Uniform PDF of offset sphere
$begingroup$
Note that throughout this I use the spherical mapping convention: $$(x,y,z) = (rcosphisintheta,rcostheta,rsinphisintheta)$$
I have derived that the uniform pdf for a sphere $S_1$ with radius $rho$ and center $(0,0,0)$ is $p_A(r,phi,theta) = frac{delta(r-rho)}{4pirho^2}$. I want to translate this sphere by $(0,rho,0)$ and find the corresponding pdf.
What I have tried is to rewrite the pdf in cartesian coordinates, that is:
$$p_B(x,y,z) = frac{p_A(r, phi, theta)}{|r^2sintheta|}$$
And translate it: $p_C(x,y,z) = p_B(x,y-rho,z)$.
Then I believe that the pdf I am looking for is: $p_D(r',phi',theta') = p_C(x,y,z)|r'^2sintheta'|$.
I have $r^2 = x^2 + (y-rho)^2 + z^2$, $costheta = frac{y-rho}{r}$, $r'^2 = x^2+y^2 + z^2$, $costheta' = frac{y}{r'}$. Assuming that this is correct I get the relationship:
$$r^2 = r'^2 - 2rho r'costheta' + rho^2$$
$$costheta = costheta' - frac{rho}{r}$$
Is everything correct? Is this the correct expression for the pdf I am looking for?
$$p_D(r',phi,theta') = p_A(r(r',theta'),phi,theta(r',theta'))frac{|r'^2sintheta'|}{|r^2(r',theta')sin(theta(r',theta'))|}$$
Edit:
Just for completeness I provide the derivation of the uniform pdf on the sphere centered at $(0,0,0)$ with radius $rho$. Since I only want to have a constant probability over the surface of the sphere I can write $p_A(r,phi,theta) = Cdelta(r-rho)$. In order to derive the pdf normalization constant $C$ I integrate the pdf:
$$int_{0}^{2pi}{int_{0}^{pi}{int_{0}^{infty}{p_A(r,phi,theta)r^2sintheta dr}dtheta}dphi} = $$
$$2pi Cint_{0}^{pi}{rho^2sintheta dtheta} =$$
$$4Cpirho^2 = 1$$
$$C = frac{1}{4pirho^2}$$
probability-distributions
$endgroup$
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$begingroup$
Note that throughout this I use the spherical mapping convention: $$(x,y,z) = (rcosphisintheta,rcostheta,rsinphisintheta)$$
I have derived that the uniform pdf for a sphere $S_1$ with radius $rho$ and center $(0,0,0)$ is $p_A(r,phi,theta) = frac{delta(r-rho)}{4pirho^2}$. I want to translate this sphere by $(0,rho,0)$ and find the corresponding pdf.
What I have tried is to rewrite the pdf in cartesian coordinates, that is:
$$p_B(x,y,z) = frac{p_A(r, phi, theta)}{|r^2sintheta|}$$
And translate it: $p_C(x,y,z) = p_B(x,y-rho,z)$.
Then I believe that the pdf I am looking for is: $p_D(r',phi',theta') = p_C(x,y,z)|r'^2sintheta'|$.
I have $r^2 = x^2 + (y-rho)^2 + z^2$, $costheta = frac{y-rho}{r}$, $r'^2 = x^2+y^2 + z^2$, $costheta' = frac{y}{r'}$. Assuming that this is correct I get the relationship:
$$r^2 = r'^2 - 2rho r'costheta' + rho^2$$
$$costheta = costheta' - frac{rho}{r}$$
Is everything correct? Is this the correct expression for the pdf I am looking for?
$$p_D(r',phi,theta') = p_A(r(r',theta'),phi,theta(r',theta'))frac{|r'^2sintheta'|}{|r^2(r',theta')sin(theta(r',theta'))|}$$
Edit:
Just for completeness I provide the derivation of the uniform pdf on the sphere centered at $(0,0,0)$ with radius $rho$. Since I only want to have a constant probability over the surface of the sphere I can write $p_A(r,phi,theta) = Cdelta(r-rho)$. In order to derive the pdf normalization constant $C$ I integrate the pdf:
$$int_{0}^{2pi}{int_{0}^{pi}{int_{0}^{infty}{p_A(r,phi,theta)r^2sintheta dr}dtheta}dphi} = $$
$$2pi Cint_{0}^{pi}{rho^2sintheta dtheta} =$$
$$4Cpirho^2 = 1$$
$$C = frac{1}{4pirho^2}$$
probability-distributions
$endgroup$
add a comment |
$begingroup$
Note that throughout this I use the spherical mapping convention: $$(x,y,z) = (rcosphisintheta,rcostheta,rsinphisintheta)$$
I have derived that the uniform pdf for a sphere $S_1$ with radius $rho$ and center $(0,0,0)$ is $p_A(r,phi,theta) = frac{delta(r-rho)}{4pirho^2}$. I want to translate this sphere by $(0,rho,0)$ and find the corresponding pdf.
What I have tried is to rewrite the pdf in cartesian coordinates, that is:
$$p_B(x,y,z) = frac{p_A(r, phi, theta)}{|r^2sintheta|}$$
And translate it: $p_C(x,y,z) = p_B(x,y-rho,z)$.
Then I believe that the pdf I am looking for is: $p_D(r',phi',theta') = p_C(x,y,z)|r'^2sintheta'|$.
