Evaluating a Contour Integral of log(z) | Explaining Branch Cuts

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The integral of log(z) over a simple closed contour encircling the origin is influenced by branch cuts, particularly when the cut is along the negative real axis. When integrating across a branch cut, the integral can yield different values due to the addition of multiples of 2πi, reflecting the discontinuity in the logarithm's values. The expression for log(z) can be represented as ln(r) + iφ, where φ varies based on the contour's path. As a result, the integral simplifies to ∫(ln(R) + iφ)dφ, with limits from 0 to 2π. Understanding these concepts is essential for correctly evaluating such integrals.
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Is it possible to evaluate the integral of log(z) taken over any simple closed contour encircling the origin? I don't fully understand how singularities on branch cuts should be treated when integrating over contours encircling such singularities. Are residues applied? Can someone explain this to me? Thanks!
 
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Looking at your specific example, ln(z), by convention we take the branch cut along the negative real axis or \theta= \pi when z= re^{i\theta}[/tex]. And, of course, ln(z)= ln(r)+ i\theta. So integrating across a branch cut results in adding 2\pi n ifor <b>some</b> integer n. That is the difficulty with integrating over branch cuts- the integral value jumps by some multiple of a constant.
 
If you put z = r*(cos(φ) + i*sin(φ)), log(z) = ln(r) + i*φ (since both sine and cosine are periodic with period 2π, there are several values of φ we can use in the expression).

Thus ∫log(z) for |z|=R, is equivalent to ∫(ln(R) +i*φ)dφ where the integration limits are 0 and 2π. The rest is left as an exercise for the student...
 

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