-1}}{(k-1)!}
> \end{aligned}
>

> Let j=kβˆ’1j=k-1. When k=1k=1, j=0j=0.
>
fβ€²β€²(x)=βˆ‘j=0∞xjj!f''(x) = \sum_{j=0}^{\infty} \frac{x^j}{j!}

> Replacing jj with nn, we get βˆ‘n=0∞xnn!\sum_{n=0}^{\infty} \frac{x^n}{n!}. This is the original series.
> This matches the property that exe^x is its own derivative.
>
> Answer: βˆ‘n=0∞xnn!\boxed{\sum_{n=0}^{\infty} \frac{x^n}{n!}}"
:::

4.3. Term-by-Term Integration

A power series can be integrated term by term within its interval of convergence. The radius of convergence remains unchanged.

πŸ“ Integration of Power Series

If f(x)=βˆ‘n=0∞cn(xβˆ’a)nf(x) = \sum_{n=0}^{\infty} c_n (x-a)^n has radius of convergence R>0R > 0, then

∫f(x)dx=C+βˆ‘n=0∞cnn+1(xβˆ’a)n+1\int f(x) dx = C + \sum_{n=0}^{\infty} \frac{c_n}{n+1} (x-a)^{n+1}

and the radius of convergence for the integrated series is also RR.

Quick Example:

Given the geometric series 11βˆ’x=βˆ‘n=0∞xn\frac{1}{1-x} = \sum_{n=0}^{\infty} x^n for ∣x∣<1|x|<1. Find the power series for ln⁑(1βˆ’x)\ln(1-x).

Step 1: Integrate the series for 11βˆ’x\frac{1}{1-x}.

> We know ∫11βˆ’xdx=βˆ’ln⁑(1βˆ’x)+C1\int \frac{1}{1-x} dx = -\ln(1-x) + C_1.
>
> Integrating the series term by term:
>

>>∫(1+x+x2+x3+… )dx=C+x+x22+x33+x44+…>=C+βˆ‘n=0∞xn+1n+1>>> \begin{aligned}> \int \left( 1 + x + x^2 + x^3 + \dots \right) dx & = C + x + \frac{x^2}{2} + \frac{x^3}{3} + \frac{x^4}{4} + \dots \\
> & = C + \sum_{n=0}^{\infty} \frac{x^{n+1}}{n+1}
> \end{aligned}
>

> Let k=n+1k=n+1. Then n=kβˆ’1n=k-1. When n=0n=0, k=1k=1.
>
=C+βˆ‘k=1∞xkk= C + \sum_{k=1}^{\infty} \frac{x^k}{k}

Step 2: Determine the constant of integration CC.

> We have βˆ’ln⁑(1βˆ’x)=C+βˆ‘k=1∞xkk-\ln(1-x) = C + \sum_{k=1}^{\infty} \frac{x^k}{k}.
> Set x=0x=0: βˆ’ln⁑(1βˆ’0)=C+0-\ln(1-0) = C + 0, so 0=C0 = C.
>
> Thus, βˆ’ln⁑(1βˆ’x)=βˆ‘k=1∞xkk=x+x22+x33+…-\ln(1-x) = \sum_{k=1}^{\infty} \frac{x^k}{k} = x + \frac{x^2}{2} + \frac{x^3}{3} + \dots.

Step 3: Express ln⁑(1βˆ’x)\ln(1-x).

>

ln⁑(1βˆ’x)=βˆ’βˆ‘k=1∞xkk=βˆ’xβˆ’x22βˆ’x33βˆ’β€¦\ln(1-x) = - \sum_{k=1}^{\infty} \frac{x^k}{k} = -x - \frac{x^2}{2} - \frac{x^3}{3} - \dots

> This series is valid for ∣x∣<1|x|<1. We must check x=βˆ’1x=-1.
> For x=βˆ’1x=-1, ln⁑(2)=βˆ’βˆ‘k=1∞(βˆ’1)kk=βˆ‘k=1∞(βˆ’1)k+1k=1βˆ’12+13βˆ’β€¦\ln(2) = - \sum_{k=1}^{\infty} \frac{(-1)^k}{k} = \sum_{k=1}^{\infty} \frac{(-1)^{k+1}}{k} = 1 - \frac{1}{2} + \frac{1}{3} - \dots, which is the alternating harmonic series, convergent.
> The interval of convergence is [βˆ’1,1)[-1, 1).

Answer: The power series for ln⁑(1βˆ’x)\ln(1-x) is βˆ’βˆ‘n=1∞xnn- \sum_{n=1}^{\infty} \frac{x^n}{n}, for x∈[βˆ’1,1)x \in [-1, 1).

:::question type="MCQ" question="Given the power series 11+x=βˆ‘n=0∞(βˆ’1)nxn\frac{1}{1+x} = \sum_{n=0}^{\infty} (-1)^n x^n for ∣x∣<1|x|<1. Find the power series for arctan⁑(x)\arctan(x)." options=["βˆ‘n=0∞(βˆ’1)nxn+1n+1\sum_{n=0}^{\infty} (-1)^n \frac{x^{n+1}}{n+1}","βˆ‘n=0∞(βˆ’1)nx2n+12n+1\sum_{n=0}^{\infty} (-1)^n \frac{x^{2n+1}}{2n+1}","βˆ‘n=0∞xn+1n+1\sum_{n=0}^{\infty} \frac{x^{n+1}}{n+1}","βˆ‘n=0∞x2n2n\sum_{n=0}^{\infty} \frac{x^{2n}}{2n}"] answer="βˆ‘n=0∞(βˆ’1)nx2n+12n+1\sum_{n=0}^{\infty} (-1)^n \frac{x^{2n+1}}{2n+1}" hint="Recall that ∫11+x2dx=arctan⁑(x)+C\int \frac{1}{1+x^2} dx = \arctan(x) + C. Manipulate the given series to match the integrand." solution="Step 1: Modify the given series to represent 11+x2\frac{1}{1+x^2}.
> Replace xx with x2x^2 in the series for 11+x\frac{1}{1+x}:
>

11+x2=βˆ‘n=0∞(βˆ’1)n(x2)n=βˆ‘n=0∞(βˆ’1)nx2n\frac{1}{1+x^2} = \sum_{n=0}^{\infty} (-1)^n (x^2)^n = \sum_{n=0}^{\infty} (-1)^n x^{2n}

