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M. next

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The approach taken by most of electrodynamics textbooks is as follows:

"If we wish to consider the problem of an insulated conducting sphere with total charge Q in the presence of a point charge q, we can build up the solution for the potential by

**linear superposition**. IN an operational sense, we can imagine that we start with the grounded conducting sphere (with its charge q' distributed over its surface). We then disconnect the ground wire and add to the sphere an amount of charge (-q'). This brings the total charge on the sphere up to Q. To find the potential we merely note that the added charge (Q-q') will distribute itself uniformly over the surface, since the electrostatic forces due to the point charge q are already balanced by the charge q'. Hence the potential due to the added charge (Q-q') will be the same as if a point charge of that magnitude were at the origin, at least for points outside the sphere." (Chapter 2, p. 61) from Electrodynamics by J. D. Jackson.

Then to find the potential, the author uses the superposition principle (the author superposes the potential due to q, q' and (Q-q').

My question here is: Can we find the electric field of this charges sphere directly from Gauss's law and then find the potential due to it as a whole & then superpose it with the charge q outside the sphere? (i.e, without the referring to q') If not, why?