Surface integral of a partially constant Dirac delta
$begingroup$
I am trying to integrate the product of a function and a partially constant delta function over a sphere of constant radius $r$.
The integral is of the form
$$int^{2pi}_0 int^{pi}_0 f(mathbf{r})delta(x-x_0)delta(y-y_0) sintheta,mathrm{d}theta ,mathrm{d}phi. $$
I know that this integral is very simple when the delta function is fully three-dimensional, such as $$delta^3(mathbf{r}-mathbf{r}_0)=delta(x-x_0)delta(y-y_0)delta(z-z_0),$$ but what I have here is something a bit different. Does anyone have anyone have any suggestions?
coordinate-systems distribution-theory dirac-delta spherical-coordinates surface-integrals
$endgroup$
add a comment |
$begingroup$
I am trying to integrate the product of a function and a partially constant delta function over a sphere of constant radius $r$.
The integral is of the form
$$int^{2pi}_0 int^{pi}_0 f(mathbf{r})delta(x-x_0)delta(y-y_0) sintheta,mathrm{d}theta ,mathrm{d}phi. $$
I know that this integral is very simple when the delta function is fully three-dimensional, such as $$delta^3(mathbf{r}-mathbf{r}_0)=delta(x-x_0)delta(y-y_0)delta(z-z_0),$$ but what I have here is something a bit different. Does anyone have anyone have any suggestions?
coordinate-systems distribution-theory dirac-delta spherical-coordinates surface-integrals
$endgroup$
1
$begingroup$
should you have also integral in $r$ for spherical coordinates?
$endgroup$
– Michael Medvinsky
Nov 10 '15 at 8:41
$begingroup$
no, it's a surface integral over the sphere of constant radius $r$, so there is no integration on $,mathrm{d}r$.
$endgroup$
– aquarkydude
Nov 10 '15 at 8:42
1
$begingroup$
if $r$ is constant $f(r)$ is constant should it be $f(r_0)$?
$endgroup$
– Michael Medvinsky
Nov 10 '15 at 8:44
$begingroup$
it's not $f(r)$ but rather $f(mathbf{r})$. That is, the function $f$ takes as an argument the vector $mathbf{r}$, not just the distance from the origin $r$
$endgroup$
– aquarkydude
Nov 10 '15 at 8:45
$begingroup$
Moreover, $r_0$ is not defined in the context of the problem, but only $x_0$ and $y_0$.
$endgroup$
– aquarkydude
Nov 10 '15 at 8:47
add a comment |
$begingroup$
I am trying to integrate the product of a function and a partially constant delta function over a sphere of constant radius $r$.
The integral is of the form
$$int^{2pi}_0 int^{pi}_0 f(mathbf{r})delta(x-x_0)delta(y-y_0) sintheta,mathrm{d}theta ,mathrm{d}phi. $$
I know that this integral is very simple when the delta function is fully three-dimensional, such as $$delta^3(mathbf{r}-mathbf{r}_0)=delta(x-x_0)delta(y-y_0)delta(z-z_0),$$ but what I have here is something a bit different. Does anyone have anyone have any suggestions?
coordinate-systems distribution-theory dirac-delta spherical-coordinates surface-integrals
$endgroup$
I am trying to integrate the product of a function and a partially constant delta function over a sphere of constant radius $r$.
The integral is of the form
$$int^{2pi}_0 int^{pi}_0 f(mathbf{r})delta(x-x_0)delta(y-y_0) sintheta,mathrm{d}theta ,mathrm{d}phi. $$
I know that this integral is very simple when the delta function is fully three-dimensional, such as $$delta^3(mathbf{r}-mathbf{r}_0)=delta(x-x_0)delta(y-y_0)delta(z-z_0),$$ but what I have here is something a bit different. Does anyone have anyone have any suggestions?
coordinate-systems distribution-theory dirac-delta spherical-coordinates surface-integrals
coordinate-systems distribution-theory dirac-delta spherical-coordinates surface-integrals
edited Jan 23 at 8:58
Qmechanic
5,13211858
5,13211858
asked Nov 10 '15 at 8:21
aquarkydudeaquarkydude
184
184
1
$begingroup$
should you have also integral in $r$ for spherical coordinates?
$endgroup$
– Michael Medvinsky
Nov 10 '15 at 8:41
$begingroup$
no, it's a surface integral over the sphere of constant radius $r$, so there is no integration on $,mathrm{d}r$.