> This series converges for ∣x2∣<1|x^2|<1, which means ∣x∣<1|x|<1.
>
> Step 2: Integrate the new series term by term.
>
>>∫11+x2dx=∫(βˆ‘n=0∞(βˆ’1)nx2n)dx>=C+βˆ‘n=0∞(βˆ’1)n∫x2ndx>=C+βˆ‘n=0∞(βˆ’1)nx2n+12n+1>>> \begin{aligned}> \int \frac{1}{1+x^2} dx & = \int \left( \sum_{n=0}^{\infty} (-1)^n x^{2n} \right) dx \\
> & = C + \sum_{n=0}^{\infty} (-1)^n \int x^{2n} dx \\
> & = C + \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n+1}}{2n+1}
> \end{aligned}
>

>
> Step 3: Determine the constant of integration CC.
> We know arctan⁑(x)=C+βˆ‘n=0∞(βˆ’1)nx2n+12n+1\arctan(x) = C + \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n+1}}{2n+1}.
> Set x=0x=0: arctan⁑(0)=C+0\arctan(0) = C + 0, so 0=C0=C.
>
> Step 4: State the power series for arctan⁑(x)\arctan(x).
>
arctan⁑(x)=βˆ‘n=0∞(βˆ’1)nx2n+12n+1=xβˆ’x33+x55βˆ’x77+…\arctan(x) = \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n+1}}{2n+1} = x - \frac{x^3}{3} + \frac{x^5}{5} - \frac{x^7}{7} + \dots

> The interval of convergence for arctan⁑(x)\arctan(x) is [βˆ’1,1][-1, 1].
>
> Answer: βˆ‘n=0∞(βˆ’1)nx2n+12n+1\boxed{\sum_{n=0}^{\infty} (-1)^n \frac{x^{2n+1}}{2n+1}}"
:::

4.4. Algebra of Power Series

Power series can be added, subtracted, and multiplied like polynomials within their common interval of convergence.

πŸ“ Algebra of Power Series

If f(x)=βˆ‘n=0∞cn(xβˆ’a)nf(x) = \sum_{n=0}^{\infty} c_n (x-a)^n with radius RfR_f and g(x)=βˆ‘n=0∞dn(xβˆ’a)ng(x) = \sum_{n=0}^{\infty} d_n (x-a)^n with radius RgR_g, then:

    • Addition/Subtraction: f(x)Β±g(x)=βˆ‘n=0∞(cnΒ±dn)(xβˆ’a)nf(x) \pm g(x) = \sum_{n=0}^{\infty} (c_n \pm d_n) (x-a)^n. The radius of convergence is at least min⁑(Rf,Rg)\min(R_f, R_g).

    • Multiplication: f(x)β‹…g(x)=βˆ‘n=0∞en(xβˆ’a)nf(x) \cdot g(x) = \sum_{n=0}^{\infty} e_n (x-a)^n, where en=βˆ‘k=0nckdnβˆ’ke_n = \sum_{k=0}^{n} c_k d_{n-k}. The radius of convergence is at least min⁑(Rf,Rg)\min(R_f, R_g).

Quick Example:

Find the first three non-zero terms of the power series for exsin⁑xe^x \sin x using multiplication of series.

Step 1: Write out the known Maclaurin series for exe^x and sin⁑x\sin x.

>

>>ex=1+x+x22!+x33!+…>sin⁑x=xβˆ’x33!+x55!βˆ’β‹―>>> \begin{aligned}> e^x & = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \dots \\
> \sin x & = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \dots
> \end{aligned}
>

Step 2: Multiply the series term by term.

>

(1+x+x22+x36+… )β‹…(xβˆ’x36+… )(1 + x + \frac{x^2}{2} + \frac{x^3}{6} + \dots) \cdot (x - \frac{x^3}{6} + \dots)

>
> Constant term: 00 (since sin⁑x\sin x has no constant term).
> Term in xx: 1β‹…x=x1 \cdot x = x.
> Term in x2x^2: xβ‹…x=x2x \cdot x = x^2.
> Term in x3x^3: x22β‹…x+1β‹…(βˆ’x36)=x32βˆ’x36=3x3βˆ’x36=2x36=x33\frac{x^2}{2} \cdot x + 1 \cdot (-\frac{x^3}{6}) = \frac{x^3}{2} - \frac{x^3}{6} = \frac{3x^3 - x^3}{6} = \frac{2x^3}{6} = \frac{x^3}{3}.

Answer: The first three non-zero terms are x+x2+x33x + x^2 + \frac{x^3}{3}.

:::question type="MCQ" question="Given ex=βˆ‘n=0∞xnn!e^x = \sum_{n=0}^{\infty} \frac{x^n}{n!} and eβˆ’x=βˆ‘n=0∞(βˆ’x)nn!e^{-x} = \sum_{n=0}^{\infty} \frac{(-x)^n}{n!}. Find the power series for cosh⁑x=ex+eβˆ’x2\cosh x = \frac{e^x + e^{-x}}{2}." options=["βˆ‘n=0∞x2n(2n)!\sum_{n=0}^{\infty} \frac{x^{2n}}{(2n)!}","βˆ‘n=0∞x2n+1(2n+1)!\sum_{n=0}^{\infty} \frac{x^{2n+1}}{(2n+1)!}","βˆ‘n=0∞xnn!\sum_{n=0}^{\infty} \frac{x^n}{n!}","βˆ‘n=0∞(βˆ’1)nxnn!\sum_{n=0}^{\infty} (-1)^n \frac{x^n}{n!}"] answer="βˆ‘n=0∞x2n(2n)!\sum_{n=0}^{\infty} \frac{x^{2n}}{(2n)!}" hint="Add the two series term by term and observe which terms cancel out or combine." solution="Step 1: Write out the series for exe^x and eβˆ’xe^{-x}.
>

>>ex=1+x+x22!+x33!+x44!+…>eβˆ’x=1βˆ’x+x22!βˆ’x33!+x44!βˆ’β‹―>>> \begin{aligned}> e^x & = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \frac{x^4}{4!} + \dots \\
> e^{-x} & = 1 - x + \frac{x^2}{2!} - \frac{x^3}{3!} + \frac{x^4}{4!} - \dots
> \end{aligned}
>

