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Question: ABCD is a square of side \( 0.2m \) . Point charges of \( + 2 \times {10^{ - 9}}C \) , \( + 4 \times...

ABCD is a square of side 0.2m0.2m . Point charges of +2×109C+ 2 \times {10^{ - 9}}C , +4×109C+ 4 \times {10^{ - 9}}C and +8×109C+ 8 \times {10^{ - 9}}C are located at the corners A, B and C respectively of the square. What is the work done in transferring a charge of +2×109C+ 2 \times {10^{ - 9}}C from D to the point of intersection of the diagonals of the square?

Explanation

Solution

Hint : To solve this question, we need to find out the potentials at the point D and at the center of the square. Then by calculating the change in potential for the two points, we can calculate the value of work done.

Formula used: The formula which is used to solve this question is given by
V=kqrV = \dfrac{{kq}}{r} , here VV is the potential due to a point charge of qq at the point which is at a distance of rr from it.
W=qΔVW = q\Delta V , here WW is the work done in transferring a charge of qq from one point to the other, between which the potential difference of ΔV\Delta V is there.

Complete step by step answer:
Consider the square ABCD of side 0.2m0.2m on which the three point charges of +2×109C+ 2 \times {10^{ - 9}}C , +4×109C+ 4 \times {10^{ - 9}}C and +8×109C+ 8 \times {10^{ - 9}}C are located.

Applying Pythagoras theorem in the triangle AOD we get
AO2+DO2=AD2A{O^2} + D{O^2} = A{D^2}
We know that in a square, the distance of the centre from each vertex is equal. Therefore substituting DO=AODO = AO we get
2AO2=AD22A{O^2} = A{D^2}
AO2=AD22\Rightarrow A{O^2} = \dfrac{{A{D^2}}}{2}
Taking square root both sides
AO=AD2AO = \dfrac{{AD}}{{\sqrt 2 }}
The side of the square is given to be equal to 0.2m0.2m . Therefore we have
AO=0.22mAO = \dfrac{{0.2}}{{\sqrt 2 }}m
Therefore we have
AO=BO=CO=DO=0.22mAO = BO = CO = DO = \dfrac{{0.2}}{{\sqrt 2 }}m (1)
Now, we calculate the net potential at the point D.
The potential will be due to all the three charges q1{q_1} , q2{q_2} and q3{q_3} . So it is given by
VD=Vq1+Vq2+Vq3{V_D} = {V_{{q_1}}} + {V_{{q_2}}} + {V_{{q_3}}} (2)
We know that the potential due to charge at a point is given by
V=KqrV = \dfrac{{Kq}}{r}
So from (2) we have
VD=Kq1AD+Kq2BD+Kq3CD{V_D} = \dfrac{{K{q_1}}}{{AD}} + \dfrac{{K{q_2}}}{{BD}} + \dfrac{{K{q_3}}}{{CD}}
VD=K(q1AD+q2BD+q3CD)\Rightarrow {V_D} = K\left( {\dfrac{{{q_1}}}{{AD}} + \dfrac{{{q_2}}}{{BD}} + \dfrac{{{q_3}}}{{CD}}} \right)
Since the side of the square is 0.2m0.2m , so AD=BD=CD=0.2mAD = BD = CD = 0.2m . Also according to the qe=uestion we have q1=+2×109C{q_1} = + 2 \times {10^{ - 9}}C , q2=+4×109C{q_2} = + 4 \times {10^{ - 9}}C , and q3=+8×109C{q_3} = + 8 \times {10^{ - 9}}C . Substituting these above we get
VD=K(2×1090.2+4×1090.2+8×1090.2){V_D} = K\left( {\dfrac{{2 \times {{10}^{ - 9}}}}{{0.2}} + \dfrac{{4 \times {{10}^{ - 9}}}}{{0.2}} + \dfrac{{8 \times {{10}^{ - 9}}}}{{0.2}}} \right)
VD=2×1090.2K(1+2+4)\Rightarrow {V_D} = \dfrac{{2 \times {{10}^{ - 9}}}}{{0.2}}K\left( {1 + 2 + 4} \right)
On solving we get
VD=70×109K{V_D} = 70 \times {10^{ - 9}}K (2)
Now, we calculate the potential at the center O.
As stated above, the potential at the center will be due to the charges q1{q_1} , q2{q_2} and q3{q_3} . So it is given by
VO=Vq1+Vq2+Vq3{V_O} = {V_{{q_1}}} + {V_{{q_2}}} + {V_{{q_3}}}
VO=K(q1AO+q2BO+q3CO)\Rightarrow {V_O} = K\left( {\dfrac{{{q_1}}}{{AO}} + \dfrac{{{q_2}}}{{BO}} + \dfrac{{{q_3}}}{{CO}}} \right)
From (1) AO=BO=CO=0.22mAO = BO = CO = \dfrac{{0.2}}{{\sqrt 2 }}m . Also q1=+2×109C{q_1} = + 2 \times {10^{ - 9}}C , q2=+4×109C{q_2} = + 4 \times {10^{ - 9}}C , and q3=+8×109C{q_3} = + 8 \times {10^{ - 9}}C . Substituting these above we get
VO=K(22×1090.2+42×1090.2+82×1090.2){V_O} = K\left( {\dfrac{{2\sqrt 2 \times {{10}^{ - 9}}}}{{0.2}} + \dfrac{{4\sqrt 2 \times {{10}^{ - 9}}}}{{0.2}} + \dfrac{{8\sqrt 2 \times {{10}^{ - 9}}}}{{0.2}}} \right)
VO=22×1090.2K(1+2+4)\Rightarrow {V_O} = \dfrac{{2\sqrt 2 \times {{10}^{ - 9}}}}{{0.2}}K\left( {1 + 2 + 4} \right)
On solving we get
VO=702×109K{V_O} = 70\sqrt 2 \times {10^{ - 9}}K (3)
Now, we know that the work done is given by
W=qΔVW = q\Delta V
According to the question, the charge of +2×109C+ 2 \times {10^{ - 9}}C is transferred from the point D to the point O. So we get
W=+2×109(VOVD)W = + 2 \times {10^{ - 9}}\left( {{V_O} - {V_D}} \right)
From (2) and (3)
W=+2×109(702×109K70×109K)W = + 2 \times {10^{ - 9}}\left( {70\sqrt 2 \times {{10}^{ - 9}}K - 70 \times {{10}^{ - 9}}K} \right)
W=2×109×70×109K(21)\Rightarrow W = 2 \times {10^{ - 9}} \times 70 \times {10^{ - 9}}K\left( {\sqrt 2 - 1} \right)
Substituting K=9×109Nm2C2K = 9 \times {10^9}\dfrac{{N{m^2}}}{{{C^2}}} we get
W=2×109×70×109×9×109(21)W = 2 \times {10^{ - 9}} \times 70 \times {10^{ - 9}} \times 9 \times {10^9}\left( {\sqrt 2 - 1} \right)
On solving we get
W=5.22×107JW = 5.22 \times {10^{ - 7}}J
Hence, the required work done is equal to 5.22×107J5.22 \times {10^{ - 7}}J .

Note:
This question could also be attempted by considering the system of all the four charges given in the question. Then calculate the potential energy of the system for the two configurations, with the fourth charge of +2×109C+ 2 \times {10^{ - 9}}C at the point D in the first configuration, and at the center O in the second configuration. Finally, calculating the change in the potential energy of the system, we will get the final answer.