Residue theorem: understood it intuitively but cannot prove mathematically

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In my opinion, residue theorem’s underlying principle is quite beautiful: one decomposes a contour integral into infinitely many small circular contour integrals around every point, and most of them are zero, except a few that encircle singularities. Those are called residues, and add them up. This is basically how residue theorem works.



However, when I try to prove it by Green’s theorem, I face some difficulties. ($f=u+iv$)



$$oint_C f(z)dz=oint(u+iv)dx+i(u+iv)dy=iint_D fracpartial (u+iv)partial x-ifracpartial (u+iv)partial ydxdy$$



I don’t see how can this be transformed into a sum of residues/circular contour integrals around singularities.



Can you please show how?



Thanks in advance.







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    In my opinion, residue theorem’s underlying principle is quite beautiful: one decomposes a contour integral into infinitely many small circular contour integrals around every point, and most of them are zero, except a few that encircle singularities. Those are called residues, and add them up. This is basically how residue theorem works.



    However, when I try to prove it by Green’s theorem, I face some difficulties. ($f=u+iv$)



    $$oint_C f(z)dz=oint(u+iv)dx+i(u+iv)dy=iint_D fracpartial (u+iv)partial x-ifracpartial (u+iv)partial ydxdy$$



    I don’t see how can this be transformed into a sum of residues/circular contour integrals around singularities.



    Can you please show how?



    Thanks in advance.







    share|cite|improve this question





















      up vote
      1
      down vote

      favorite









      up vote
      1
      down vote

      favorite











      In my opinion, residue theorem’s underlying principle is quite beautiful: one decomposes a contour integral into infinitely many small circular contour integrals around every point, and most of them are zero, except a few that encircle singularities. Those are called residues, and add them up. This is basically how residue theorem works.



      However, when I try to prove it by Green’s theorem, I face some difficulties. ($f=u+iv$)



      $$oint_C f(z)dz=oint(u+iv)dx+i(u+iv)dy=iint_D fracpartial (u+iv)partial x-ifracpartial (u+iv)partial ydxdy$$



      I don’t see how can this be transformed into a sum of residues/circular contour integrals around singularities.



      Can you please show how?



      Thanks in advance.







      share|cite|improve this question











      In my opinion, residue theorem’s underlying principle is quite beautiful: one decomposes a contour integral into infinitely many small circular contour integrals around every point, and most of them are zero, except a few that encircle singularities. Those are called residues, and add them up. This is basically how residue theorem works.



      However, when I try to prove it by Green’s theorem, I face some difficulties. ($f=u+iv$)



      $$oint_C f(z)dz=oint(u+iv)dx+i(u+iv)dy=iint_D fracpartial (u+iv)partial x-ifracpartial (u+iv)partial ydxdy$$



      I don’t see how can this be transformed into a sum of residues/circular contour integrals around singularities.



      Can you please show how?



      Thanks in advance.









      share|cite|improve this question










      share|cite|improve this question




      share|cite|improve this question









      asked Jul 25 at 3:47









      Szeto

      4,0931521




      4,0931521




















          1 Answer
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          You are given a region $Omegasubsetmathbb C$ with boundary cycle $partialOmega$ and a function $f:>Omegatomathbb C$ which is analytic apart from finitely many isolated singularities at the points $a_jinOmega$ $(1leq jleq m)$. The trick now is to draw tiny discs $B_j$ of radius $epsilon>0$ centered at these points. Then we consider the punched domain $Omega':=Omegasetminusbigcup_j=1^m B_j$ with boundary cycle
          $$partialOmega'=partialOmega-sum_j=1^m partial B_j .$$
          Note the minus signs here! The function $f$ is analytic in $Omega'$; therefore we may apply Green's, resp., Cauchy's, theorem to $f$ and $Omega'$. It follows that $int_partialOmega'f(z)>dz=0$, so that
          $$int_partialOmegaf(z)>dz=sum_j=1^mint_partial B_jf(z)>dz .$$
          Here the LHS is independent of $epsilon$. It follows that
          $$int_partialOmegaf(z)>dz=sum_j=1^mlim_epsilonto0int_partial B_jf(z)>dz=2pi i sum_j=1^mrm res(f, a_j) ,$$
          by definition of the residue.






          share|cite|improve this answer





















          • This is brilliant. Just one thing: how can I derive with details and rigor that $$int_partialOmega+partial B=int_partialOmega+int_partial B$$ to ‘convince’ a starter in complex analysis? (I know this is almost trivial to you.)
            – Szeto
            Jul 25 at 13:59











          • Also, to my surprise, I cannot google a similar proof. Indeed, a formal proof of residue theorem is quite rare on the internet.
            – Szeto
            Jul 25 at 14:02










          • Already $partialOmega$ might consist of several disjoint closed curves. If you accept the notion of boundary cycle as defined in your community, as well as the notion of integral over a chain (formal sum of smooth curves) then there is no problem with $partialOmega'=partialOmega-sum_jpartial B_j$.
            – Christian Blatter
            Jul 25 at 14:10










