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Develop the Taylor expansion of \(\ln (1+z)\). $$ \text { ANS. } \sum_{n=1}^{\infty}(-1)^{n-1} \frac{z^{n}}{n} \text { . } $$

Short Answer

Expert verified
The Taylor expansion of \( \ln(1+z) \) is \( \sum_{n=1}^{\infty}(-1)^{n-1} \frac{z^n}{n} \).

Step by step solution

01

Recall the Taylor Series Formula

The general Taylor series expansion of a function \( f(z) \) around \( z=a \) is given by:\[ f(z) = f(a) + f'(a)(z-a) + \frac{f''(a)}{2!}(z-a)^2 + \frac{f'''(a)}{3!}(z-a)^3 + \ldots\]For the function \( \ln(1+z) \), we expand around \( z=0 \), which means \( a=0 \).
02

Compute the Function and its Derivatives

For \( f(z) = \ln(1+z) \):\[-\ f(0) = \ln(1) = 0. \]\[-\ f'(z) = \frac{1}{1+z}, \quad f'(0) = 1. \]\[-\ f''(z) = -\frac{1}{(1+z)^2}, \quad f''(0) = -1. \]\[-\ f'''(z) = \frac{2}{(1+z)^3}, \quad f'''(0) = 2.\]Continue this pattern to find higher derivatives at \( z=0 \).
03

Substitute Derivatives into the Taylor Series Formula

Using the derivatives computed in Step 2, substitute into the Taylor series formula:\[ \ln(1+z) = 0 + 1 \cdot z - \frac{1}{2!}z^2 + \frac{2}{3!}z^3 - \frac{6}{4!}z^4 + \ldots \]This simplifies to:\[ \ln(1+z) = z - \frac{z^2}{2} + \frac{z^3}{3} - \frac{z^4}{4} + \ldots \]
04

Identify the Pattern

The coefficients of the series reveal a pattern:Each term has the form \((-1)^{n-1}\frac{z^n}{n}\) which alternates based on the power of \(-1\) and uses the harmonic numbers as denominators. Thus, the Taylor series expansion for \( \ln(1+z) \) is:\[ \ln(1+z) = \sum_{n=1}^{\infty}(-1)^{n-1} \frac{z^n}{n} \]

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Logarithmic Function
Understanding the nature of the logarithmic function is crucial when diving into series expansions, especially when dealing with functions like \( \ln(1+z) \). The natural logarithm, \( \ln(x) \), is fundamentally the inverse of the exponential function \( e^x \). For \( \ln(1+z) \), the domain is all real numbers \( z > -1 \).The function helps in various real-world applications, like computing interests and growth rates. It's important to note that around \( z = 0 \), \( \ln(1+z) \) can be approximated very well using a series expansion. That is precisely what the Taylor series aims to represent: an approximate polynomial near the initial point of expansion. Through repeated derivatives, this function can be expressed as a summation of its polynomial approximations.
Series Expansion
The Taylor series expansion provides a way to approximate functions using an infinite series of terms calculated from the values of its derivatives at a single point. For \( \ln(1+z) \), expanding around \( z = 0 \), allows us to express the logarithmic function as:\[ \ln(1+z) = z - \frac{z^2}{2} + \frac{z^3}{3} - \frac{z^4}{4} + \ldots \] In this series, every term calculated gets successively smaller when \( |z| < 1 \), making the series converge to the function as more terms are added.
  • Each coefficient is derived from the derivatives of the function.
  • The contributions of higher powers of \( z \) become less significant for small \( |z| \).
  • The alternating signs arise from the properties of the logarithmic function's derivatives.
Understanding the pattern in these expansions helps tremendously in predicting higher terms without recalculating derivatives.
Derivatives
In the context of finding a Taylor series, derivatives are used to understand the behavior of a function around a point. For the function \( \ln(1+z) \):
  • The first derivative, \( \frac{1}{1+z} \), transforms into \( 1 \) at \( z = 0 \).
  • The second derivative, \( -\frac{1}{(1+z)^2} \), simplifies to \(-1\).
  • This pattern continues, where each derivative modifies the function's slope.
Computing these derivatives gives insight into how the function changes and provides the coefficients for the Taylor series. Each derivative has a crucial role in constructing the polynomial terms:- **First derivative** affects the linear term.- **Second derivative** influences the quadratic term.- Higher terms are adjusted by subsequent derivatives.Recognizing this iterative process allows for systematic expansion, capturing more details about \( \ln(1+z) \) with each derivative considered.
Mathematical Pattern Recognition
Identifying patterns within the terms of a series can amplify understanding and predictive abilities in mathematics. By examining the Taylor series for \( \ln(1+z) \):
  • We see a clear (-1)^{n-1} pattern, making the terms alternate in sign.
  • The numerator follows the power sequence of \( z^n \).
  • Denominators are defined by the harmonic numbers \( n \).
By recognizing that the Taylor series for \( \ln(1+z) \) indeed follows the pattern:\[ \ln(1+z) = \sum_{n=1}^{\infty}(-1)^{n-1} \frac{z^n}{n} \]You can predict future terms without recalculating each derivative separately. This predictable pattern highlights the beauty of mathematics—transforming complex expressions into manageable series. Acknowledging such patterns aids in efficient calculation, comprehension, and appreciation of mathematical beauty in functions.

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Most popular questions from this chapter

How do circles centered on the origin in the \(z\) -plane transform for (a) \(w_{1}(z)=z+\frac{1}{2}\), (b) \(w_{2}(z)=z-\frac{1}{z}, \quad\) for \(z \neq 0 ?\) What happens when \(|z| \rightarrow 1\) ?

Using the identities $$ \cos z=\frac{e^{i z}+e^{-i z}}{2}, \quad \sin z=\frac{e^{i z}-e^{-i z}}{2 i} $$ established from comparison of power series, show that(a) \(\sin (x+i y)=\sin x \cosh y+i \cos x \sinh y\), \(\cos (x+i y)=\cos x \cosh y-i \sin x \sinh y\) (b) \(|\sin z|^{2}=\sin ^{2} x+\sinh ^{2} y, \quad|\cos z|^{2}=\cos ^{2} x+\sinh ^{2} y .\) This demonstrates that we may have \(|\sin z|,|\cos z|>\mid\) in the complex plane.

Having shown that the real part \(u(x, y)\) and the imaginary part \(v(x, y)\) of an analytic function \(w(z)\) each satisfy Laplace's equation, show that \(u(x, y)\) and \(v(x, y)\) cannot have either a maximum or a minimum in the interior of any region in which \(w(z)\) is analytic. (They can have saddle points.)

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Two-dimensional irrotational fluid flow is conveniently described by a complex potential \(f(z)=u(x, v)+i v(x, y)\). We label the real part \(u(x, y)\) the velocity potential, and the imaginary part \(v(x, y)\) the stream function. The fluid velocity \(\mathbf{V}\) is given by \(\mathbf{V}=\nabla u\). If \(f(z)\) is analytic, (a) Show that \(d f / d z=V_{x}-i V_{y}\); (b) Show that \(\nabla \cdot \mathbf{V}=0\) (no sources or sinks); (c) Show that \(\nabla \times \mathbf{V}=0\) (irrotational, nonturbulent flow).

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