>
> Step 2: Add the two series.
>
>>ex+eβˆ’x=(1+1)+(xβˆ’x)+(x22!+x22!)+(x33!βˆ’x33!)+(x44!+x44!)+…>ex+eβˆ’x=2+0+2x22!+0+2x44!+…>ex+eβˆ’x=2(1+x22!+x44!+… )>>> \begin{aligned}> e^x + e^{-x} & = (1+1) + (x-x) + \left(\frac{x^2}{2!}+\frac{x^2}{2!}\right) + \left(\frac{x^3}{3!}-\frac{x^3}{3!}\right) + \left(\frac{x^4}{4!}+\frac{x^4}{4!}\right) + \dots \\
> e^x + e^{-x} & = 2 + 0 + 2\frac{x^2}{2!} + 0 + 2\frac{x^4}{4!} + \dots \\
> e^x + e^{-x} & = 2 \left( 1 + \frac{x^2}{2!} + \frac{x^4}{4!} + \dots \right)
> \end{aligned}
>

>
> Step 3: Divide by 2 to get cosh⁑x\cosh x.
>
cosh⁑x=ex+eβˆ’x2=1+x22!+x44!+…\cosh x = \frac{e^x + e^{-x}}{2} = 1 + \frac{x^2}{2!} + \frac{x^4}{4!} + \dots

> This can be written in summation notation as βˆ‘n=0∞x2n(2n)!\sum_{n=0}^{\infty} \frac{x^{2n}}{(2n)!}.
>
> Answer: βˆ‘n=0∞x2n(2n)!\boxed{\sum_{n=0}^{\infty} \frac{x^{2n}}{(2n)!}}"
:::

5. Taylor and Maclaurin Series

Taylor series provide a general method to represent a function as a power series. A Maclaurin series is a special case of a Taylor series where the expansion is centered at a=0a=0.

πŸ“ Taylor Series

The Taylor series for a function f(x)f(x) about x=ax=a is given by:

f(x)=βˆ‘n=0∞f(n)(a)n!(xβˆ’a)n=f(a)+fβ€²(a)(xβˆ’a)+fβ€²β€²(a)2!(xβˆ’a)2+…\begin{aligned}f(x) & = \sum_{n=0}^{\infty} \frac{f^{(n)}(a)}{n!} (x-a)^n \\
& = f(a) + f'(a)(x-a) + \frac{f''(a)}{2!}(x-a)^2 + \dots\end{aligned}

πŸ“ Maclaurin Series

The Maclaurin series for a function f(x)f(x) is the Taylor series centered at a=0a=0:

f(x)=βˆ‘n=0∞f(n)(0)n!xn=f(0)+fβ€²(0)x+fβ€²β€²(0)2!x2+…\begin{aligned}f(x) & = \sum_{n=0}^{\infty} \frac{f^{(n)}(0)}{n!} x^n \\
& = f(0) + f'(0)x + \frac{f''(0)}{2!}x^2 + \dots\end{aligned}

We list several common Maclaurin series, as they are frequently tested:

πŸ“ Common Maclaurin Series

  • Geometric Series: 11βˆ’x=βˆ‘n=0∞xn=1+x+x2+x3+…for ∣x∣<1\frac{1}{1-x} = \sum_{n=0}^{\infty} x^n = 1 + x + x^2 + x^3 + \dots \quad \text{for } |x|<1.

  • Exponential Function: ex=βˆ‘n=0∞xnn!=1+x+x22!+x33!+…forΒ allΒ xe^x = \sum_{n=0}^{\infty} \frac{x^n}{n!} = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \dots \quad \text{for all } x.

  • Sine Function: sin⁑x=βˆ‘n=0∞(βˆ’1)nx2n+1(2n+1)!=xβˆ’x33!+x55!βˆ’β€¦forΒ allΒ x\sin x = \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n+1}}{(2n+1)!} = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \dots \quad \text{for all } x.

  • Cosine Function: cos⁑x=βˆ‘n=0∞(βˆ’1)nx2n(2n)!=1βˆ’x22!+x44!βˆ’β€¦forΒ allΒ x\cos x = \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n}}{(2n)!} = 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \dots \quad \text{for all } x.

  • Natural Logarithm: ln⁑(1+x)=βˆ‘n=1∞(βˆ’1)nβˆ’1xnn=xβˆ’x22+x33βˆ’β€¦forΒ βˆ’1<x≀1\ln(1+x) = \sum_{n=1}^{\infty} (-1)^{n-1} \frac{x^n}{n} = x - \frac{x^2}{2} + \frac{x^3}{3} - \dots \quad \text{for } -1 < x \le 1.

  • * Note: ln⁑(1βˆ’x)=βˆ’βˆ‘n=1∞xnn=βˆ’xβˆ’x22βˆ’x33βˆ’β€¦forΒ βˆ’1≀x<1\ln(1-x) = - \sum_{n=1}^{\infty} \frac{x^n}{n} = -x - \frac{x^2}{2} - \frac{x^3}{3} - \dots \quad \text{for } -1 \le x < 1.
  • Inverse Tangent: arctan⁑x=βˆ‘n=0∞(βˆ’1)nx2n+12n+1=xβˆ’x33+x55βˆ’β€¦forΒ βˆ’1≀x≀1\arctan x = \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n+1}}{2n+1} = x - \frac{x^3}{3} + \frac{x^5}{5} - \dots \quad \text{for } -1 \le x \le 1.

  • Binomial Series: (1+x)k=βˆ‘n=0∞(kn)xn=1+kx+k(kβˆ’1)2!x2+…for ∣x∣<1(1+x)^k = \sum_{n=0}^{\infty} \binom{k}{n} x^n = 1 + kx + \frac{k(k-1)}{2!}x^2 + \dots \quad \text{for } |x|<1.

Quick Example:

Find the Maclaurin series for f(x)=sin⁑xf(x) = \sin x.

Step 1: Find the derivatives of f(x)f(x) and evaluate them at x=0x=0.