$endgroup$
– aquarkydude
Nov 10 '15 at 8:42
1
$begingroup$
if $r$ is constant $f(r)$ is constant should it be $f(r_0)$?
$endgroup$
– Michael Medvinsky
Nov 10 '15 at 8:44
$begingroup$
it's not $f(r)$ but rather $f(mathbf{r})$. That is, the function $f$ takes as an argument the vector $mathbf{r}$, not just the distance from the origin $r$
$endgroup$
– aquarkydude
Nov 10 '15 at 8:45
$begingroup$
Moreover, $r_0$ is not defined in the context of the problem, but only $x_0$ and $y_0$.
$endgroup$
– aquarkydude
Nov 10 '15 at 8:47
add a comment |
1
$begingroup$
should you have also integral in $r$ for spherical coordinates?
$endgroup$
– Michael Medvinsky
Nov 10 '15 at 8:41
$begingroup$
no, it's a surface integral over the sphere of constant radius $r$, so there is no integration on $,mathrm{d}r$.
$endgroup$
– aquarkydude
Nov 10 '15 at 8:42
1
$begingroup$
if $r$ is constant $f(r)$ is constant should it be $f(r_0)$?
$endgroup$
– Michael Medvinsky
Nov 10 '15 at 8:44
$begingroup$
it's not $f(r)$ but rather $f(mathbf{r})$. That is, the function $f$ takes as an argument the vector $mathbf{r}$, not just the distance from the origin $r$
$endgroup$
– aquarkydude
Nov 10 '15 at 8:45
$begingroup$
Moreover, $r_0$ is not defined in the context of the problem, but only $x_0$ and $y_0$.
$endgroup$
– aquarkydude
Nov 10 '15 at 8:47
1
1
$begingroup$
should you have also integral in $r$ for spherical coordinates?
$endgroup$
– Michael Medvinsky
Nov 10 '15 at 8:41
$begingroup$
should you have also integral in $r$ for spherical coordinates?
$endgroup$
– Michael Medvinsky
Nov 10 '15 at 8:41
$begingroup$
no, it's a surface integral over the sphere of constant radius $r$, so there is no integration on $,mathrm{d}r$.
$endgroup$
– aquarkydude
Nov 10 '15 at 8:42
$begingroup$
no, it's a surface integral over the sphere of constant radius $r$, so there is no integration on $,mathrm{d}r$.
$endgroup$
– aquarkydude
Nov 10 '15 at 8:42
1
1
$begingroup$
if $r$ is constant $f(r)$ is constant should it be $f(r_0)$?
$endgroup$
– Michael Medvinsky
Nov 10 '15 at 8:44
$begingroup$
if $r$ is constant $f(r)$ is constant should it be $f(r_0)$?
$endgroup$
– Michael Medvinsky
Nov 10 '15 at 8:44
$begingroup$
it's not $f(r)$ but rather $f(mathbf{r})$. That is, the function $f$ takes as an argument the vector $mathbf{r}$, not just the distance from the origin $r$
$endgroup$
– aquarkydude
Nov 10 '15 at 8:45
$begingroup$
it's not $f(r)$ but rather $f(mathbf{r})$. That is, the function $f$ takes as an argument the vector $mathbf{r}$, not just the distance from the origin $r$
$endgroup$
– aquarkydude
Nov 10 '15 at 8:45
$begingroup$
Moreover, $r_0$ is not defined in the context of the problem, but only $x_0$ and $y_0$.
$endgroup$
– aquarkydude
Nov 10 '15 at 8:47
$begingroup$
Moreover, $r_0$ is not defined in the context of the problem, but only $x_0$ and $y_0$.
$endgroup$
– aquarkydude
Nov 10 '15 at 8:47
add a comment |
1 Answer
1
active
oldest
votes
$begingroup$
Here we give a rough sketch, and leave it to the reader to iron out various technical issues.
Define the spherical coordinates $(r,theta,phi)$ as
$$tag{1} x~=~rxi, qquad xi~=~sinthetacosphi, qquad y~=~reta, qquad eta~=~sinthetasinphi, qquad z~=~rcostheta. $$Define reflection $$tag{2}sigma: (x,y,z)mapsto (x,y,-z)$$ in the $(x,y)$-plane.