I have $r^2 = x^2 + (y-rho)^2 + z^2$, $costheta = frac{y-rho}{r}$, $r'^2 = x^2+y^2 + z^2$, $costheta' = frac{y}{r'}$. Assuming that this is correct I get the relationship:
$$r^2 = r'^2 - 2rho r'costheta' + rho^2$$
$$costheta = costheta' - frac{rho}{r}$$
Is everything correct? Is this the correct expression for the pdf I am looking for?
$$p_D(r',phi,theta') = p_A(r(r',theta'),phi,theta(r',theta'))frac{|r'^2sintheta'|}{|r^2(r',theta')sin(theta(r',theta'))|}$$
Edit:
Just for completeness I provide the derivation of the uniform pdf on the sphere centered at $(0,0,0)$ with radius $rho$. Since I only want to have a constant probability over the surface of the sphere I can write $p_A(r,phi,theta) = Cdelta(r-rho)$. In order to derive the pdf normalization constant $C$ I integrate the pdf:
$$int_{0}^{2pi}{int_{0}^{pi}{int_{0}^{infty}{p_A(r,phi,theta)r^2sintheta dr}dtheta}dphi} = $$
$$2pi Cint_{0}^{pi}{rho^2sintheta dtheta} =$$
$$4Cpirho^2 = 1$$
$$C = frac{1}{4pirho^2}$$
probability-distributions
$endgroup$
Note that throughout this I use the spherical mapping convention: $$(x,y,z) = (rcosphisintheta,rcostheta,rsinphisintheta)$$
I have derived that the uniform pdf for a sphere $S_1$ with radius $rho$ and center $(0,0,0)$ is $p_A(r,phi,theta) = frac{delta(r-rho)}{4pirho^2}$. I want to translate this sphere by $(0,rho,0)$ and find the corresponding pdf.
What I have tried is to rewrite the pdf in cartesian coordinates, that is:
$$p_B(x,y,z) = frac{p_A(r, phi, theta)}{|r^2sintheta|}$$
And translate it: $p_C(x,y,z) = p_B(x,y-rho,z)$.
Then I believe that the pdf I am looking for is: $p_D(r',phi',theta') = p_C(x,y,z)|r'^2sintheta'|$.
I have $r^2 = x^2 + (y-rho)^2 + z^2$, $costheta = frac{y-rho}{r}$, $r'^2 = x^2+y^2 + z^2$, $costheta' = frac{y}{r'}$. Assuming that this is correct I get the relationship:
$$r^2 = r'^2 - 2rho r'costheta' + rho^2$$
$$costheta = costheta' - frac{rho}{r}$$
Is everything correct? Is this the correct expression for the pdf I am looking for?
$$p_D(r',phi,theta') = p_A(r(r',theta'),phi,theta(r',theta'))frac{|r'^2sintheta'|}{|r^2(r',theta')sin(theta(r',theta'))|}$$
Edit:
Just for completeness I provide the derivation of the uniform pdf on the sphere centered at $(0,0,0)$ with radius $rho$. Since I only want to have a constant probability over the surface of the sphere I can write $p_A(r,phi,theta) = Cdelta(r-rho)$. In order to derive the pdf normalization constant $C$ I integrate the pdf:
$$int_{0}^{2pi}{int_{0}^{pi}{int_{0}^{infty}{p_A(r,phi,theta)r^2sintheta dr}dtheta}dphi} = $$
$$2pi Cint_{0}^{pi}{rho^2sintheta dtheta} =$$
$$4Cpirho^2 = 1$$
$$C = frac{1}{4pirho^2}$$
probability-distributions
probability-distributions
edited Jan 21 at 2:38
lightxbulb
asked Jan 20 at 17:14
lightxbulblightxbulb
945311
945311
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The denominator seems to be redundant, since it actually cancels out with the term $|r^2sintheta|$ in the numerator, which I forgot to add in the pdf it seems: $p_A(r,phi,theta) = delta(r-rho)frac{|r^2sintheta|}{4pirho^2}$.
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$begingroup$
The denominator seems to be redundant, since it actually cancels out with the term $|r^2sintheta|$ in the numerator, which I forgot to add in the pdf it seems: $p_A(r,phi,theta) = delta(r-rho)frac{|r^2sintheta|}{4pirho^2}$.
$endgroup$
add a comment |
$begingroup$
The denominator seems to be redundant, since it actually cancels out with the term $|r^2sintheta|$ in the numerator, which I forgot to add in the pdf it seems: $p_A(r,phi,theta) = delta(r-rho)frac{|r^2sintheta|}{4pirho^2}$.
$endgroup$
add a comment |
$begingroup$
The denominator seems to be redundant, since it actually cancels out with the term $|r^2sintheta|$ in the numerator, which I forgot to add in the pdf it seems: $p_A(r,phi,theta) = delta(r-rho)frac{|r^2sintheta|}{4pirho^2}$.
$endgroup$
The denominator seems to be redundant, since it actually cancels out with the term $|r^2sintheta|$ in the numerator, which I forgot to add in the pdf it seems: $p_A(r,phi,theta) = delta(r-rho)frac{|r^2sintheta|}{4pirho^2}$.
answered Feb 8 at 18:34
lightxbulblightxbulb
945311
945311
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