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๐Ÿ“Complex Analysis Unit 6 Review

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6.5 Residues

6.5 Residues

Written by the Fiveable Content Team โ€ข Last updated August 2025
Written by the Fiveable Content Team โ€ข Last updated August 2025
๐Ÿ“Complex Analysis
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Residues are powerful tools in complex analysis, helping us evaluate tricky integrals. They're the secret sauce in the Laurent series expansion of functions with singularities. By finding residues, we can tackle complex contour integrals that seemed impossible before.

The residue theorem connects the dots between singularities and contour integrals. It's like a cheat code for solving real-world problems in physics and engineering. Mastering residues opens up a whole new world of problem-solving techniques in complex analysis.

Residues of functions

Definition and properties of residues

  • The residue of a function f(z)f(z) at an isolated singular point z0z_0 is the coefficient aโˆ’1a_{-1} of the term (zโˆ’z0)โˆ’1(z-z_0)^{-1} in the Laurent series expansion of f(z)f(z) about z0z_0
  • Residues are only defined for isolated singular points, which can be poles (of any order) or essential singularities
    • Poles are characterized by a finite number of negative power terms in the Laurent series expansion
    • Essential singularities have an infinite number of negative power terms in the Laurent series expansion
  • The residue is independent of the choice of contour around the singular point, as long as the contour encloses no other singularities
    • This property allows for flexibility in choosing contours when applying the residue theorem
  • Residues can be used to evaluate complex contour integrals and real integrals using the residue theorem
    • The residue theorem relates the sum of residues within a contour to the value of the contour integral

Types of isolated singular points

  • Simple poles (poles of order 1)
    • A simple pole occurs when the Laurent series expansion has only one negative power term, (zโˆ’z0)โˆ’1(z-z_0)^{-1}
    • The residue at a simple pole can be calculated using the limit: Res(f,z0)=limโกzโ†’z0[(zโˆ’z0)f(z)]\text{Res}(f,z_0) = \lim_{z\to z_0}[(z-z_0)f(z)]
  • Poles of order mm
    • A pole of order mm occurs when the Laurent series expansion has mm negative power terms, up to (zโˆ’z0)โˆ’m(z-z_0)^{-m}
    • The residue at a pole of order mm can be calculated using the formula: Res(f,z0)=1(mโˆ’1)!limโกzโ†’z0dmโˆ’1dzmโˆ’1[(zโˆ’z0)mf(z)]\text{Res}(f,z_0) = \frac{1}{(m-1)!} \lim_{z\to z_0}\frac{d^{m-1}}{dz^{m-1}}[(z-z_0)^m f(z)]
  • Essential singularities
    • An essential singularity occurs when the Laurent series expansion has an infinite number of negative power terms
    • The residue at an essential singularity must be determined from the Laurent series expansion by identifying the aโˆ’1a_{-1} coefficient

Calculating residues with Laurent series

Definition and properties of residues, complex analysis - Laurent Series and Taylor Expansion of $ 1 / (e^z - 1) $ - Mathematics Stack ...

Expanding functions as Laurent series

  • To find the residue at a singular point z0z_0, expand the function f(z)f(z) as a Laurent series centered at z0z_0
    • The Laurent series expansion is of the form: f(z)=โˆ‘n=โˆ’โˆžโˆžan(zโˆ’z0)nf(z) = \sum_{n=-\infty}^{\infty} a_n(z-z_0)^n
    • The coefficients ana_n can be determined using the formula: an=12ฯ€iโˆฎCf(z)(zโˆ’z0)n+1dza_n = \frac{1}{2\pi i} \oint_C \frac{f(z)}{(z-z_0)^{n+1}}dz, where CC is a contour enclosing z0z_0
  • Identify the coefficient aโˆ’1a_{-1} of the term (zโˆ’z0)โˆ’1(z-z_0)^{-1} in the Laurent series expansion
    • The coefficient aโˆ’1a_{-1} is the residue of f(z)f(z) at z0z_0
    • For a simple pole, aโˆ’1a_{-1} can be found using the limit formula: Res(f,z0)=limโกzโ†’z0[(zโˆ’z0)f(z)]\text{Res}(f,z_0) = \lim_{z\to z_0}[(z-z_0)f(z)]

