Consider Gauss's law ∮→E⋅→ds=qϵ0. Then, for the situation shown in Fig. at the Gaussian surface.
A
→E due to q2 would be zero
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B
→E due to both q1 and q2 would not be zero
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C
ϕ due to both q1 and q2 would not be zero
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D
ϕ due to q2 would be zero
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Solution
The correct options are B→E due to both q1 and q2 would not be zero Dϕ due to q2 would be zero In L.H.S. of Gauss's law, →E is due to all point charges present in space and ϕ depends only on the enclosed charges.