We know that "\\vec{E} = -\\nabla \\varphi."
The change of potential is "\\varphi(A) - \\varphi(B) = \\int\\limits_A^B \\vec{E}\\cdot d\\vec{l}" .
For the small distance we'll get "\\varphi(A) - \\varphi(B) \\approx \\vec{E}\\cdot d\\vec{n} = (20i+30j)(30i-20j) = 60 - 0 + 0 - 60 = 0."
So the change of potential is zero. It is clear, because the change is perpendicular to the electric field, so the potential remains constant.
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