> f(x)=sin⁑xβ€…β€ŠβŸΉβ€…β€Šf(0)=0f(x) = \sin x \implies f(0) = 0
> fβ€²(x)=cos⁑xβ€…β€ŠβŸΉβ€…β€Šfβ€²(0)=1f'(x) = \cos x \implies f'(0) = 1
> fβ€²β€²(x)=βˆ’sin⁑xβ€…β€ŠβŸΉβ€…β€Šfβ€²β€²(0)=0f''(x) = -\sin x \implies f''(0) = 0
> fβ€²β€²β€²(x)=βˆ’cos⁑xβ€…β€ŠβŸΉβ€…β€Šfβ€²β€²β€²(0)=βˆ’1f'''(x) = -\cos x \implies f'''(0) = -1
> f(4)(x)=sin⁑xβ€…β€ŠβŸΉβ€…β€Šf(4)(0)=0f^{(4)}(x) = \sin x \implies f^{(4)}(0) = 0
> The pattern of derivatives at x=0x=0 is 0,1,0,βˆ’1,0,1,0,βˆ’1,…0, 1, 0, -1, 0, 1, 0, -1, \dots

Step 2: Substitute these values into the Maclaurin series formula.

>

>>f(x)=f(0)+fβ€²(0)x+fβ€²β€²(0)2!x2+fβ€²β€²β€²(0)3!x3+f(4)(0)4!x4+…>f(x)=0+1β‹…x+02!x2+βˆ’13!x3+04!x4+15!x5+…>f(x)=xβˆ’x33!+x55!βˆ’x77!+β‹―>>> \begin{aligned}> f(x) & = f(0) + f'(0)x + \frac{f''(0)}{2!}x^2 + \frac{f'''(0)}{3!}x^3 + \frac{f^{(4)}(0)}{4!}x^4 + \dots \\
> f(x) & = 0 + 1 \cdot x + \frac{0}{2!}x^2 + \frac{-1}{3!}x^3 + \frac{0}{4!}x^4 + \frac{1}{5!}x^5 + \dots \\
> f(x) & = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \frac{x^7}{7!} + \dots
> \end{aligned}
>

Step 3: Write the series in summation notation.

> The terms are for odd powers of xx with alternating signs. The general term can be written as (βˆ’1)nx2n+1(2n+1)!(-1)^n \frac{x^{2n+1}}{(2n+1)!}.
>
>

sin⁑x=βˆ‘n=0∞(βˆ’1)nx2n+1(2n+1)!\sin x = \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n+1}}{(2n+1)!}

Answer: The Maclaurin series for sin⁑x\sin x is βˆ‘n=0∞(βˆ’1)nx2n+1(2n+1)!\sum_{n=0}^{\infty} (-1)^n \frac{x^{2n+1}}{(2n+1)!}.

:::question type="MCQ" question="Which of the following functions has the Maclaurin series expansion 1βˆ’x1!+x22!βˆ’x33!+…1 - \frac{x}{1!} + \frac{x^2}{2!} - \frac{x^3}{3!} + \dots?" options=["exe^x","eβˆ’xe^{-x}","sin⁑x\sin x","cos⁑x\cos x"] answer="eβˆ’xe^{-x}" hint="Compare the given series with the standard Maclaurin series expansions." solution="The given series is 1βˆ’x1!+x22!βˆ’x33!+…1 - \frac{x}{1!} + \frac{x^2}{2!} - \frac{x^3}{3!} + \dots.
This can be written as βˆ‘n=0∞(βˆ’1)nxnn!\sum_{n=0}^{\infty} (-1)^n \frac{x^n}{n!}.
We know that the Maclaurin series for exe^x is βˆ‘n=0∞xnn!\sum_{n=0}^{\infty} \frac{x^n}{n!}.
If we replace xx with βˆ’x-x in the series for exe^x, we get:

eβˆ’x=βˆ‘n=0∞(βˆ’x)nn!=βˆ‘n=0∞(βˆ’1)nxnn!e^{-x} = \sum_{n=0}^{\infty} \frac{(-x)^n}{n!} = \sum_{n=0}^{\infty} \frac{(-1)^n x^n}{n!}

This matches the given series.
>
> Answer: eβˆ’x\boxed{e^{-x}}"
:::

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Advanced Applications

Power series can be used to approximate values, evaluate difficult integrals, or solve differential equations.

Quick Example:

Evaluate the definite integral ∫01sin⁑xxdx\int_0^1 \frac{\sin x}{x} dx as an infinite series.

Step 1: Write the Maclaurin series for sin⁑x\sin x.

>

sin⁑x=xβˆ’x33!+x55!βˆ’x77!+β‹―=βˆ‘n=0∞(βˆ’1)nx2n+1(2n+1)!\sin x = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \frac{x^7}{7!} + \dots = \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n+1}}{(2n+1)!}

Step 2: Form the series for sin⁑xx\frac{\sin x}{x}.

> Divide each term by xx (for x≠0x \ne 0):
>

sin⁑xx=1βˆ’x23!+x45!βˆ’x67!+β‹―=βˆ‘n=0∞(βˆ’1)nx2n(2n+1)!\frac{\sin x}{x} = 1 - \frac{x^2}{3!} + \frac{x^4}{5!} - \frac{x^6}{7!} + \dots = \sum_{n=0}^{\infty} (-1)^n \frac{x^{2n}}{(2n+1)!}

Step 3: Integrate the series term by term from 00 to 11.

>

>>∫01sin⁑xxdx=∫01(1βˆ’x23!+x45!βˆ’x67!+… )dx>=[xβˆ’x33β‹…3!+x55β‹…5!βˆ’x77β‹…7!+… ]01>=(1βˆ’13β‹…3!+15β‹…5!βˆ’17β‹…7!+… )βˆ’(0)>=βˆ‘n=0∞(βˆ’1)n1(2n+1)(2n+1)!>>> \begin{aligned}> \int_0^1 \frac{\sin x}{x} dx & = \int_0^1 \left( 1 - \frac{x^2}{3!} + \frac{x^4}{5!} - \frac{x^6}{7!} + \dots \right) dx \\
> & = \left[ x - \frac{x^3}{3 \cdot 3!} + \frac{x^5}{5 \cdot 5!} - \frac{x^7}{7 \cdot 7!} + \dots \right]_0^1 \\
> & = \left( 1 - \frac{1}{3 \cdot 3!} + \frac{1}{5 \cdot 5!} - \frac{1}{7 \cdot 7!} + \dots \right) - (0) \\
> & = \sum_{n=0}^{\infty} (-1)^n \frac{1}{(2n+1)(2n+1)!}
> \end{aligned}
>

Answer: The integral is 1βˆ’118+1600βˆ’β€¦1 - \frac{1}{18} + \frac{1}{600} - \dots.