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          1 Answer
          1






          active

          oldest

          votes








          1 Answer
          1






          active

          oldest

          votes









          active

          oldest

          votes






          active

          oldest

          votes








          up vote
          3
          down vote



          accepted










          You are given a region $Omegasubsetmathbb C$ with boundary cycle $partialOmega$ and a function $f:>Omegatomathbb C$ which is analytic apart from finitely many isolated singularities at the points $a_jinOmega$ $(1leq jleq m)$. The trick now is to draw tiny discs $B_j$ of radius $epsilon>0$ centered at these points. Then we consider the punched domain $Omega':=Omegasetminusbigcup_j=1^m B_j$ with boundary cycle
          $$partialOmega'=partialOmega-sum_j=1^m partial B_j .$$
          Note the minus signs here! The function $f$ is analytic in $Omega'$; therefore we may apply Green's, resp., Cauchy's, theorem to $f$ and $Omega'$. It follows that $int_partialOmega'f(z)>dz=0$, so that
          $$int_partialOmegaf(z)>dz=sum_j=1^mint_partial B_jf(z)>dz .$$
          Here the LHS is independent of $epsilon$. It follows that
          $$int_partialOmegaf(z)>dz=sum_j=1^mlim_epsilonto0int_partial B_jf(z)>dz=2pi i sum_j=1^mrm res(f, a_j) ,$$
          by definition of the residue.






          share|cite|improve this answer





















          • This is brilliant. Just one thing: how can I derive with details and rigor that $$int_partialOmega+partial B=int_partialOmega+int_partial B$$ to ‘convince’ a starter in complex analysis? (I know this is almost trivial to you.)
            – Szeto
            Jul 25 at 13:59











          • Also, to my surprise, I cannot google a similar proof. Indeed, a formal proof of residue theorem is quite rare on the internet.
            – Szeto
            Jul 25 at 14:02










          • Already $partialOmega$ might consist of several disjoint closed curves. If you accept the notion of boundary cycle as defined in your community, as well as the notion of integral over a chain (formal sum of smooth curves) then there is no problem with $partialOmega'=partialOmega-sum_jpartial B_j$.
            – Christian Blatter
            Jul 25 at 14:10














          up vote
          3
          down vote



          accepted










          You are given a region $Omegasubsetmathbb C$ with boundary cycle $partialOmega$ and a function $f:>Omegatomathbb C$ which is analytic apart from finitely many isolated singularities at the points $a_jinOmega$ $(1leq jleq m)$. The trick now is to draw tiny discs $B_j$ of radius $epsilon>0$ centered at these points. Then we consider the punched domain $Omega':=Omegasetminusbigcup_j=1^m B_j$ with boundary cycle
          $$partialOmega'=partialOmega-sum_j=1^m partial B_j .$$
          Note the minus signs here! The function $f$ is analytic in $Omega'$; therefore we may apply Green's, resp., Cauchy's, theorem to $f$ and $Omega'$. It follows that $int_partialOmega'f(z)>dz=0$, so that
          $$int_partialOmegaf(z)>dz=sum_j=1^mint_partial B_jf(z)>dz .$$
          Here the LHS is independent of $epsilon$. It follows that
          $$int_partialOmegaf(z)>dz=sum_j=1^mlim_epsilonto0int_partial B_jf(z)>dz=2pi i sum_j=1^mrm res(f, a_j) ,$$
          by definition of the residue.






          share|cite|improve this answer





















          • This is brilliant. Just one thing: how can I derive with details and rigor that $$int_partialOmega+partial B=int_partialOmega+int_partial B$$ to ‘convince’ a starter in complex analysis? (I know this is almost trivial to you.)
            – Szeto
            Jul 25 at 13:59











          • Also, to my surprise, I cannot google a similar proof. Indeed, a formal proof of residue theorem is quite rare on the internet.
            – Szeto
            Jul 25 at 14:02










          • Already $partialOmega$ might consist of several disjoint closed curves. If you accept the notion of boundary cycle as defined in your community, as well as the notion of integral over a chain (formal sum of smooth curves) then there is no problem with $partialOmega'=partialOmega-sum_jpartial B_j$.
            – Christian Blatter
            Jul 25 at 14:10












          up vote
          3
          down vote



          accepted







          up vote
          3
          down vote



          accepted






          You are given a region $Omegasubsetmathbb C$ with boundary cycle $partialOmega$ and a function $f:>Omegatomathbb C$ which is analytic apart from finitely many isolated singularities at the points $a_jinOmega$ $(1leq jleq m)$. The trick now is to draw tiny discs $B_j$ of radius $epsilon>0$ centered at these points. Then we consider the punched domain $Omega':=Omegasetminusbigcup_j=1^m B_j$ with boundary cycle
          $$partialOmega'=partialOmega-sum_j=1^m partial B_j .$$
          Note the minus signs here! The function $f$ is analytic in $Omega'$; therefore we may apply Green's, resp., Cauchy's, theorem to $f$ and $Omega'$. It follows that $int_partialOmega'f(z)>dz=0$, so that
          $$int_partialOmegaf(z)>dz=sum_j=1^mint_partial B_jf(z)>dz .$$
          Here the LHS is independent of $epsilon$. It follows that
          $$int_partialOmegaf(z)>dz=sum_j=1^mlim_epsilonto0int_partial B_jf(z)>dz=2pi i sum_j=1^mrm res(f, a_j) ,$$
          by definition of the residue.






