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Question: Two equal points charges are fixed at \( x = - a \) and \( x = + a \) on the x-axis another point ch...

Two equal points charges are fixed at x=ax = - a and x=+ax = + a on the x-axis another point charge QQ is placed at origin find the change in ‘P.E.’ of particle when it is displaced by a small distance xx along positive x-axis is approximately proportional to:
(A) xx
(B) x2{x^2}
(C) x3{x^3}
(D) x4{x^4}

Explanation

Solution

Hint : Potential energy is a scalar quantity and when more than one charge influences a single charge the net potential energy on that single charge will be the sum of potential energy applied by the other charges on that single charge.

Formula used:
P=KqQr\Rightarrow P = \dfrac{{KqQ}}{r}
Where PP is the electric potential energy, KK is Coulomb constant whose value is 9×109N.m2.C29 \times {10^9}N.{m^2}.{C^{ - 2}} , qq and QQ are the two charges whose PP is being calculated and rr is the distance between them.

Complete step by step answer
Let the two equal point charges be of charge qq and Ui{U_i} be the initial potential energy of QQ and Uf{U_f} be the final potential energy of QQ .
We know that,
P=KqQr\Rightarrow P = \dfrac{{KqQ}}{r}
Where PP is the electric potential energy, KK is Coulomb constant whose value is 9×109N.m2.C29 \times {10^9}N.{m^2}.{C^{ - 2}} , qq and QQ are the two charges whose PP is being calculated and rr is the distance between them.
This KK is the short form of 14πεo\dfrac{1}{{4\pi {\varepsilon _o}}} where εo{\varepsilon _o} is the permittivity in free space i.e. vacuum.
Hence,
Ui=KQqa+KQqa\Rightarrow {U_i} = \dfrac{{KQq}}{a} + \dfrac{{KQq}}{a}
Ui=2KQqa\Rightarrow {U_i} = \dfrac{{2KQq}}{a}
Let the final position be the situation when the charge QQ has moved a distance xx such that x<<ax < < a .
Uf=KQqa+x+KQqax\Rightarrow {U_f} = \dfrac{{KQq}}{{a + x}} + \dfrac{{KQq}}{{a - x}}
Uf=KQq(1a+x+1ax)\Rightarrow {U_f} = KQq\left( {\dfrac{1}{{a + x}} + \dfrac{1}{{a - x}}} \right)
Uf=KQq(2a(a+x)(ax))\Rightarrow {U_f} = KQq\left( {\dfrac{{2a}}{{(a + x)(a - x)}}} \right)
Uf=KQq(2aa2x2)\Rightarrow {U_f} = KQq\left( {\dfrac{{2a}}{{{a^2} - {x^2}}}} \right)
Uf=KQq(2aa2(1(xa)2))\Rightarrow {U_f} = KQq\left( {\dfrac{{2a}}{{{a^2}(1 - {{\left( {\dfrac{x}{a}} \right)}^2})}}} \right)
Using binomial expansion as xa<<1\dfrac{x}{a} < < 1
Uf=KQq(2a(1+(xa)2)a2)\Rightarrow {U_f} = KQq\left( {\dfrac{{2a(1 + {{\left( {\dfrac{x}{a}} \right)}^2})}}{{{a^2}}}} \right)
On further solving,
Uf=KQq(2(a2+(x)2)a3)\Rightarrow {U_f} = KQq\left( {\dfrac{{2({a^2} + {{\left( x \right)}^2})}}{{{a^3}}}} \right)
Uf=2KQqx2a3+2KQqa\Rightarrow {U_f} = \dfrac{{2KQq{x^2}}}{{{a^3}}} + \dfrac{{2KQq}}{a}
We want to know the value of,
ΔU=UfUi\Rightarrow \Delta U = {U_f} - {U_i}
Where ΔU\Delta U is the change in potential energy of the charge QQ .
ΔU=2KQqx2a3+2KQqa2KQqa\Rightarrow \Delta U = \dfrac{{2KQq{x^2}}}{{{a^3}}} + \dfrac{{2KQq}}{a} - \dfrac{{2KQq}}{a}
ΔU=2KQqx2a3\therefore \Delta U = \dfrac{{2KQq{x^2}}}{{{a^3}}}
Hence we can say that ΔUx2\Delta U \propto {x^2}
Therefore the correct answer is (B) x2{x^2} .

Note
The electric P.E. of an arrangement of charges is defined as the work involved in assembling the given system of charges by bringing them close to each other in the given arrangement from an infinite distance. A system of charges always tries to attain an arrangement in which it has minimum electric potential energy.