Calculating residues at poles and essential singularities

  • For a pole of order mm, use the formula: Res(f,z0)=1(mโˆ’1)!limโกzโ†’z0dmโˆ’1dzmโˆ’1[(zโˆ’z0)mf(z)]\text{Res}(f,z_0) = \frac{1}{(m-1)!} \lim_{z\to z_0}\frac{d^{m-1}}{dz^{m-1}}[(z-z_0)^m f(z)]
    • This formula involves taking the (mโˆ’1)(m-1)-th derivative of (zโˆ’z0)mf(z)(z-z_0)^m f(z) and evaluating the limit as zz approaches z0z_0
    • Example: For f(z)=1(zโˆ’1)2(z+1)f(z) = \frac{1}{(z-1)^2(z+1)} at z0=1z_0=1, Res(f,1)=limโกzโ†’1ddz[(zโˆ’1)21(zโˆ’1)2(z+1)]=limโกzโ†’11z+1=12\text{Res}(f,1) = \lim_{z\to 1}\frac{d}{dz}[(z-1)^2 \frac{1}{(z-1)^2(z+1)}] = \lim_{z\to 1}\frac{1}{z+1} = \frac{1}{2}
  • For an essential singularity, determine the residue from the Laurent series expansion by identifying the aโˆ’1a_{-1} coefficient
    • Example: For f(z)=e1zf(z) = e^{\frac{1}{z}} at z0=0z_0=0, the Laurent series expansion is f(z)=1+1z+12!z2+13!z3+โ‹ฏf(z) = 1 + \frac{1}{z} + \frac{1}{2!z^2} + \frac{1}{3!z^3} + \cdots, so the residue is aโˆ’1=1a_{-1} = 1

Evaluating integrals with the residue theorem

Definition and properties of residues, complex analysis - Contour integration of $\frac{(\ln z)^2}{z^2+1} $ - Mathematics Stack Exchange

Statement and conditions of the residue theorem

  • The residue theorem states that for a meromorphic function f(z)f(z) and a simple closed contour CC enclosing isolated singular points z1,z2,โ€ฆ,znz_1, z_2, \ldots, z_n, the contour integral โˆฎCf(z)dz\oint_C f(z)dz equals 2ฯ€i2\pi i times the sum of the residues of f(z)f(z) at those singular points
    • In mathematical notation: โˆฎCf(z)dz=2ฯ€iโˆ‘k=1nRes(f,zk)\oint_C f(z)dz = 2\pi i \sum_{k=1}^{n} \text{Res}(f,z_k)
  • The contour CC must be simple (non-self-intersecting) and closed
    • The contour can be a circle, a rectangle, or any other simple closed curve
  • The function f(z)f(z) must be meromorphic (analytic except for isolated poles) within and on the contour
    • The residue theorem does not apply to functions with branch cuts or other non-isolated singularities within the contour

Applying the residue theorem to contour integrals

  • To apply the residue theorem, follow these steps:
    1. Identify the isolated singular points within the contour
    2. Calculate the residues at each singular point using the appropriate method (limit formula for simple poles, derivative formula for higher-order poles, or Laurent series for essential singularities)
    3. Sum the residues multiplied by 2ฯ€i2\pi i to obtain the value of the contour integral
  • Example: Evaluate โˆฎC1z(zโˆ’1)dz\oint_C \frac{1}{z(z-1)}dz, where CC is the circle โˆฃzโˆฃ=2|z|=2
    1. The isolated singular points within the contour are z1=0z_1=0 and z2=1z_2=1
    2. Res(f,0)=limโกzโ†’0[z1z(zโˆ’1)]=1\text{Res}(f,0) = \lim_{z\to 0}[z \frac{1}{z(z-1)}] = 1 and Res(f,1)=limโกzโ†’1[(zโˆ’1)1z(zโˆ’1)]=โˆ’1\text{Res}(f,1) = \lim_{z\to 1}[(z-1) \frac{1}{z(z-1)}] = -1
    3. โˆฎC1z(zโˆ’1)dz=2ฯ€i(Res(f,0)+Res(f,1))=2ฯ€i(1โˆ’1)=0\oint_C \frac{1}{z(z-1)}dz = 2\pi i (\text{Res}(f,0) + \text{Res}(f,1)) = 2\pi i (1 - 1) = 0

