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Question: Two charges \({{q}_{1}}\) and \({{q}_{2}}\) are placed 30cm apart, as shown in figure. A third charg...

Two charges q1{{q}_{1}} and q2{{q}_{2}} are placed 30cm apart, as shown in figure. A third charge q3{{q}_{3}} is moved along the arc of a circle of radius 40cm from C to D. the change in the potential energy of the system is q34πε0k\dfrac{{{q}_{3}}}{4\pi {{\varepsilon }_{0}}}k , where kk is
A.8q18{{q}_{1}}
B.6q16{{q}_{1}}
C.8q28{{q}_{2}}
D.6q26{{q}_{2}}

Explanation

Solution

We are given two charges and a third charge is entering their in space. These already present charges had some potential energy due to each other and third charge at point C. This will be considered as the initial potential energy of the system. When a third charge is introduced, they develop more potential energy due to it. This sums up as the final potential energy. We will subtract the initial and final potential energies to get the change in potential energy.

Complete answer:
The potential energy, UU of any charged body is given as:
U=14πε0.q1q2rU=\dfrac{1}{4\pi {{\varepsilon }_{0}}}.\dfrac{{{q}_{1}}{{q}_{2}}}{r}
Where,
q1={{q}_{1}}= charge on first body
q2={{q}_{2}}= charge on second body
r=r= distance between the two charges
We have AB=30cm,AC=40cmAB=30cm,AC=40cm, thus by Pythagorean triplets, BC is given as:
BC=AB2+AC2 BC=302+402 BC=900+1600 BC=2500 \begin{aligned} & BC=\sqrt{A{{B}^{2}}+A{{C}^{2}}} \\\ & \Rightarrow BC=\sqrt{{{30}^{2}}+{{40}^{2}}} \\\ & \Rightarrow BC=\sqrt{900+1600} \\\ & \Rightarrow BC=\sqrt{2500} \\\ \end{aligned}
BC=50cm\therefore BC=50cm
Also,
BD=ADAB BD=4030 BD=10cm \begin{aligned} & BD=AD-AB \\\ & \Rightarrow BD=40-30 \\\ & \Rightarrow BD=10cm \\\ \end{aligned}
For a discrete system of charges, the potential energy is expressed as the sum of all potential energies of the system.
U=14πε0[q1q2r12+q2q3r23+q1q3r13]U=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\left[ \dfrac{{{q}_{1}}{{q}_{2}}}{{{r}_{12}}}+\dfrac{{{q}_{2}}{{q}_{3}}}{{{r}_{23}}}+\dfrac{{{q}_{1}}{{q}_{3}}}{{{r}_{13}}} \right]
For the initial potential energy when q3{{q}_{3}} is at point C,
r12=AB=30cm=0.3m{{r}_{12}}=AB=30cm=0.3m, r23=BC=50cm=0.5m{{r}_{23}}=BC=50cm=0.5m, r13=AC=40cm=0.4m{{r}_{13}}=AC=40cm=0.4m
The potential energy is calculated as:
Ui=14πε0[q1q2AB+q2q3BC+q1q3AC]{{U}_{i}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\left[ \dfrac{{{q}_{1}}{{q}_{2}}}{AB}+\dfrac{{{q}_{2}}{{q}_{3}}}{BC}+\dfrac{{{q}_{1}}{{q}_{3}}}{AC} \right]
Ui=14πε0[q1q20.3+q2q30.5+q1q30.4]\Rightarrow {{U}_{i}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\left[ \dfrac{{{q}_{1}}{{q}_{2}}}{0.3}+\dfrac{{{q}_{2}}{{q}_{3}}}{0.5}+\dfrac{{{q}_{1}}{{q}_{3}}}{0.4} \right] ………………… equation (1)