Define function $$tag{3}g({bf r})~:=~f({bf r})+fcircsigma({bf r}), qquad {bf r}~=~(x,y,z).$$
Define function $$tag{4}h({bf r})~:=~frac{g({bf r})}{rz}.$$
Define unit disk
$$ tag{5} D~:=~{(xi,eta)inmathbb{R}^2 mid xi^2+eta^2~<~1}. $$OP's integral then reads
$$ I:~=~ int_0^{2pi}!dphi~int_0^{pi}!dtheta~sintheta ~f({bf r}) delta(x-x_0)delta(y-y_0)$$
$$ ~=~int_0^{2pi}!dphi~int_0^{frac{pi}{2}}!dtheta~sinthetacostheta ~h({bf r})deltaleft(xi-frac{x_0}{r}right)deltaleft(eta-frac{x_0}{r}right)$$
$$~=~iint_D !dxi~deta ~h({bf r})deltaleft(xi-frac{x_0}{r}right)deltaleft(eta-frac{x_0}{r}right)$$
$$tag{6}~=~left{begin{array}{ccc} hleft(x_0, y_0, sqrt{r^2-x_0^2-y_0^2}right) &{rm for}& x_0^2+y_0^2<r^2, cr
frac{1}{2}h(x_0, y_0, 0) &{rm for}& x_0^2+y_0^2=r^2, cr
0 &{rm for}& x_0^2+y_0^2>r^2.
end{array}right. $$
$endgroup$
$begingroup$
Wow. Thank you. Tremendously.
$endgroup$
– aquarkydude
Nov 11 '15 at 17:01
$begingroup$
Sorry, I'm not great with proper mathematics notations. The open circle in equation 5: does this indicate applying the reflection operation to the argument of the function $f(mathbf{r})$?
$endgroup$
– aquarkydude
Nov 11 '15 at 17:08
$begingroup$
Also, it appears you've defined $eta$ and $xi$ identically. I think $eta = sin{theta} sin{phi}$?
$endgroup$
– aquarkydude
Nov 11 '15 at 17:15
$begingroup$
Ups. Yes. Corrected. And yes: $fcircsigma({bf r})=f(sigma({bf r}))$.
$endgroup$
– Qmechanic
Nov 11 '15 at 17:20
1
$begingroup$
1. Well, that was one of the reasons to put the disclaimer in the first line of the answer :) Note however that the fraction $h$ could be extended to a well-defined regular function if the numerator $f$ has a matching zero at $z=0$. 2. Finally, your last intuitive comment about a delta function seems to make no mathematical sense.
$endgroup$
– Qmechanic
Nov 11 '15 at 20:42
|
show 2 more comments
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1 Answer
1
active
oldest
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active
oldest
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$begingroup$
Here we give a rough sketch, and leave it to the reader to iron out various technical issues.
Define the spherical coordinates $(r,theta,phi)$ as
$$tag{1} x~=~rxi, qquad xi~=~sinthetacosphi, qquad y~=~reta, qquad eta~=~sinthetasinphi, qquad z~=~rcostheta. $$Define reflection $$tag{2}sigma: (x,y,z)mapsto (x,y,-z)$$ in the $(x,y)$-plane.
Define function $$tag{3}g({bf r})~:=~f({bf r})+fcircsigma({bf r}), qquad {bf r}~=~(x,y,z).$$
Define function $$tag{4}h({bf r})~:=~frac{g({bf r})}{rz}.$$
Define unit disk
$$ tag{5} D~:=~{(xi,eta)inmathbb{R}^2 mid xi^2+eta^2~<~1}. $$OP's integral then reads
$$ I:~=~ int_0^{2pi}!dphi~int_0^{pi}!dtheta~sintheta ~f({bf r}) delta(x-x_0)delta(y-y_0)$$
$$ ~=~int_0^{2pi}!dphi~int_0^{frac{pi}{2}}!dtheta~sinthetacostheta ~h({bf r})deltaleft(xi-frac{x_0}{r}right)deltaleft(eta-frac{x_0}{r}right)$$
$$~=~iint_D !dxi~deta ~h({bf r})deltaleft(xi-frac{x_0}{r}right)deltaleft(eta-frac{x_0}{r}right)$$
$$tag{6}~=~left{begin{array}{ccc} hleft(x_0, y_0, sqrt{r^2-x_0^2-y_0^2}right) &{rm for}& x_0^2+y_0^2<r^2, cr
frac{1}{2}h(x_0, y_0, 0) &{rm for}& x_0^2+y_0^2=r^2, cr
0 &{rm for}& x_0^2+y_0^2>r^2.
end{array}right. $$
$endgroup$
$begingroup$
Wow. Thank you. Tremendously.
$endgroup$
– aquarkydude
Nov 11 '15 at 17:01
$begingroup$
Sorry, I'm not great with proper mathematics notations. The open circle in equation 5: does this indicate applying the reflection operation to the argument of the function $f(mathbf{r})$?