Residue theorem applications for contour and real integrals

Evaluating real integrals using the residue theorem

  • Real integrals of the form โˆซโˆ’โˆžโˆžR(x)dx\int_{-\infty}^{\infty} R(x)dx, where R(x)R(x) is a rational function, can be evaluated using the residue theorem by considering a complex contour integral and applying the theorem
  • To evaluate real integrals using the residue theorem:
    1. Express the real integral as a complex contour integral by extending the integrand into the complex plane
    2. Choose an appropriate contour (e.g., a semicircle in the upper or lower half-plane) that encloses the poles of the integrand and avoids branch cuts, if present
    3. Apply the residue theorem to the contour integral, calculating the residues at the enclosed poles
    4. Relate the contour integral to the original real integral using techniques such as the Cauchy principal value or by considering the limit as the radius of the contour approaches infinity
  • Example: Evaluate โˆซโˆ’โˆžโˆž1x2+1dx\int_{-\infty}^{\infty} \frac{1}{x^2+1}dx
    1. Express the integral as a contour integral: โˆฎC1z2+1dz\oint_C \frac{1}{z^2+1}dz, where CC is a semicircle in the upper half-plane with radius Rโ†’โˆžR\to\infty
    2. The contour encloses a single pole at z=iz=i
    3. Res(f,i)=limโกzโ†’i[(zโˆ’i)1z2+1]=12i\text{Res}(f,i) = \lim_{z\to i}[(z-i) \frac{1}{z^2+1}] = \frac{1}{2i}, so โˆฎC1z2+1dz=2ฯ€iRes(f,i)=ฯ€\oint_C \frac{1}{z^2+1}dz = 2\pi i \text{Res}(f,i) = \pi
    4. As Rโ†’โˆžR\to\infty, the integral along the circular arc vanishes, and the contour integral equals twice the real integral, so โˆซโˆ’โˆžโˆž1x2+1dx=12โˆฎC1z2+1dz=ฯ€2\int_{-\infty}^{\infty} \frac{1}{x^2+1}dx = \frac{1}{2}\oint_C \frac{1}{z^2+1}dz = \frac{\pi}{2}

Other applications of the residue theorem

  • The residue theorem can also be used to evaluate integrals involving trigonometric functions, logarithms, and other transcendental functions by expressing them in terms of complex exponentials and applying the theorem
    • Example: Evaluate โˆซ02ฯ€dฮธa+cosโกฮธ\int_0^{2\pi} \frac{d\theta}{a+\cos\theta}, where a>1a>1
      1. Express the integral in terms of complex exponentials: โˆซC1a+12(z+1z)dziz\int_C \frac{1}{a+\frac{1}{2}(z+\frac{1}{z})} \frac{dz}{iz}, where CC is the unit circle
      2. The integrand has simple poles at z=aยฑa2โˆ’1z=a\pm\sqrt{a^2-1}, but only z1=aโˆ’a2โˆ’1z_1=a-\sqrt{a^2-1} lies within the unit circle
      3. Res(f,z1)=1ia2โˆ’1\text{Res}(f,z_1) = \frac{1}{i\sqrt{a^2-1}}, so โˆซC1a+12(z+1z)dziz=2ฯ€iRes(f,z1)=2ฯ€a2โˆ’1\int_C \frac{1}{a+\frac{1}{2}(z+\frac{1}{z})} \frac{dz}{iz} = 2\pi i \text{Res}(f,z_1) = \frac{2\pi}{\sqrt{a^2-1}}
      4. The contour integral equals the original real integral, so โˆซ02ฯ€dฮธa+cosโกฮธ=2ฯ€a2โˆ’1\int_0^{2\pi} \frac{d\theta}{a+\cos\theta} = \frac{2\pi}{\sqrt{a^2-1}}
  • Contour integration using the residue theorem can be applied to solve problems in various fields, such as physics, engineering, and applied mathematics
    • Examples include calculating Fourier transforms, solving differential equations, and evaluating improper integrals arising in quantum mechanics and fluid dynamics