          share|cite|improve this answer













          You are given a region $Omegasubsetmathbb C$ with boundary cycle $partialOmega$ and a function $f:>Omegatomathbb C$ which is analytic apart from finitely many isolated singularities at the points $a_jinOmega$ $(1leq jleq m)$. The trick now is to draw tiny discs $B_j$ of radius $epsilon>0$ centered at these points. Then we consider the punched domain $Omega':=Omegasetminusbigcup_j=1^m B_j$ with boundary cycle
          $$partialOmega'=partialOmega-sum_j=1^m partial B_j .$$
          Note the minus signs here! The function $f$ is analytic in $Omega'$; therefore we may apply Green's, resp., Cauchy's, theorem to $f$ and $Omega'$. It follows that $int_partialOmega'f(z)>dz=0$, so that
          $$int_partialOmegaf(z)>dz=sum_j=1^mint_partial B_jf(z)>dz .$$
          Here the LHS is independent of $epsilon$. It follows that
          $$int_partialOmegaf(z)>dz=sum_j=1^mlim_epsilonto0int_partial B_jf(z)>dz=2pi i sum_j=1^mrm res(f, a_j) ,$$
          by definition of the residue.







          share|cite|improve this answer













          share|cite|improve this answer



          share|cite|improve this answer











          answered Jul 25 at 13:05









          Christian Blatter

          163k7107306




          163k7107306











          • This is brilliant. Just one thing: how can I derive with details and rigor that $$int_partialOmega+partial B=int_partialOmega+int_partial B$$ to ‘convince’ a starter in complex analysis? (I know this is almost trivial to you.)
            – Szeto
            Jul 25 at 13:59











          • Also, to my surprise, I cannot google a similar proof. Indeed, a formal proof of residue theorem is quite rare on the internet.
            – Szeto
            Jul 25 at 14:02










          • Already $partialOmega$ might consist of several disjoint closed curves. If you accept the notion of boundary cycle as defined in your community, as well as the notion of integral over a chain (formal sum of smooth curves) then there is no problem with $partialOmega'=partialOmega-sum_jpartial B_j$.
            – Christian Blatter
            Jul 25 at 14:10
















          • This is brilliant. Just one thing: how can I derive with details and rigor that $$int_partialOmega+partial B=int_partialOmega+int_partial B$$ to ‘convince’ a starter in complex analysis? (I know this is almost trivial to you.)
            – Szeto
            Jul 25 at 13:59











          • Also, to my surprise, I cannot google a similar proof. Indeed, a formal proof of residue theorem is quite rare on the internet.
            – Szeto
            Jul 25 at 14:02










          • Already $partialOmega$ might consist of several disjoint closed curves. If you accept the notion of boundary cycle as defined in your community, as well as the notion of integral over a chain (formal sum of smooth curves) then there is no problem with $partialOmega'=partialOmega-sum_jpartial B_j$.
            – Christian Blatter
            Jul 25 at 14:10















          This is brilliant. Just one thing: how can I derive with details and rigor that $$int_partialOmega+partial B=int_partialOmega+int_partial B$$ to ‘convince’ a starter in complex analysis? (I know this is almost trivial to you.)
          – Szeto
          Jul 25 at 13:59





          This is brilliant. Just one thing: how can I derive with details and rigor that $$int_partialOmega+partial B=int_partialOmega+int_partial B$$ to ‘convince’ a starter in complex analysis? (I know this is almost trivial to you.)
          – Szeto
          Jul 25 at 13:59













          Also, to my surprise, I cannot google a similar proof. Indeed, a formal proof of residue theorem is quite rare on the internet.
          – Szeto
          Jul 25 at 14:02




          Also, to my surprise, I cannot google a similar proof. Indeed, a formal proof of residue theorem is quite rare on the internet.
          – Szeto
          Jul 25 at 14:02












          Already $partialOmega$ might consist of several disjoint closed curves. If you accept the notion of boundary cycle as defined in your community, as well as the notion of integral over a chain (formal sum of smooth curves) then there is no problem with $partialOmega'=partialOmega-sum_jpartial B_j$.
          – Christian Blatter
          Jul 25 at 14:10




          Already $partialOmega$ might consist of several disjoint closed curves. If you accept the notion of boundary cycle as defined in your community, as well as the notion of integral over a chain (formal sum of smooth curves) then there is no problem with $partialOmega'=partialOmega-sum_jpartial B_j$.
          – Christian Blatter
          Jul 25 at 14:10












           

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