$endgroup$
– aquarkydude
Nov 11 '15 at 17:08
$begingroup$
Also, it appears you've defined $eta$ and $xi$ identically. I think $eta = sin{theta} sin{phi}$?
$endgroup$
– aquarkydude
Nov 11 '15 at 17:15
$begingroup$
Ups. Yes. Corrected. And yes: $fcircsigma({bf r})=f(sigma({bf r}))$.
$endgroup$
– Qmechanic
Nov 11 '15 at 17:20
1
$begingroup$
1. Well, that was one of the reasons to put the disclaimer in the first line of the answer :) Note however that the fraction $h$ could be extended to a well-defined regular function if the numerator $f$ has a matching zero at $z=0$. 2. Finally, your last intuitive comment about a delta function seems to make no mathematical sense.
$endgroup$
– Qmechanic
Nov 11 '15 at 20:42
|
show 2 more comments
$begingroup$
Here we give a rough sketch, and leave it to the reader to iron out various technical issues.
Define the spherical coordinates $(r,theta,phi)$ as
$$tag{1} x~=~rxi, qquad xi~=~sinthetacosphi, qquad y~=~reta, qquad eta~=~sinthetasinphi, qquad z~=~rcostheta. $$Define reflection $$tag{2}sigma: (x,y,z)mapsto (x,y,-z)$$ in the $(x,y)$-plane.
Define function $$tag{3}g({bf r})~:=~f({bf r})+fcircsigma({bf r}), qquad {bf r}~=~(x,y,z).$$
Define function $$tag{4}h({bf r})~:=~frac{g({bf r})}{rz}.$$
Define unit disk
$$ tag{5} D~:=~{(xi,eta)inmathbb{R}^2 mid xi^2+eta^2~<~1}. $$OP's integral then reads
$$ I:~=~ int_0^{2pi}!dphi~int_0^{pi}!dtheta~sintheta ~f({bf r}) delta(x-x_0)delta(y-y_0)$$
$$ ~=~int_0^{2pi}!dphi~int_0^{frac{pi}{2}}!dtheta~sinthetacostheta ~h({bf r})deltaleft(xi-frac{x_0}{r}right)deltaleft(eta-frac{x_0}{r}right)$$
$$~=~iint_D !dxi~deta ~h({bf r})deltaleft(xi-frac{x_0}{r}right)deltaleft(eta-frac{x_0}{r}right)$$
$$tag{6}~=~left{begin{array}{ccc} hleft(x_0, y_0, sqrt{r^2-x_0^2-y_0^2}right) &{rm for}& x_0^2+y_0^2<r^2, cr
frac{1}{2}h(x_0, y_0, 0) &{rm for}& x_0^2+y_0^2=r^2, cr
0 &{rm for}& x_0^2+y_0^2>r^2.
end{array}right. $$
$endgroup$
$begingroup$
Wow. Thank you. Tremendously.
$endgroup$
– aquarkydude
Nov 11 '15 at 17:01
$begingroup$
Sorry, I'm not great with proper mathematics notations. The open circle in equation 5: does this indicate applying the reflection operation to the argument of the function $f(mathbf{r})$?
$endgroup$
– aquarkydude
Nov 11 '15 at 17:08
$begingroup$
Also, it appears you've defined $eta$ and $xi$ identically. I think $eta = sin{theta} sin{phi}$?
$endgroup$
– aquarkydude
Nov 11 '15 at 17:15
$begingroup$
Ups. Yes. Corrected. And yes: $fcircsigma({bf r})=f(sigma({bf r}))$.
$endgroup$
– Qmechanic
Nov 11 '15 at 17:20
1
$begingroup$
1. Well, that was one of the reasons to put the disclaimer in the first line of the answer :) Note however that the fraction $h$ could be extended to a well-defined regular function if the numerator $f$ has a matching zero at $z=0$. 2. Finally, your last intuitive comment about a delta function seems to make no mathematical sense.
$endgroup$
– Qmechanic
Nov 11 '15 at 20:42
|
show 2 more comments
$begingroup$
Here we give a rough sketch, and leave it to the reader to iron out various technical issues.
Define the spherical coordinates $(r,theta,phi)$ as
$$tag{1} x~=~rxi, qquad xi~=~sinthetacosphi, qquad y~=~reta, qquad eta~=~sinthetasinphi, qquad z~=~rcostheta. $$Define reflection $$tag{2}sigma: (x,y,z)mapsto (x,y,-z)$$ in the $(x,y)$-plane.
