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Contour integral

From Simple English Wikipedia, the free encyclopedia

In complex analysis, contour integration is a way to calculate an integral around a contour on the complex plane. In other words, it is a way of integrating along the complex plane.

More specifically, given a complex-valued function f and a contour C, the contour integral of f along C is written as ∫Cf(z)dz or ∮Cf(z)dz.[1][2]

Calculating contour integrals with the residue theorem

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For a standard contour integral, we can evaluate it by using the residue theorem. This theorem states that

∮Cf(z)dz=2πi⋅Resf(z)

where Res is the residue of the function f(z), C is the contour located on the complex plane. Here, f(z) is the integrand of the function, or part of the integral to be integrated. A residue of order p is defined as follows Res⁡(f,c)=1(p−1)!limz→cdp−1dzp−1((z−c)pf(z)).

The following examples illustrate how contour integrals can be calculated using the residue theorem. The following two examples have a residue of order p=3 where c=0, i.e., Res(f,0)=12!limz→0d2dz2[z3f(z)]


Example 1

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∮Cezz3dz=2πi⋅Res(ezz3)=2πi⋅12=πi

Example 2

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∮C1z3dz=2πiResf(z)=2πiRes1z3=2πi⋅0=0

Multivariable contour integrals

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To solve multivariable contour integrals (contour integrals on functions of several variables), such as surface integrals, complex volume integrals and higher order integrals, we must use the divergence theorem. For right now, let ∇ be interchangeable with Div. These will both serve as the divergence of the vector field written as 𝐅. This theorem states that:

∫⋯∫U⏟nDiv(𝐅)dV=∮⋯∮∂U⏟n−1𝐅⋅𝐧dS

In addition, we also need to evaluate ∇⋅𝐅, where ∇⋅𝐅 is an alternate notation of div𝐅. [1]The divergence of any dimension can be described as

Div⁡𝐅=∇⋅𝐅=(∂∂u,∂∂x,∂∂y,∂∂z,⋯)⋅(Fu,Fx,Fy,Fz⋯)=(∂Fu∂u+∂Fx∂x+∂Fy∂y+∂Fz∂z⋯)

The following examples illustrate the use of divergence theorem in the calculation of multivariate contour integrals.

Example 1

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Let the vector field 𝐅=sin⁡(2x)+sin⁡(2y)+sin⁡(2z) be bounded by the following conditions

0≤x≤10≤y≤3π−1≤z≤4

The corresponding double contour integral would be set up as such:

\oiiintS 𝐅⋅ndS

We now evaluate ∇⋅𝐅 by setting up the corresponding triple integral:

=∭V(∂Fx∂x+∂Fy∂y+∂Fz∂z)dV=∭V(∂sin⁡(2x)∂x+∂sin⁡(2y)∂y+∂sin⁡(2z)∂z)dV=∭V=2(cos⁡(2x)+cos⁡(2y)+cos⁡(2z))dV

From this, we can now evaluate the integral as follows:

∫01∫03∫−142(cos⁡(2x)+cos⁡(2y)+cos⁡(2z))dxdydz=∫01∫03(10cos⁡(2y)+sin⁡(8)+sin⁡(2)+10cos⁡(z))dydz=∫01(30cos⁡(2z)+3sin⁡(2)+3sin⁡(8)+5sin⁡(6))dz=18sin⁡(2)+3sin⁡(8)+5sin⁡(6)

Example 2

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Given the vector field 𝐅=u4+x5+y6+z−3 and n being the fourth dimension. Let this vector field be bounded by the following:

0≤x≤1−10≤y≤2π4≤z≤5−1≤u≤3

To evaluate this, we use the divergence theorem as stated before, and evaluate ∇⋅𝐅 afterwards. Let dV=dxdydzdu, then:

\oiintS 𝐅⋅nd𝐒
=⨌V(∂Fu∂u+∂Fx∂x+∂Fy∂y+∂Fz∂z)dV=⨌V(∂u4∂u+∂x5∂x+∂y6∂y+∂z−3∂z)dV=⨌V4u3z4+5x4z4+5y4z4−3z4dV

From this, we now can evaluate the integral:

⨌V4u3z4+5x4z4+5y4z4−3z4dV=∫01∫−102π∫45∫−134u3z4+5x4z4+5y4z4−3z4dV=∫01∫−102π∫45(4(3u4z3+3y6+91z3+3)3z3)dydzdu=∫01∫−102π(4u4+74344021+4z3)dzdu=∫01(−12π2+1486880π21+8πu4+40u4+3717200211050)du=3717284211050+14869136π3−105210π2≈576468.77

Thus, we can evaluate a contour integral of the fourth dimension.

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References

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  1. 1 2 "List of Calculus and Analysis Symbols". Math Vault. 2020-05-11. Retrieved 2020-09-18.
  2. ↑ "Contour Integration | Brilliant Math & Science Wiki". brilliant.org. Retrieved 2020-09-18.