For the final potential energy when q3{{q}_{3}} is at point D,
r12=AB=30cm=0.3m{{r}_{12}}=AB=30cm=0.3m, r23=BD=10cm=0.1m{{r}_{23}}=BD=10cm=0.1m, r13=AD=40cm=0.4m{{r}_{13}}=AD=40cm=0.4m
The potential energy is calculated as:
Uf=14πε0[q1q2AB+q2q3BD+q1q3AD]{{U}_{f}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\left[ \dfrac{{{q}_{1}}{{q}_{2}}}{AB}+\dfrac{{{q}_{2}}{{q}_{3}}}{BD}+\dfrac{{{q}_{1}}{{q}_{3}}}{AD} \right]
Uf=14πε0[q1q20.3+q2q30.1+q1q30.4]\Rightarrow {{U}_{f}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\left[ \dfrac{{{q}_{1}}{{q}_{2}}}{0.3}+\dfrac{{{q}_{2}}{{q}_{3}}}{0.1}+\dfrac{{{q}_{1}}{{q}_{3}}}{0.4} \right] ………………… equation (2)
Change in potential energy= final potential energy – initial potential energy
ΔU=UfUi\Rightarrow \Delta U={{U}_{f}}-{{U}_{i}}
From equation (1) and (2),
ΔU=14πε0[q1q20.3+q2q30.1+q1q30.4]14πε0[q1q20.3+q2q30.5+q1q30.4]\Rightarrow \Delta U=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\left[ \dfrac{{{q}_{1}}{{q}_{2}}}{0.3}+\dfrac{{{q}_{2}}{{q}_{3}}}{0.1}+\dfrac{{{q}_{1}}{{q}_{3}}}{0.4} \right]-\dfrac{1}{4\pi {{\varepsilon }_{0}}}\left[ \dfrac{{{q}_{1}}{{q}_{2}}}{0.3}+\dfrac{{{q}_{2}}{{q}_{3}}}{0.5}+\dfrac{{{q}_{1}}{{q}_{3}}}{0.4} \right]
Taking 14πε0\dfrac{1}{4\pi {{\varepsilon }_{0}}} common, we get
ΔU=14πε0[q1q20.3+q2q30.1+q1q30.4q1q20.3q2q30.5q1q30.4]\Rightarrow \Delta U=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\left[ \dfrac{{{q}_{1}}{{q}_{2}}}{0.3}+\dfrac{{{q}_{2}}{{q}_{3}}}{0.1}+\dfrac{{{q}_{1}}{{q}_{3}}}{0.4}-\dfrac{{{q}_{1}}{{q}_{2}}}{0.3}-\dfrac{{{q}_{2}}{{q}_{3}}}{0.5}-\dfrac{{{q}_{1}}{{q}_{3}}}{0.4} \right]
ΔU=14πε0[q2q3(10.110.5)] ΔU=14πε0[q2q3(0.50.10.1(0.5))] \begin{aligned} & \Rightarrow \Delta U=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\left[ {{q}_{2}}{{q}_{3}}\left( \dfrac{1}{0.1}-\dfrac{1}{0.5} \right) \right] \\\ & \Rightarrow \Delta U=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\left[ {{q}_{2}}{{q}_{3}}\left( \dfrac{0.5-0.1}{0.1\left( 0.5 \right)} \right) \right] \\\ \end{aligned}
ΔU=14πε0[q2q30.400.05]\Rightarrow \Delta U=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\left[ {{q}_{2}}{{q}_{3}}\dfrac{0.40}{0.05} \right]
ΔU=14πε08q2q3\Rightarrow \Delta U=\dfrac{1}{4\pi {{\varepsilon }_{0}}}8{{q}_{2}}{{q}_{3}}
Therefore, the change in potential energy is equal to 14πε08q2q3\dfrac{1}{4\pi {{\varepsilon }_{0}}}8{{q}_{2}}{{q}_{3}}.

Hence, the correct option is (C) 8q28{{q}_{2}}

Note:
Every charged body has its own electric potential. However, the potential energy of any charged body is always measured with respect to some other charged body in its vicinity. This is because any charged body develops a potential energy due to interaction with another charged body near it. The potential energy of any charged body is zero if it is isolated in space.