Define function $$tag{3}g({bf r})~:=~f({bf r})+fcircsigma({bf r}), qquad {bf r}~=~(x,y,z).$$
Define function $$tag{4}h({bf r})~:=~frac{g({bf r})}{rz}.$$
Define unit disk
$$ tag{5} D~:=~{(xi,eta)inmathbb{R}^2 mid xi^2+eta^2~<~1}. $$OP's integral then reads
$$ I:~=~ int_0^{2pi}!dphi~int_0^{pi}!dtheta~sintheta ~f({bf r}) delta(x-x_0)delta(y-y_0)$$
$$ ~=~int_0^{2pi}!dphi~int_0^{frac{pi}{2}}!dtheta~sinthetacostheta ~h({bf r})deltaleft(xi-frac{x_0}{r}right)deltaleft(eta-frac{x_0}{r}right)$$
$$~=~iint_D !dxi~deta ~h({bf r})deltaleft(xi-frac{x_0}{r}right)deltaleft(eta-frac{x_0}{r}right)$$
$$tag{6}~=~left{begin{array}{ccc} hleft(x_0, y_0, sqrt{r^2-x_0^2-y_0^2}right) &{rm for}& x_0^2+y_0^2<r^2, cr
frac{1}{2}h(x_0, y_0, 0) &{rm for}& x_0^2+y_0^2=r^2, cr
0 &{rm for}& x_0^2+y_0^2>r^2.
end{array}right. $$
$endgroup$
Here we give a rough sketch, and leave it to the reader to iron out various technical issues.
Define the spherical coordinates $(r,theta,phi)$ as
$$tag{1} x~=~rxi, qquad xi~=~sinthetacosphi, qquad y~=~reta, qquad eta~=~sinthetasinphi, qquad z~=~rcostheta. $$Define reflection $$tag{2}sigma: (x,y,z)mapsto (x,y,-z)$$ in the $(x,y)$-plane.
Define function $$tag{3}g({bf r})~:=~f({bf r})+fcircsigma({bf r}), qquad {bf r}~=~(x,y,z).$$
Define function $$tag{4}h({bf r})~:=~frac{g({bf r})}{rz}.$$
Define unit disk
$$ tag{5} D~:=~{(xi,eta)inmathbb{R}^2 mid xi^2+eta^2~<~1}. $$OP's integral then reads
$$ I:~=~ int_0^{2pi}!dphi~int_0^{pi}!dtheta~sintheta ~f({bf r}) delta(x-x_0)delta(y-y_0)$$
$$ ~=~int_0^{2pi}!dphi~int_0^{frac{pi}{2}}!dtheta~sinthetacostheta ~h({bf r})deltaleft(xi-frac{x_0}{r}right)deltaleft(eta-frac{x_0}{r}right)$$
$$~=~iint_D !dxi~deta ~h({bf r})deltaleft(xi-frac{x_0}{r}right)deltaleft(eta-frac{x_0}{r}right)$$
$$tag{6}~=~left{begin{array}{ccc} hleft(x_0, y_0, sqrt{r^2-x_0^2-y_0^2}right) &{rm for}& x_0^2+y_0^2<r^2, cr
frac{1}{2}h(x_0, y_0, 0) &{rm for}& x_0^2+y_0^2=r^2, cr
0 &{rm for}& x_0^2+y_0^2>r^2.
end{array}right. $$
edited Nov 11 '15 at 17:20
answered Nov 10 '15 at 15:39
QmechanicQmechanic
5,13211858
5,13211858
$begingroup$
Wow. Thank you. Tremendously.
$endgroup$
– aquarkydude
Nov 11 '15 at 17:01
$begingroup$
Sorry, I'm not great with proper mathematics notations. The open circle in equation 5: does this indicate applying the reflection operation to the argument of the function $f(mathbf{r})$?
$endgroup$
– aquarkydude
Nov 11 '15 at 17:08
$begingroup$
Also, it appears you've defined $eta$ and $xi$ identically. I think $eta = sin{theta} sin{phi}$?
$endgroup$
– aquarkydude
Nov 11 '15 at 17:15
$begingroup$
Ups. Yes. Corrected. And yes: $fcircsigma({bf r})=f(sigma({bf r}))$.