:::question type="NAT" question="Using the Maclaurin series for exe^x, approximate e0.1e^{0.1} to four decimal places. (Truncate the series after the x3x^3 term)." answer="1.1052" hint="Substitute x=0.1x=0.1 into the Maclaurin series for exe^x and sum the first four terms." solution="Step 1: Write the Maclaurin series for exe^x.
>

ex=1+x+x22!+x33!+x44!+…e^x = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \frac{x^4}{4!} + \dots

>
> Step 2: Substitute x=0.1x=0.1 and sum the terms up to x3x^3.
>
>>e0.1β‰ˆ1+0.1+(0.1)22!+(0.1)33!>e0.1β‰ˆ1+0.1+0.012+0.0016>e0.1β‰ˆ1+0.1+0.005+0.0001666β‹―>>> \begin{aligned}> e^{0.1} & \approx 1 + 0.1 + \frac{(0.1)^2}{2!} + \frac{(0.1)^3}{3!} \\
> e^{0.1} & \approx 1 + 0.1 + \frac{0.01}{2} + \frac{0.001}{6} \\
> e^{0.1} & \approx 1 + 0.1 + 0.005 + 0.0001666\dots
> \end{aligned}
>

>
> Step 3: Calculate the sum and round to four decimal places.
>
e0.1β‰ˆ1.1051666…e^{0.1} \approx 1.1051666\dots

> Rounding to four decimal places, we get 1.10521.1052.
>
> Answer: 1.1052\boxed{1.1052}"
:::

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Problem-Solving Strategies

πŸ’‘ CUET PG Strategy
    • Identify the Series Type: Recognize if you need to find the radius/interval of convergence, or a specific series expansion.
    • Ratio Test for R: For radius of convergence, the Ratio Test is almost always the most efficient method.
    • Endpoint Checks are CRITICAL: Never forget to test the series convergence at the endpoints of the interval after finding the radius. Use comparison, alternating series, or p-series tests.
    • Memorize Common Series: Knowing the Maclaurin series for ex,sin⁑x,cos⁑x,11βˆ’x,ln⁑(1+x),arctan⁑xe^x, \sin x, \cos x, \frac{1}{1-x}, \ln(1+x), \arctan x will save significant time.
    • Manipulation over Recalculation: If asked for a series of a function like xsin⁑(x2)x \sin(x^2), it is faster to substitute and multiply a known series (sin⁑x\sin x) than to compute derivatives for a Taylor series.
    • Differentiation/Integration: Utilize term-by-term differentiation or integration to derive new series from known ones, especially for functions like 1(1βˆ’x)2\frac{1}{(1-x)^2} or arctan⁑x\arctan x.

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Common Mistakes

⚠️ Watch Out

❌ Forgetting to check endpoints for interval of convergence.
βœ… Always check x=aβˆ’Rx=a-R and x=a+Rx=a+R using appropriate convergence tests (e.g., AST, p-series, Integral Test).

❌ Incorrectly applying the Ratio Test formula.
βœ… Ensure you compute lim⁑nβ†’βˆžβˆ£cn+1cn∣∣xβˆ’a∣\lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right| |x-a| and set it less than 1. Then solve for RR to find RR.

❌ Confusing Taylor and Maclaurin series.
βœ… Maclaurin series are Taylor series centered at a=0a=0. Taylor series can be centered at any aa.

❌ Assuming the interval of convergence is always open.
βœ… The interval can be open, closed, or half-open, depending on endpoint behavior. RR is always positive or zero/infinity.

❌ Mistakes in algebraic manipulation of series (e.g., multiplication).
βœ… Be careful with coefficient calculations when multiplying series. It's often easier to find the first few terms by direct multiplication before looking for a general pattern.

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Practice Questions

:::question type="MCQ" question="The radius of convergence of the power series βˆ‘n=0∞xn3n(n+1)\sum_{n=0}^{\infty} \frac{x^n}{3^n (n+1)} is:" options=["00","11","33","∞\infty"] answer="33" hint="Apply the Ratio Test to find the limit of the ratio of consecutive terms." solution="Step 1: Identify cnc_n.
> Here cn=13n(n+1)c_n = \frac{1}{3^n (n+1)}.
>
> Step 2: Apply the Ratio Test.
> We calculate L=lim⁑nβ†’βˆžβˆ£cn+1cn∣L = \lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right|.
>

L=lim⁑nβ†’βˆžβˆ£1/(3n+1(n+2))1/(3n(n+1))∣=lim⁑nβ†’βˆžβˆ£3n(n+1)3n+1(n+2)∣=lim⁑nβ†’βˆž13β‹…n+1n+2=13β‹…1=13\begin{aligned}L & = \lim_{n \to \infty} \left| \frac{1/(3^{n+1}(n+2))}{1/(3^n(n+1))} \right| \\
& = \lim_{n \to \infty} \left| \frac{3^n(n+1)}{3^{n+1}(n+2)} \right| \\
& = \lim_{n \to \infty} \frac{1}{3} \cdot \frac{n+1}{n+2} = \frac{1}{3} \cdot 1 = \frac{1}{3}\end{aligned}

>
> Step 3: Determine RR.
> The radius of convergence R=1L=11/3=3R = \frac{1}{L} = \frac{1}{1/3} = 3.
Answer: 3\boxed{3}"
:::

