Since by Gauss law we
have:
phi(flux)=q/epsilon
This is the flux linked with a closed surface(complete)In this case
what you have to do is that you'll have to manually think that in
which direction/face the flux is not zero.
Imagine a cube with charge q at one of its corner ,now place
another cube besides it touching one of its sides(such that two
faces exactly meet each other), now similarly place two more cubes
beneath these two,now you get 4 cubes,the corner charge is still
not fully covered its visible from one side, place 4 more cubes in
a similar fashion to cover the charge completely. now by the
formula, the flux linked with the whole structure(now a closed
surface) is =q/epsilon not, but the flux linked with one cube will
be = 1/8 *q/(epsilon) because flux has been distributed to 8 cubes
symmetrically.
but even in One(original)cube. You should be able to see electric
field lines originating radially outwards from the cornered charge
in every direction, but note that these lines run parallel to(don't
penetrate) at least 3 faces(two on the sides on at the bottom), so
that means the flux linked with one cube is distributed only to 3
faces in it. So I think the flux linked with one face will be 1/3
of flux linked with one cube i.e
=1/3* 1/8 * q/epsilon
=1/24 * q/epsilon
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