$endgroup$
– Qmechanic
Nov 11 '15 at 17:20
1
$begingroup$
1. Well, that was one of the reasons to put the disclaimer in the first line of the answer :) Note however that the fraction $h$ could be extended to a well-defined regular function if the numerator $f$ has a matching zero at $z=0$. 2. Finally, your last intuitive comment about a delta function seems to make no mathematical sense.
$endgroup$
– Qmechanic
Nov 11 '15 at 20:42
|
show 2 more comments
$begingroup$
Wow. Thank you. Tremendously.
$endgroup$
– aquarkydude
Nov 11 '15 at 17:01
$begingroup$
Sorry, I'm not great with proper mathematics notations. The open circle in equation 5: does this indicate applying the reflection operation to the argument of the function $f(mathbf{r})$?
$endgroup$
– aquarkydude
Nov 11 '15 at 17:08
$begingroup$
Also, it appears you've defined $eta$ and $xi$ identically. I think $eta = sin{theta} sin{phi}$?
$endgroup$
– aquarkydude
Nov 11 '15 at 17:15
$begingroup$
Ups. Yes. Corrected. And yes: $fcircsigma({bf r})=f(sigma({bf r}))$.
$endgroup$
– Qmechanic
Nov 11 '15 at 17:20
1
$begingroup$
1. Well, that was one of the reasons to put the disclaimer in the first line of the answer :) Note however that the fraction $h$ could be extended to a well-defined regular function if the numerator $f$ has a matching zero at $z=0$. 2. Finally, your last intuitive comment about a delta function seems to make no mathematical sense.
$endgroup$
– Qmechanic
Nov 11 '15 at 20:42
$begingroup$
Wow. Thank you. Tremendously.
$endgroup$
– aquarkydude
Nov 11 '15 at 17:01
$begingroup$
Wow. Thank you. Tremendously.
$endgroup$
– aquarkydude
Nov 11 '15 at 17:01
$begingroup$
Sorry, I'm not great with proper mathematics notations. The open circle in equation 5: does this indicate applying the reflection operation to the argument of the function $f(mathbf{r})$?
$endgroup$
– aquarkydude
Nov 11 '15 at 17:08
$begingroup$
Sorry, I'm not great with proper mathematics notations. The open circle in equation 5: does this indicate applying the reflection operation to the argument of the function $f(mathbf{r})$?
$endgroup$
– aquarkydude
Nov 11 '15 at 17:08
$begingroup$
Also, it appears you've defined $eta$ and $xi$ identically. I think $eta = sin{theta} sin{phi}$?
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– aquarkydude
Nov 11 '15 at 17:15
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Also, it appears you've defined $eta$ and $xi$ identically. I think $eta = sin{theta} sin{phi}$?
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– aquarkydude
Nov 11 '15 at 17:15
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Ups. Yes. Corrected. And yes: $fcircsigma({bf r})=f(sigma({bf r}))$.
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– Qmechanic
Nov 11 '15 at 17:20
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Ups. Yes. Corrected. And yes: $fcircsigma({bf r})=f(sigma({bf r}))$.
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– Qmechanic
Nov 11 '15 at 17:20
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1. Well, that was one of the reasons to put the disclaimer in the first line of the answer :) Note however that the fraction $h$ could be extended to a well-defined regular function if the numerator $f$ has a matching zero at $z=0$. 2. Finally, your last intuitive comment about a delta function seems to make no mathematical sense.
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– Qmechanic
Nov 11 '15 at 20:42
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1. Well, that was one of the reasons to put the disclaimer in the first line of the answer :) Note however that the fraction $h$ could be extended to a well-defined regular function if the numerator $f$ has a matching zero at $z=0$. 2. Finally, your last intuitive comment about a delta function seems to make no mathematical sense.
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– Qmechanic
Nov 11 '15 at 20:42
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1
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should you have also integral in $r$ for spherical coordinates?
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– Michael Medvinsky
Nov 10 '15 at 8:41
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no, it's a surface integral over the sphere of constant radius $r$, so there is no integration on $,mathrm{d}r$.
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– aquarkydude
Nov 10 '15 at 8:42
1
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if $r$ is constant $f(r)$ is constant should it be $f(r_0)$?
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– Michael Medvinsky
Nov 10 '15 at 8:44
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it's not $f(r)$ but rather $f(mathbf{r})$. That is, the function $f$ takes as an argument the vector $mathbf{r}$, not just the distance from the origin $r$
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– aquarkydude
Nov 10 '15 at 8:45
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Moreover, $r_0$ is not defined in the context of the problem, but only $x_0$ and $y_0$.
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– aquarkydude
Nov 10 '15 at 8:47