:::question type="MCQ" question="The power series for f(x)=1(1βˆ’x)2f(x) = \frac{1}{(1-x)^2} centered at x=0x=0 is:" options=["βˆ‘n=0∞xn\sum_{n=0}^{\infty} x^n","βˆ‘n=1∞nxnβˆ’1\sum_{n=1}^{\infty} n x^{n-1}","βˆ‘n=0∞nxn\sum_{n=0}^{\infty} n x^n","βˆ‘n=2∞n(nβˆ’1)xnβˆ’2\sum_{n=2}^{\infty} n(n-1) x^{n-2}"] answer="βˆ‘n=1∞nxnβˆ’1\sum_{n=1}^{\infty} n x^{n-1}" hint="Recall the geometric series and its derivative." solution="Step 1: Start with the geometric series.
> We know that 11βˆ’x=βˆ‘n=0∞xn=1+x+x2+x3+…\frac{1}{1-x} = \sum_{n=0}^{\infty} x^n = 1 + x + x^2 + x^3 + \dots for ∣x∣<1|x|<1.
>
> Step 2: Differentiate both sides with respect to xx.
> The derivative of 11βˆ’x\frac{1}{1-x} is ddx(1βˆ’x)βˆ’1=βˆ’1(1βˆ’x)βˆ’2(βˆ’1)=1(1βˆ’x)2\frac{d}{dx}(1-x)^{-1} = -1(1-x)^{-2}(-1) = \frac{1}{(1-x)^2}.
>
> Step 3: Differentiate the series term by term.
>

ddx(βˆ‘n=0∞xn)=ddx(1+x+x2+x3+… )=0+1+2x+3x2+…=βˆ‘n=1∞nxnβˆ’1\begin{aligned}\frac{d}{dx} \left( \sum_{n=0}^{\infty} x^n \right) & = \frac{d}{dx} (1 + x + x^2 + x^3 + \dots) \\
& = 0 + 1 + 2x + 3x^2 + \dots \\
& = \sum_{n=1}^{\infty} n x^{n-1}\end{aligned}

>
> Thus, 1(1βˆ’x)2=βˆ‘n=1∞nxnβˆ’1\frac{1}{(1-x)^2} = \sum_{n=1}^{\infty} n x^{n-1}.
Answer: βˆ‘n=1∞nxnβˆ’1\boxed{\sum_{n=1}^{\infty} n x^{n-1}}"
:::

:::question type="NAT" question="If f(x)=βˆ‘n=0∞xnn!f(x) = \sum_{n=0}^{\infty} \frac{x^n}{n!}, what is the value of fβ€²(0)f'(0)?" answer="1" hint="Identify the function represented by the power series and evaluate its derivative at x=0x=0." solution="Step 1: Identify the function represented by the power series.
> The series f(x)=βˆ‘n=0∞xnn!=1+x+x22!+x33!+…f(x) = \sum_{n=0}^{\infty} \frac{x^n}{n!} = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \dots is the Maclaurin series for exe^x.
> So, f(x)=exf(x) = e^x.
>
> Step 2: Find the first derivative of f(x)f(x).
> fβ€²(x)=ddx(ex)=exf'(x) = \frac{d}{dx}(e^x) = e^x.
>
> Step 3: Evaluate fβ€²(0)f'(0).
> fβ€²(0)=e0=1f'(0) = e^0 = 1.
Answer: 1\boxed{1}"
:::

:::question type="MCQ" question="Consider the series S=1βˆ’12+13βˆ’14+…S = 1 - \frac{1}{2} + \frac{1}{3} - \frac{1}{4} + \dots. This series represents:" options=["ln⁑(2)\ln(2)","ln⁑(1)\ln(1)","Ο€4\frac{\pi}{4}","diverges"] answer="ln⁑(2)\ln(2)" hint="Compare the series with the Maclaurin series for ln⁑(1+x)\ln(1+x)." solution="Step 1: Recall the Maclaurin series for ln⁑(1+x)\ln(1+x).
>

ln⁑(1+x)=xβˆ’x22+x33βˆ’x44+…forΒ βˆ’1<x≀1\ln(1+x) = x - \frac{x^2}{2} + \frac{x^3}{3} - \frac{x^4}{4} + \dots \quad \text{for } -1 < x \le 1

>
> Step 2: Substitute x=1x=1 into the series.
> When x=1x=1, the series becomes:
>
ln⁑(1+1)=1βˆ’122+133βˆ’144+…ln⁑(2)=1βˆ’12+13βˆ’14+…\begin{aligned}\ln(1+1) & = 1 - \frac{1^2}{2} + \frac{1^3}{3} - \frac{1^4}{4} + \dots \\
\ln(2) & = 1 - \frac{1}{2} + \frac{1}{3} - \frac{1}{4} + \dots\end{aligned}

> This exactly matches the given series SS.
>
> The series converges at x=1x=1 by the Alternating Series Test.
Answer: ln⁑(2)\boxed{\ln(2)}"
:::

:::question type="MSQ" question="Which of the following statements about the interval of convergence for βˆ‘n=1∞(xβˆ’5)nn2\sum_{n=1}^{\infty} \frac{(x-5)^n}{n^2} are correct?" options=["The radius of convergence is 11.","The interval of convergence is (4,6)(4, 6).","The series converges at x=4x=4.","The series converges at x=6x=6."] answer="The radius of convergence is 11,The series converges at x=4x=4,The series converges at x=6x=6" hint="Use the Ratio Test for the radius. Then check both endpoints for convergence." solution="Step 1: Find the radius of convergence.
> The series is centered at a=5a=5. Let cn=1n2c_n = \frac{1}{n^2}.
>

lim⁑nβ†’βˆžβˆ£cn+1cn∣=lim⁑nβ†’βˆžβˆ£1/(n+1)21/n2∣=lim⁑nβ†’βˆžβˆ£n2(n+1)2∣=lim⁑nβ†’βˆž(nn+1)2=12=1\begin{aligned}\lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right| & = \lim_{n \to \infty} \left| \frac{1/(n+1)^2}{1/n^2} \right| = \lim_{n \to \infty} \left| \frac{n^2}{(n+1)^2} \right| \\
& = \lim_{n \to \infty} \left( \frac{n}{n+1} \right)^2 = 1^2 = 1\end{aligned}

> So, L=1L=1, which means R=1L=1R = \frac{1}{L} = 1.
> Thus, 'The radius of convergence is 11' is correct.
>
> Step 2: Determine the open interval.
> The series converges for ∣xβˆ’5∣<1|x-5| < 1, which means βˆ’1<xβˆ’5<1-1 < x-5 < 1, so 4<x<64 < x < 6.
> Thus, 'The interval of convergence is (4,6)(4, 6)' is incorrect because it doesn't account for endpoints.
>
> Step 3: Check the left endpoint x=4x=4.
> Substitute x=4x=4 into the series:
>
βˆ‘n=1∞(4βˆ’5)nn2=βˆ‘n=1∞(βˆ’1)nn2\sum_{n=1}^{\infty} \frac{(4-5)^n}{n^2} = \sum_{n=1}^{\infty} \frac{(-1)^n}{n^2}

