Problem 24
Question
Determine the order of the poles for the given function. $$ f(z)=\frac{e^{z}-1}{z^{2}} $$
Step-by-Step Solution
Verified Answer
The function has a simple pole of order 1 at \( z = 0 \).
1Step 1: Understand the Expression
We need to determine the order of the poles for the function \( f(z) = \frac{e^z - 1}{z^2} \). A pole is a point at which a function goes to infinity.
2Step 2: Identify the Problematic Point
Examine the denominator, \( z^2 \). There is a potential pole at \( z = 0 \) because the denominator becomes zero, making the function undefined.
3Step 3: Analyze the Numerator
The numerator is \( e^z - 1 \). The Taylor series expansion for \( e^z \) around \( z = 0 \) is \( e^z = 1 + z + \frac{z^2}{2} + \cdots \). Thus, \( e^z - 1 = z + \frac{z^2}{2} + \cdots \), which simplifies to \( z(1 + \frac{z}{2} + \cdots) \).
4Step 4: Determine the Order of the Pole
Rewrite the function using the expansion obtained. Substitute the expansion of the numerator into the function: \( f(z) = \frac{z(1 + \frac{z}{2} + \cdots)}{z^2} = \frac{1 + \frac{z}{2} + \cdots}{z} \). We see that the smallest power of \( z \) in the denominator is larger than the smallest power of \( z \) in the numerator, confirming the presence of a pole at \( z = 0 \).
5Step 5: Compute the Order
The restructured function \( \frac{1 + \frac{z}{2} + \cdots}{z} \) shows that as \( z \to 0 \), the term \( \frac{1}{z} \) dominates. Since this term is the only one causing \( f(z) \to \infty \) at \( z = 0 \), the order of the pole is \( 1 \).
Key Concepts
Poles of a functionOrder of polesTaylor series expansion
Poles of a function
When studying complex functions, understanding the concept of poles is essential. A pole is a specific type of singularity where a function's value approaches infinity. Consider a function like \( f(z) \). If at a point \( z = z_0 \) there is a pole, then the function becomes undefined because the denominator of a fraction tends to zero.
To locate poles, follow these steps:
For example, consider the function \( f(z) = \frac{e^z - 1}{z^2} \). We see a potential problem point at \( z = 0 \) because plugging zero into \( z^2 \) in the denominator yields an undefined expression. This indicates a pole at \( z = 0 \).
To locate poles, follow these steps:
- Identify the points where the denominator equals zero.
- Analyze the numerator to see if these points cause indeterminate forms like \( \frac{0}{0} \).
For example, consider the function \( f(z) = \frac{e^z - 1}{z^2} \). We see a potential problem point at \( z = 0 \) because plugging zero into \( z^2 \) in the denominator yields an undefined expression. This indicates a pole at \( z = 0 \).
Order of poles
Not only is it crucial to identify a pole, but understanding its order deepens our analysis. The order of a pole gives us information about how rapidly a function approaches infinity near that point.
To find the order of a pole:
The smallest power of \( z \) here is in the denominator. Thus, this function has a dominant \( \frac{1}{z} \) term, confirming that the pole at \( z = 0 \) is of order 1.
To find the order of a pole:
- Conduct a factor analysis of the numerator and denominator around the pole.
- The order is the difference in the power of \( z \) in the denominator minus the power in the numerator.
The smallest power of \( z \) here is in the denominator. Thus, this function has a dominant \( \frac{1}{z} \) term, confirming that the pole at \( z = 0 \) is of order 1.
Taylor series expansion
The Taylor series is a powerful tool in complex analysis that allows us to approximate functions near a given point. It expresses a function as an infinite sum of terms calculated from the function's derivatives at a certain point.
The Taylor series expansion around \( z = 0 \) (also called a Maclaurin series) for the exponential function \( e^z \) is:\[e^z = 1 + z + \frac{z^2}{2!} + \frac{z^3}{3!} + \cdots\]This series allows us to approximate \( e^z - 1 \) as \( z + \frac{z^2}{2} + \cdots \).
This expansion is crucial when evaluating expressions like \( \frac{e^z - 1}{z^2} \). When simplifying, it helps to isolate the lowest power of \( z \) in the numerator, ensuring that calculations of poles and their orders are accurate. Thus, Taylor expansions provide clarity by rewriting functions in a manageable form that identifies both the effects of singularities and convergence behavior near those points.
The Taylor series expansion around \( z = 0 \) (also called a Maclaurin series) for the exponential function \( e^z \) is:\[e^z = 1 + z + \frac{z^2}{2!} + \frac{z^3}{3!} + \cdots\]This series allows us to approximate \( e^z - 1 \) as \( z + \frac{z^2}{2} + \cdots \).
This expansion is crucial when evaluating expressions like \( \frac{e^z - 1}{z^2} \). When simplifying, it helps to isolate the lowest power of \( z \) in the numerator, ensuring that calculations of poles and their orders are accurate. Thus, Taylor expansions provide clarity by rewriting functions in a manageable form that identifies both the effects of singularities and convergence behavior near those points.
Other exercises in this chapter
Problem 23
Find the circle and radius of convergence of the given power series. $$ \sum_{k=1}^{\infty} \frac{(-1)^{k}}{k 2^{k}}(z-1-i)^{k} $$
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Evaluate the Cauchy principal value of the given improper integral. $$ \int_{0}^{\infty} \frac{1}{x^{6}+1} d x $$
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Use Cauchy's residue theorem to evaluate the given integral along the indicated contour. $$ \oint_{C} \frac{z}{(z+1)\left(z^{2}+1\right)} d z, C: 16 x^{2}+y^{2}
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Expand \(f(z)=\frac{1}{(z-2)(z-1)^{3}}\) in a Laurent series valid for the given annular domain. $$ 0
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