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Question: ABCD is a square of side \(2m\). Charges of \(5nC\), \(10nC\) and \[ - 5nC\] are at corners A, B and...

ABCD is a square of side 2m2m. Charges of 5nC5nC, 10nC10nC and 5nC - 5nC are at corners A, B and C respectively. What is the work done in transferring a charge of 5μC5\mu C from D to the point of intersection of the diagonals?

Explanation

Solution

Here, the system consists of four charges out of which the position of one charge is being changed. As the particles are charged, they possess an electrostatic energy among themselves. This energy is the electrostatic potential energy. This energy depends on the relative positions of the charges. So, if you want to change the position of any charge, you need to work against this electrostatic potential energy.

Complete step by step answer:

Potential energy is an energy of a system, against which a work is done in order to bring changes. Hence, we say that the work required will be equal to the change in the potential energy of the system. Mathematically,
W=ΔU W=UfUi  W = \Delta U \\\ \Rightarrow W = {U_f} - {U_i} \\\
The potential energy can be written in terms of potential. Mathematically,
U=qVU = qV
Therefore, we can write Uf=qVf{U_f} = q{V_f} and Ui=qVi{U_i} = q{V_i}.
In this case, the only change happening is the position of the charge 5μC5\mu C from point D to the centre of the square. Hence, we conclude that the work done will be equal to change in the potential energy related to the charge 5μC5\mu C.
Let q1{q_1} be the charge at point A, q2{q_2} is the charge at point B, q3{q_3} is the charge at point C.
Now, the potential energy of the 5μC5\mu Ccharge at point D is given as
UD=qVD UD=q(q14πεor1+q24πεor2+q34πεor3) UD=q4πε0(q1r1+q2r2+q3r3) UD=5×106×9×109(5×1092+10×10922+(5×109)2) UD=159.099μJ  {U_D} = q{V_D} \\\ \Rightarrow {U_D} = q\left( {\dfrac{{{q_1}}}{{4\pi {\varepsilon _o}{r_1}}} + \dfrac{{{q_2}}}{{4\pi {\varepsilon _o}{r_2}}} + \dfrac{{{q_3}}}{{4\pi {\varepsilon _o}{r_3}}}} \right) \\\ \Rightarrow {U_D} = \dfrac{q}{{4\pi {\varepsilon _0}}}\left( {\dfrac{{{q_1}}}{{{r_1}}} + \dfrac{{{q_2}}}{{{r_2}}} + \dfrac{{{q_3}}}{{{r_3}}}} \right) \\\ \Rightarrow {U_D} = 5 \times {10^{ - 6}} \times 9 \times {10^9}\left( {\dfrac{{5 \times {{10}^{ - 9}}}}{2} + \dfrac{{10 \times {{10}^{ - 9}}}}{{2\sqrt 2 }} + \dfrac{{( - 5 \times {{10}^{ - 9}})}}{2}} \right) \\\ \Rightarrow {U_D} = 159.099\mu J \\\
And the potential energy of the 5μC5\mu Ccharge at point O is given as
UO=q(q14πε0r1+q24πε0r2+q34πε0r3) UO=q4πε0(q1r1+q2r2+q3r3) UO=5×106×9×109(5×1092+10×1092+(5×109)2) UO=318.198μJ  \Rightarrow {U_O} = q\left( {\dfrac{{{q_1}}}{{4\pi {\varepsilon _0}{r_1}'}} + \dfrac{{{q_2}}}{{4\pi {\varepsilon _0}{r_2}'}} + \dfrac{{{q_3}}}{{4\pi {\varepsilon _0}{r_3}'}}} \right) \\\ \Rightarrow {U_O} = \dfrac{q}{{4\pi {\varepsilon _0}}}\left( {\dfrac{{{q_1}}}{{{r_1}'}} + \dfrac{{{q_2}}}{{{r_2}'}} + \dfrac{{{q_3}}}{{{r_3}'}}} \right) \\\ \Rightarrow {U_O} = 5 \times {10^{ - 6}} \times 9 \times {10^9}\left( {\dfrac{{5 \times {{10}^{ - 9}}}}{{\sqrt 2 }} + \dfrac{{10 \times {{10}^{ - 9}}}}{{\sqrt 2 }} + \dfrac{{( - 5 \times {{10}^{ - 9}})}}{{\sqrt 2 }}} \right) \\\ {U_O} = 318.198\mu J \\\
Here, q1{q_1} is the charge at point A, q2{q_2} is the charge at point B, q3{q_3} is the charge at point C.
The work done will be W=UfUiW = {U_f} - {U_i}. Here Uf=UO{U_f} = {U_O} and Ui=UD{U_i} = {U_D}
W=318.198159.099 W=159.099μJ  \Rightarrow W = 318.198 - 159.099 \\\ \therefore W = 159.099\mu J \\\
Hence, the work done in transferring a charge of 5μC5\mu C from D to the point of intersection of the diagonals is 159.099μJ159.099\mu J.

Note:
Here, the initial velocity and the final velocity of the charge 5μC5\mu C is zero, implying the change in kinetic energy is zero or the initial and final both the kinetic energies are zero. If they were not zero, we still would have applied the same logic for finding work, but instead of finding only the work required to change the potential energy we would be finding work required to change the potential energy plus the work required to change the kinetic energy.