- #1
Shinobii
- 34
- 0
Hi gang, I am hoping you can clear something up for me. When evaluating the potential of a solid sphere, I find myself confused about the volumes used such that,
[tex] \phi = Q \int_{\infty}^R \frac{1}{V_1} r^2 \sin(\theta) \, dr \, d\theta \, d\phi + Q \int_R^r \frac{1}{V_2} r^2 \sin(\theta) \, dr \, d\theta \, d\phi. [/tex]
where [itex] V_1 = 4 \pi r^3/3 [/itex] and [itex] V_2 = 4 \pi R^3/3 [/itex].
Why is [itex] V_1 [/itex] the volume inside and [itex] V_2 [/itex] the volume at r = R?
The first volume I understand since we are coming from infinity to the surface of the sphere. But when evaluating the second integral with the second volume, why is it only at r=R.
My current logic is that the volume depends on the initial point of integration (which would be consistent with this problem), but surely this cannot be always true?
I hope someone can shed some light on this matter.
[tex] \phi = Q \int_{\infty}^R \frac{1}{V_1} r^2 \sin(\theta) \, dr \, d\theta \, d\phi + Q \int_R^r \frac{1}{V_2} r^2 \sin(\theta) \, dr \, d\theta \, d\phi. [/tex]
where [itex] V_1 = 4 \pi r^3/3 [/itex] and [itex] V_2 = 4 \pi R^3/3 [/itex].
Why is [itex] V_1 [/itex] the volume inside and [itex] V_2 [/itex] the volume at r = R?
The first volume I understand since we are coming from infinity to the surface of the sphere. But when evaluating the second integral with the second volume, why is it only at r=R.
My current logic is that the volume depends on the initial point of integration (which would be consistent with this problem), but surely this cannot be always true?
I hope someone can shed some light on this matter.