> This is an alternating series. The terms 1n2\frac{1}{n^2} are positive, decreasing, and tend to 0. By the Alternating Series Test, it converges. Moreover, βˆ‘βˆ£(βˆ’1)nn2∣=βˆ‘1n2\sum \left| \frac{(-1)^n}{n^2} \right| = \sum \frac{1}{n^2}, which is a convergent p-series (p=2>1p=2 > 1). So the series converges absolutely.
> Thus, 'The series converges at x=4x=4' is correct.
>
> Step 4: Check the right endpoint x=6x=6.
> Substitute x=6x=6 into the series:
>
βˆ‘n=1∞(6βˆ’5)nn2=βˆ‘n=1∞1nn2=βˆ‘n=1∞1n2\sum_{n=1}^{\infty} \frac{(6-5)^n}{n^2} = \sum_{n=1}^{\infty} \frac{1^n}{n^2} = \sum_{n=1}^{\infty} \frac{1}{n^2}

> This is a p-series with p=2>1p=2 > 1, which converges.
> Thus, 'The series converges at x=6x=6' is correct.
>
> The full interval of convergence is [4,6][4, 6].
Answer: TheΒ radiusΒ ofΒ convergenceΒ isΒ 1,Β TheΒ seriesΒ convergesΒ atΒ x=4,Β TheΒ seriesΒ convergesΒ atΒ x=6\boxed{\text{The radius of convergence is } 1 \text{, The series converges at } x=4 \text{, The series converges at } x=6}"
:::

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Summary

❗ Key Formulas & Takeaways

| # | Formula/Concept | Expression |
|---|----------------|------------|
| 1 | Power Series | βˆ‘n=0∞cn(xβˆ’a)n\sum_{n=0}^{\infty} c_n (x-a)^n |
| 2 | Radius of Convergence (Ratio Test) | R=1LR = \frac{1}{L}, where L=lim⁑nβ†’βˆžβˆ£cn+1cn∣L = \lim_{n \to \infty} \left| \frac{c_{n+1}}{c_n} \right| |
| 3 | Term-by-Term Differentiation | fβ€²(x)=βˆ‘n=1∞ncn(xβˆ’a)nβˆ’1f'(x) = \sum_{n=1}^{\infty} n c_n (x-a)^{n-1} (same RR) |
| 4 | Term-by-Term Integration | ∫f(x)dx=C+βˆ‘n=0∞cnn+1(xβˆ’a)n+1\int f(x) dx = C + \sum_{n=0}^{\infty} \frac{c_n}{n+1} (x-a)^{n+1} (same RR) |
| 5 | Maclaurin Series | f(x)=βˆ‘n=0∞f(n)(0)n!xnf(x) = \sum_{n=0}^{\infty} \frac{f^{(n)}(0)}{n!} x^n |
| 6 | Common Series (e.g., exe^x) | βˆ‘n=0∞xnn!\sum_{n=0}^{\infty} \frac{x^n}{n!} (for all xx) |
| 7 | Common Series (e.g., ln⁑(1βˆ’x)\ln(1-x)) | βˆ’βˆ‘n=1∞xnn-\sum_{n=1}^{\infty} \frac{x^n}{n} (for βˆ’1≀x<1-1 \le x < 1) |

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What's Next?

πŸ’‘ Continue Learning

This topic connects to:

    • Fourier Series: Power series are representations of functions as infinite sums of powers; Fourier series represent periodic functions as infinite sums of sines and cosines. Both are crucial for functional analysis.

    • Complex Analysis: Power series form the basis for defining analytic functions in the complex plane, where their convergence properties are extended to complex variables.

    • Differential Equations: Power series methods are used to find series solutions to linear differential equations, especially those with variable coefficients.

Chapter Summary

❗ Power Series β€” Key Points

A power series βˆ‘n=0∞an(xβˆ’c)n\sum_{n=0}^{\infty} a_n (x-c)^n converges absolutely for ∣xβˆ’c∣<R|x-c| < R and diverges for ∣xβˆ’c∣>R|x-c| > R, where RR is the radius of convergence.
The radius of convergence RR can be determined using the ratio test R=lim⁑nβ†’βˆžβˆ£anan+1∣R = \lim_{n \to \infty} \left| \frac{a_n}{a_{n+1}} \right| or the root test R=1lim⁑nβ†’βˆžβˆ£an∣1/nR = \frac{1}{\lim_{n \to \infty} |a_n|^{1/n}}.
The interval of convergence requires separate analysis at the endpoints x=cΒ±Rx = c \pm R using appropriate convergence tests (e.g., Alternating Series Test, p-series test).
Within its radius of convergence, a power series can be differentiated and integrated term-by-term, and the radius of convergence of the resulting series remains the same.
If a function f(x)f(x) has a power series representation f(x)=βˆ‘n=0∞an(xβˆ’c)nf(x) = \sum_{n=0}^{\infty} a_n (x-c)^n on an open interval, then this representation is unique, with an=f(n)(c)n!a_n = \frac{f^{(n)}(c)}{n!} (Taylor coefficients).
Common functions (e.g., ex,sin⁑x,cos⁑x,11βˆ’xe^x, \sin x, \cos x, \frac{1}{1-x}) have well-known Maclaurin series representations, which are crucial for approximations and solving problems.

---

Chapter Review Questions

:::question type="MCQ" question="What is the interval of convergence for the power series βˆ‘n=1∞(xβˆ’3)nn\sum_{n=1}^{\infty} \frac{(x-3)^n}{n}?" options=["[2,4)[2, 4)","(2,4](2, 4]","(2,4)(2, 4)","[2,4][2, 4]"] answer="[2,4)[2, 4)" hint="Use the Ratio Test to find the radius of convergence, then check the endpoints separately." solution="Applying the Ratio Test:

lim⁑nβ†’βˆžβˆ£(xβˆ’3)n+1/(n+1)(xβˆ’3)n/n∣=lim⁑nβ†’βˆžβˆ£(xβˆ’3)nn+1∣=∣xβˆ’3∣\lim_{n \to \infty} \left| \frac{(x-3)^{n+1}/(n+1)}{(x-3)^n/n} \right| = \lim_{n \to \infty} \left| (x-3) \frac{n}{n+1} \right| = |x-3|

