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The minimum strength of a uniform electric field which can tear a conducting uncharged thin-walled sphere into two parts is known to be E0.

Determine the minimum electric field strength E1 required to tear the sphere of twice as large radius if the thickness of its walls is the same as in the former case.

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The density of charges induced on the sphere is proportional to the electric field strength: σ  E. The force acting on the hemispheres is proportional to the field strength:

where S is the area of the hemisphere, and R is its radius. As the radius of the sphere changes by a factor of n, and the field strength by a factor of k, the force will change by a factor of k2n2. Since the thickness of the sphere walls remains unchanged, the force tearing the sphere per unit length must remain unchanged, i.e. k2n2/n = 1 and k = 1/n = 1/2. Consequently, the minimum electric field strength capable of tearing the conducting shell of twice as large radius is

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