I Calculating the change of the volume of a sphere using this integral

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The discussion centers on calculating the volume change of a spherical cap of liquid using a specific integral. The integral is parameterized in spherical coordinates, with the volume change expressed as a function of a small disturbance, denoted as η. The author clarifies that the volume change can be derived by integrating from R to R + η, indicating that this range accounts for the deviation from equilibrium. The conversation highlights the importance of understanding how the position of the drop's surface affects the enclosed volume. Overall, the mathematical approach effectively captures the relationship between the perturbation and the resulting volume change.
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I have a spherical cap of liquid (drop) that rests on a substrate. The substrate has a small hole at the base where liquid is pumped into the drop. One way to parameterize the spherical cap is via: $$x = \sin(s)\cos\phi/\sin\alpha, \,\,\,y= \sin(s)\sin\phi/\sin\alpha,\,\,\,z=(\cos(s)-\cos\alpha)/\sin\alpha$$ where here ##\alpha## is the angle the spherical cap makes with the x-y plane, and ##\phi \in [0,2\pi]## and ##s\in[0,\alpha]##.

Now ##\eta## is a small disturbance to the drop. The author then states the volume change can be written as $$\Delta V = \int_0^{2\pi}\int_{\cos\alpha}^1 R^2 \eta d(\cos(s))d\phi$$

Can someone explain the math behind that integral? I understand the ##\phi## integral, but the inside integral I can't make sense of. For help, here's a sketch:
Screenshot 2023-12-17 at 12.06.10 PM.png
 
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This is a straightforward use of spherical polar coordinates (r, s, \phi):
\begin{split} <br /> \Delta V &amp;= \int_0^{2\pi} \int_0^{\alpha} \int_R^{R + \eta} r^2\sin s\,dr\,ds\,d\phi \\<br /> &amp;= \int_0^{2\pi} \int_0^\alpha \frac13\left( (R + \eta)^3 - R^3 \right) \sin s\,ds\,d\phi \\<br /> &amp;= \int_0^{2\pi} \int_{\cos \alpha}^1 \frac13\left( 3R^2\eta + 3R\eta^2 + \eta^3\right)\,d(\cos s)\,d\phi.<br /> \end{split} Since \eta is a small perturbation, only the term \frac13 (3R^2\eta) is retained.
 
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pasmith said:
This is a straightforward use of spherical polar coordinates (r, s, \phi):
\begin{split}<br /> \Delta V &amp;= \int_0^{2\pi} \int_0^{\alpha} \int_R^{R + \eta} r^2\sin s\,dr\,ds\,d\phi \\<br /> &amp;= \int_0^{2\pi} \int_0^\alpha \frac13\left( (R + \eta)^3 - R^3 \right) \sin s\,ds\,d\phi \\<br /> &amp;= \int_0^{2\pi} \int_{\cos \alpha}^1 \frac13\left( 3R^2\eta + 3R\eta^2 + \eta^3\right)\,d(\cos s)\,d\phi.<br /> \end{split} Since \eta is a small perturbation, only the term \frac13 (3R^2\eta) is retained.
This is great! What made you think to integrate from ##R## to ##R + \eta##? Becasue ##\eta## is deviation from equilibrium, so for me it wasn't obvious that it implies a change in volume.

EDIT: except now I look at the form and it's a function of ##t## which of course means it grows. Thanks so much!
 
If the position of the surface of the drop changes, then the volume enclosed by it will also change.