For convergence, ∣xβˆ’3∣<1|x-3| < 1, which implies 2<x<42 < x < 4.
At x=2x=2: The series becomes βˆ‘n=1∞(βˆ’1)nn\sum_{n=1}^{\infty} \frac{(-1)^n}{n}, which converges by the Alternating Series Test.
At x=4x=4: The series becomes βˆ‘n=1∞1n\sum_{n=1}^{\infty} \frac{1}{n}, which is the harmonic series and diverges.
Thus, the interval of convergence is [2,4)[2, 4).
Answer: \boxed{[2, 4)}}"
:::

:::question type="NAT" question="What is the radius of convergence of the power series βˆ‘n=0∞nnn!xn\sum_{n=0}^{\infty} \frac{n^n}{n!} x^n?" answer="0.36787944" hint="Use the Ratio Test and recall the definition of ee as a limit." solution="Using the Ratio Test:

L=lim⁑nβ†’βˆžβˆ£an+1an∣=lim⁑nβ†’βˆžβˆ£(n+1)n+1/(n+1)!nn/n!∣=lim⁑nβ†’βˆžβˆ£(n+1)n+1(n+1)nn∣=lim⁑nβ†’βˆžβˆ£(n+1n)n∣=lim⁑nβ†’βˆž(1+1n)n=eL = \lim_{n \to \infty} \left| \frac{a_{n+1}}{a_n} \right| = \lim_{n \to \infty} \left| \frac{(n+1)^{n+1}/(n+1)!}{n^n/n!} \right| = \lim_{n \to \infty} \left| \frac{(n+1)^{n+1}}{(n+1)n^n} \right| = \lim_{n \to \infty} \left| \left( \frac{n+1}{n} \right)^n \right| = \lim_{n \to \infty} \left( 1 + \frac{1}{n} \right)^n = e

For convergence,
L∣x∣<1β€…β€ŠβŸΉβ€…β€Še∣x∣<1β€…β€ŠβŸΉβ€…β€Šβˆ£x∣<1/eL|x| < 1 \implies e|x| < 1 \implies |x| < 1/e

Therefore, the radius of convergence R=1/eβ‰ˆ0.36787944R = 1/e \approx 0.36787944.
Answer: \boxed{0.36787944}"
:::

:::question type="MCQ" question="Consider the function f(x)=sin⁑(x2)f(x) = \sin(x^2). Which of the following is its Maclaurin series?" options=["βˆ‘n=0∞(βˆ’1)n(2n+1)!x2n+2\sum_{n=0}^{\infty} \frac{(-1)^n}{(2n+1)!} x^{2n+2}","βˆ‘n=0∞(βˆ’1)n(2n)!x4n\sum_{n=0}^{\infty} \frac{(-1)^n}{(2n)!} x^{4n}","βˆ‘n=0∞(βˆ’1)n(2n+1)!x4n+2\sum_{n=0}^{\infty} \frac{(-1)^n}{(2n+1)!} x^{4n+2}","βˆ‘n=0∞(βˆ’1)n(2n)!x2n+2\sum_{n=0}^{\infty} \frac{(-1)^n}{(2n)!} x^{2n+2}"] answer="βˆ‘n=0∞(βˆ’1)n(2n+1)!x4n+2\sum_{n=0}^{\infty} \frac{(-1)^n}{(2n+1)!} x^{4n+2}" hint="Recall the Maclaurin series for sin⁑u\sin u and substitute u=x2u=x^2." solution="The Maclaurin series for sin⁑u\sin u is given by βˆ‘n=0∞(βˆ’1)n(2n+1)!u2n+1\sum_{n=0}^{\infty} \frac{(-1)^n}{(2n+1)!} u^{2n+1}.
Substituting u=x2u = x^2, we get:

f(x)=sin⁑(x2)=βˆ‘n=0∞(βˆ’1)n(2n+1)!(x2)2n+1=βˆ‘n=0∞(βˆ’1)n(2n+1)!x4n+2f(x) = \sin(x^2) = \sum_{n=0}^{\infty} \frac{(-1)^n}{(2n+1)!} (x^2)^{2n+1} = \sum_{n=0}^{\infty} \frac{(-1)^n}{(2n+1)!} x^{4n+2}

Answer: \boxed{\sum_{n=0}^{\infty} \frac{(-1)^n}{(2n+1)!} x^{4n+2}}}"
:::

:::question type="NAT" question="If f(x)=βˆ‘n=0∞xnn!f(x) = \sum_{n=0}^{\infty} \frac{x^n}{n!} for all x∈Rx \in \mathbb{R}, what is fβ€²(1)f'(1)?" answer="2.71828" hint="Identify the function represented by the power series and then differentiate." solution="The given power series is the Maclaurin series for exe^x, so f(x)=exf(x) = e^x.
Differentiating term-by-term:

fβ€²(x)=ddx(βˆ‘n=0∞xnn!)=βˆ‘n=1∞nxnβˆ’1n!=βˆ‘n=1∞xnβˆ’1(nβˆ’1)!f'(x) = \frac{d}{dx} \left( \sum_{n=0}^{\infty} \frac{x^n}{n!} \right) = \sum_{n=1}^{\infty} \frac{n x^{n-1}}{n!} = \sum_{n=1}^{\infty} \frac{x^{n-1}}{(n-1)!}

Let k=nβˆ’1k = n-1. Then
fβ€²(x)=βˆ‘k=0∞xkk!=exf'(x) = \sum_{k=0}^{\infty} \frac{x^k}{k!} = e^x

Therefore,
fβ€²(1)=e1=eβ‰ˆ2.71828f'(1) = e^1 = e \approx 2.71828

Answer: \boxed{2.71828}"
:::

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What's Next?

πŸ’‘ Continue Your CUET PG Journey

This chapter on Power Series is foundational for several advanced topics in Real Analysis. A solid understanding here is crucial for studying Uniform Convergence of Sequences and Series of Functions, where the concept of convergence across an interval is generalized. Furthermore, Power Series serve as the bedrock for defining and analyzing analytic functions, a central theme in Complex Analysis. Mastery of these concepts will significantly aid in understanding more complex functional transformations and representations.

🎯 Key Points to Remember

  • βœ“ Master the core concepts in Power Series before moving to advanced topics
  • βœ“ Practice with previous year questions to understand exam patterns
  • βœ“ Review short notes regularly for quick revision before exams

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