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Question: The electric field due to electric potential \[V = 2{x^2} - 4x\] (A) \[(4x + 4){\text{ }}i\] (B) ...

The electric field due to electric potential V=2x24xV = 2{x^2} - 4x

(A) (4x+4) i(4x + 4){\text{ }}i

(B) (4x4) i(4x - 4){\text{ }}i

(C) (4x+4) i( - 4x + 4){\text{ }}i

(D) (4x4) i( - 4x - 4){\text{ }}i

Explanation

Solution

The electric field at a point is defined as the negative of gradient of the potential at that point, where gradient is the dot product of Del operator with quantity V. Since only the x - component is here we get the final answer with unit vector i^\hat i.

Complete step-by-step answer:

As we know that,

E=.V= (dVdxi^+dVdyj^+dVdzk^)\overrightarrow E = - \overrightarrow \nabla .V = {\text{ }} - \left( {\dfrac{{dV}}{{dx}}\widehat i + \dfrac{{dV}}{{dy}}\widehat j + \dfrac{{dV}}{{dz}}\widehat k} \right)

This means that change in potential of a point with respect to the distance in 3 axes is termed as electric field. The negative sign is present to show that the potential of a point decreases with distance which will create a negative potential gradient.

Solving the above equation we obtain:

E= d(2x24x)dxi^\overrightarrow E = {\text{ }} - \dfrac{{d(2{x^2} - 4x)}}{{dx}}\widehat i

E= (4x  4)i^E = {\text{ }} - (4x{\text{ }} - {\text{ }}4)\hat i

E=( 4x + 4) i^E = ({\text{ }} - 4x{\text{ }} + {\text{ }}4)\widehat {{\text{ }}i}

As the expression of electric field is only dependent on x, i.e. the coordinate in the i^\widehat {\text{i}} direction, we will add the unit vectori^\widehat {\text{i}} to denote the direction of the Electric field.

Therefore, the correct answer is option C.

Note: The potential and potential difference of a point is a scalar quantity but electric field is a vector quantity. An electric field is a vector quantity equal to the negative of the potential gradient. E=dVdrE = - \dfrac{{dV}}{{dr}}