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roshoka
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How to prove Gauss law geometrically (without coordinates) from Coulomb's law?
I guess I don't understand. How is the divergence theorem equivalent to Gauss' law? It seems like Gauss' integral law is a consequence of the divergence theorem, which is something you prove in Real Analysis class
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How to prove Gauss law geometrically (without coordinates) from Coulomb's law?
This is a proof if you start with Maxwell's equations and the divergence theorem being given. What is your starting point then? Also, are you just downvoting answers you don't like, even if they aren't wrong?
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Electric flux through finite width/ infinitely long plane due to a point charge
Have you tried other Gaussian surfaces besides a cylinder?
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Most probable free path length
put the variables in the question in math notation
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Why do we not care about force from the string on a pendulum or the normal force when skating down a ramp?
I edited it. The dot product is the formula $\vec{F} \cdot \vec{d}$. If you haven't seen that, just pay attention to the part with the cosine (they are equivalent). The formula for work goes to $0$ when the force is perpendicular to the displacement ($cos(90^\circ)=0$). In your examples, gravity isn't always perpendicular to the displacement, so it can still contribute.
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Why do we not care about force from the string on a pendulum or the normal force when skating down a ramp?
The work mentioned here goes to zero when the angle between the force and displacement is $90^\circ$ (assuming there is a nonzero force and displacement). In both cases you mentioned, the gravitational force is not always perpendicular to the displacement.
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