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The discussion centers on the function P(R, θ, φ) defined in spherical coordinates and its maximum value Pmax within a closed sphere S. The normalized function F(R, θ, φ) is derived as F(R, θ, φ) = P(R, θ, φ) / Pmax, where Fmax equals 1. The key question raised is whether the equality between the ratios of P and F over their respective integrals holds true, contingent on Pmax being a constant. The conclusion confirms that Pmax is indeed a constant, allowing it to be moved inside the integral, thus validating the equality.

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Let [itex]\;P(R,\theta,\phi)\;[/itex] be function at each point defined by [itex]R,\theta,\phi[/itex] in spherical coordinates.

Let [itex]\;P_{max} \;[/itex] be the maximum value of [itex]\;P(R,\theta,\phi)\;[/itex] in the closed sphere S.

[tex]\hbox {Let }\;F(R,\theta,\phi)=\frac {P(R,\theta,\phi)}{P_{max}}[/tex]

Which is the normalized value of [itex]\;P(R,\theta,\phi)\; \hbox {where } \; F_{max} = 1[/itex].

My question is whether:

[tex]\frac {P(R,\theta,\phi)}{\oint_S P(R,\theta,\phi) d\;S}\; =\; \frac {F(R,\theta,\phi)}{\oint_S F(R,\theta,\phi) d\;S}[/tex]

I thought

[tex]\frac {\left [\frac {P(R,\theta,\phi)}{P_{max}}\right ]} {\left [\frac {\oint_S P(R,\theta,\phi) d\;S}{P_{max}}\right ]} \;\hbox { not equal to } \; \frac {F(R,\theta,\phi)}{\oint_S F(R,\theta,\phi) d\;S}[/tex]

Unless we can consider [itex]\;P_{max}\;[/itex] is a constant and can be moved inside the integration. So the question is whether [itex]\;P_{max}\;[/itex] is a constant? I am not sure.

Please help.

Thanks

Alan
 
Last edited:
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Yes, once P has been defined, Pmax is a specific number, a constant.
 
HallsofIvy said:
Yes, once P has been defined, Pmax is a specific number, a constant.

Thanks so much for answering.

So I can move [itex]\;P_{max}\;[/itex] inside the integral and:


[tex]\frac {P(R,\theta,\phi)}{\oint_S P(R,\theta,\phi) d\;S}\; =\; \frac {F(R,\theta,\phi)}{\oint_S F(R,\theta,\phi) d\;S}[/tex]

Thanks

Alan
 

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