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Concepts Of Physics MCQ Edition [Volume 2]
Exam
Concepts Of Physics MCQ Edition [Volume 2]
Subject
Physics
Chapter
Capacitors

Concepts Of Physics MCQ Edition [Volume 2] · Physics · Capacitors

Determine the equivalent capacitances between the specified points...

Determine the equivalent capacitances between the specified points for the combinations illustrated in the figure.
Determine the equivalent capacitances between the specified points for the combinations illustrated in the figure.

Options

  1. A(a) 114μF\dfrac{11}{4} \mu\text{F}, (b) 116μF\dfrac{11}{6} \mu\text{F}, (c) 8μF8 \mu\text{F}, (d) 8μF8 \mu\text{F}
  2. B(a) 116μF\dfrac{11}{6} \mu\text{F}, (b) 114μF\dfrac{11}{4} \mu\text{F}, (c) 12μF12 \mu\text{F}, (d) 16μF16 \mu\text{F}
  3. C(a) 116μF\dfrac{11}{6} \mu\text{F}, (b) 114μF\dfrac{11}{4} \mu\text{F}, (c) 8μF8 \mu\text{F}, (d) 8μF8 \mu\text{F}
  4. D(a) 2μF2 \mu\text{F}, (b) 4μF4 \mu\text{F}, (c) 8μF8 \mu\text{F}, (d) 8μF8 \mu\text{F}

Correct answer

C. (a) 116μF\dfrac{11}{6} \mu\text{F}, (b) 114μF\dfrac{11}{4} \mu\text{F}, (c) 8μF8 \mu\text{F}, (d) 8μF8 \mu\text{F}

Step-by-step solution

For circuit (a):
Let the input node be at potential VV and the output node be at 00. Let the potentials at the top and bottom junctions be xx and yy respectively.
Applying Kirchhoff's Current Law (KCL) at the top junction:
(x−V)×1+(x−0)×3+(x−y)×4=0⇒8x−4y=V(x - V) \times 1 + (x - 0) \times 3 + (x - y) \times 4 = 0 \Rightarrow 8x - 4y = V
Applying KCL at the bottom junction:
(y−V)×3+(y−0)×1+(y−x)×4=0⇒−4x+8y=3V(y - V) \times 3 + (y - 0) \times 1 + (y - x) \times 4 = 0 \Rightarrow -4x + 8y = 3V
Solving these two equations, we get x=5V12x = \dfrac{5V}{12} and y=7V12y = \dfrac{7V}{12}.
The total charge QQ supplied by the source is the sum of charges on the input capacitors:
Q=(V−x)×1+(V−y)×3=(V−5V12)×1+(V−7V12)×3=7V12+15V12=22V12=11V6Q = (V - x) \times 1 + (V - y) \times 3 = \left(V - \dfrac{5V}{12}\right) \times 1 + \left(V - \dfrac{7V}{12}\right) \times 3 = \dfrac{7V}{12} + \dfrac{15V}{12} = \dfrac{22V}{12} = \dfrac{11V}{6}
The equivalent capacitance is Ceq=QV=116μFC_{eq} = \dfrac{Q}{V} = \dfrac{11}{6} \mu\text{F}.

For circuit (b):
Let the input be at VV and output at 00. Let the potentials at the top, middle, and bottom junctions be VCV_C, VDV_D, and VEV_E respectively.
Applying KCL at the three junctions:
Top: (VC−V)×1+VC×3+(VC−VD)×4=0⇒8VC−4VD=V(V_C - V) \times 1 + V_C \times 3 + (V_C - V_D) \times 4 = 0 \Rightarrow 8V_C - 4V_D = V
Middle: (VD−V)×2+VD×2+(VD−VC)×4+(VD−VE)×4=0⇒12VD−4VC−4VE=2V(V_D - V) \times 2 + V_D \times 2 + (V_D - V_C) \times 4 + (V_D - V_E) \times 4 = 0 \Rightarrow 12V_D - 4V_C - 4V_E = 2V
Bottom: (VE−V)×3+VE×1+(VE−VD)×4=0⇒8VE−4VD=3V(V_E - V) \times 3 + V_E \times 1 + (V_E - V_D) \times 4 = 0 \Rightarrow 8V_E - 4V_D = 3V
Adding the top and bottom equations gives 8(VC+VE)−8VD=4V⇒VC+VE=VD+V28(V_C + V_E) - 8V_D = 4V \Rightarrow V_C + V_E = V_D + \dfrac{V}{2}.
Substituting this into the middle equation gives 12VD−4(VD+V2)=2V⇒8VD=4V⇒VD=V212V_D - 4\left(V_D + \dfrac{V}{2}\right) = 2V \Rightarrow 8V_D = 4V \Rightarrow V_D = \dfrac{V}{2}.
Using VD=V2V_D = \dfrac{V}{2} in the top and bottom equations yields VC=3V8V_C = \dfrac{3V}{8} and VE=5V8V_E = \dfrac{5V}{8}.
Total charge Q=(V−VC)×1+(V−VD)×2+(V−VE)×3=5V8+V+9V8=22V8=11V4Q = (V - V_C) \times 1 + (V - V_D) \times 2 + (V - V_E) \times 3 = \dfrac{5V}{8} + V + \dfrac{9V}{8} = \dfrac{22V}{8} = \dfrac{11V}{4}.
The equivalent capacitance is Ceq=QV=114μFC_{eq} = \dfrac{Q}{V} = \dfrac{11}{4} \mu\text{F}.

For circuit (c):
The upper part of the circuit forms a Wheatstone bridge. The ratio of capacitances in the top branch is 24=12\dfrac{2}{4} = \dfrac{1}{2} and in the middle branch is 48=12\dfrac{4}{8} = \dfrac{1}{2}.
Since the bridge is balanced, no charge flows through the 5μF5 \mu\text{F} capacitor, and it can be removed.
The equivalent capacitance of the bridge is 2×42+4+4×84+8=43+83=4μF\dfrac{2 \times 4}{2 + 4} + \dfrac{4 \times 8}{4 + 8} = \dfrac{4}{3} + \dfrac{8}{3} = 4 \mu\text{F}.
This is in parallel with the bottom 4μF4 \mu\text{F} capacitor, so Ceq=4+4=8μFC_{eq} = 4 + 4 = 8 \mu\text{F}.

For circuit (d):
The circuit consists of four parallel branches. The ratio of capacitances in each branch is 24=12\dfrac{2}{4} = \dfrac{1}{2}, 48=12\dfrac{4}{8} = \dfrac{1}{2}, 48=12\dfrac{4}{8} = \dfrac{1}{2}, and 24=12\dfrac{2}{4} = \dfrac{1}{2}.
Because the ratios are identical, the midpoints of all four branches are at the same potential. Thus, the three 6μF6 \mu\text{F} capacitors have no potential difference across them and can be removed.
The equivalent capacitance is the sum of the series combinations of each branch:
Ceq=2×42+4+4×84+8+4×84+8+2×42+4=43+83+83+43=243=8μFC_{eq} = \dfrac{2 \times 4}{2 + 4} + \dfrac{4 \times 8}{4 + 8} + \dfrac{4 \times 8}{4 + 8} + \dfrac{2 \times 4}{2 + 4} = \dfrac{4}{3} + \dfrac{8}{3} + \dfrac{8}{3} + \dfrac{4}{3} = \dfrac{24}{3} = 8 \mu\text{F}.

Answer: (a) 116μF\dfrac{11}{6} \mu\text{F}, (b) 114μF\dfrac{11}{4} \mu\text{F}, (c) 8μF8 \mu\text{F}, (d) 8μF8 \mu\text{F}
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