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Question: A, B, C, D, P and Q are points in a uniform electric field. The potentials at these points are \(V(A...

A, B, C, D, P and Q are points in a uniform electric field. The potentials at these points are V(A)=2r,V(P)=V(B)=V(D)=5V,V(C)=8VV(A) = 2r, V(P) = V(B) = V(D) = 5V, V(C) = 8V. The electric field at P is

(A) 10Vm110V{m^{ - 1}} along PQ
(B) 152Vm115\sqrt 2 V{m^{ - 1}} along PA
(C) 5Vm15V{m^{ - 1}} along PC
(D) 5Vm15V{m^{ - 1}} along PA

Explanation

Solution

In order to solve this problem, first we calculate the net potential at point P and then calculate the electric field at point P by using following formula –
E=dVdr\vec E = - \dfrac{{dV}}{{dr}}
Where E=\vec E = electric field
V=V = Electric potential

Complete step by step answer:
We know that the relation between electric field and electric potential is given as
E=dVdr\vec E = - \dfrac{{dV}}{{dr}}
In x-direction
Ex=dVdx{E_x} = - \dfrac{{dV}}{{dx}}
According to diagram
dx=0.2mdx = 0.2m
dV=V0VAdV = {V_0} - {V_A}
So, Ex=(V0VA)0.2{E_x} = \dfrac{{ - ({V_0} - {V_A})}}{{0.2}}
Given that V(D)=5VV(D) = 5V
V(A)=2VV(A) = 2V
So, Ex=(52)0.2=30.2{E_x} = \dfrac{{ - (5 - 2)}}{{0.2}} = \dfrac{{ - 3}}{{0.2}}
Ex=302=15Vm{E_x} = \dfrac{{ - 30}}{2} = - 15\dfrac{V}{m} …..(1)
In y-direction
Ey=dVdy{E_y} = - \dfrac{{dV}}{{dy}}
According to diagram
dy=0.2mdy = 0.2m
dV=VBVAdV = {V_B} - {V_A}
So, Ey=(VBVA)0.2{E_y} = - \dfrac{{({V_B} - {V_A})}}{{0.2}}
Given that V(B)=5V,V(A)=2VV(B) = 5V,V(A) = 2V
Ey=(52)0.2=30.2{E_y} = \dfrac{{ - (5 - 2)}}{{0.2}} = \dfrac{{ - 3}}{{0.2}}
Ey=302=15Vm{E_y} = \dfrac{{ - 30}}{2} = - 15\dfrac{V}{m} …..(2)
E=Exi^+Eyj^\because \vec E = {E_x}\hat i + {E_y}\hat j
So, E=Ex2+Ey2|\vec E| = \sqrt {E_x^2 + E_y^2}
From equation 1 & 2
Electric field E at P is
=(15)2+(15)2= \sqrt {{{( - 15)}^2} + {{( - 15)}^2}}
=2(15)2= \sqrt {2{{(15)}^2}}
=215=152Vm= \sqrt 2 15 = 15\sqrt 2 \dfrac{V}{m}
Hence, the electric field at point P is 152Vm115\sqrt 2 V{m^{ - 1}} along PA.

Note: In many cases potential is the function of x, y and z then electric field is given as
E=Vxi^Vyj^Vzk^\vec E = \dfrac{{ - \partial V}}{{\partial x}}\hat i - \dfrac{{\partial V}}{{\partial y}}\hat j - \dfrac{{\partial V}}{{\partial z}}\hat k
Where Ex=Vx,Ey=Vy,Ez=Vz{E_x} = \dfrac{{ - \partial V}}{{\partial x}},{E_y} = - \dfrac{{\partial V}}{{\partial y}},{E_z} = \dfrac{{ - \partial V}}{{\partial z}}