A capacitor consists of two metal plates each \(500 \times 500 \text{ mm}^2\) and spaced \(6 \text{ mm}\) apart. The space between the metal plates is filled with a glass plate of \(4 \text{ mm}\) thickness and a layer of paper of \(2 \text{ mm}\) thickness. The relative permittivity of the glass and paper are 8 and 2 respectively. Neglecting the fringing effect, the capacitance will be (Given that \(\varepsilon_0 = 8.85 \times 10^{-12} \text{ F/m}\)).
- \(983.33 \text{ pF}\)
- \(1475 \text{ pF}\)
- \(6637.5 \text{ pF}\)
- \(9956.25 \text{ pF}\)
Solution
Given:
- Area (\(A\)): \(500 \times 500 \text{ mm}^2 = 250,000 \text{ mm}^2 = 0.25 \text{ m}^2\)
- Permittivity (\(\varepsilon_0\)): \(8.85 \times 10^{-12} \text{ F/m}\)
- Dielectric Layers:
- Glass: \(d_g = 4 \text{ mm} = 4 \times 10^{-3} \text{ m}, \quad \varepsilon_{r,g} = 8\)
- Paper: \(d_p = 2 \text{ mm} = 2 \times 10^{-3} \text{ m}, \quad \varepsilon_{r,p} = 2\)
The arrangement acts as two capacitors in series. The equivalent capacitance \(C\) for composite dielectrics in series is given by:
Equation
\[C = \frac{\varepsilon_0 A}{\frac{d_g}{\varepsilon_{r,g}} + \frac{d_p}{\varepsilon_{r,p}}}\]
Substituting the values:
Equation
\[\begin{aligned}
C &= \frac{(8.85 \times 10^{-12}) \times (0.25)}{\frac{4 \times 10^{-3}}{8} + \frac{2 \times 10^{-3}}{2}} \\
C &= \frac{2.2125 \times 10^{-12}}{(0.5 \times 10^{-3}) + (1.0 \times 10^{-3})} \\
C &= \frac{2.2125 \times 10^{-12}}{1.5 \times 10^{-3}} \\
C &= 1.475 \times 10^{-9} \text{ F} \\
C &= 1475 \text{ pF}
\end{aligned}\]
B
Final Answer
Correct answer: B.
Two point charges \(Q_1 = 10 \text{ } \mu\text{C}\) and \(Q_2 = 20 \text{ } \mu\text{C}\) are placed at coordinates \((1, 1, 0)\) and \((-1, -1, 0)\) respectively. The total electric flux passing through a plane \(z = 20\) will be:
- \(7.5 \text{ } \mu\text{C}\)
- \(13.5 \text{ } \mu\text{C}\)
- \(15.0 \text{ } \mu\text{C}\)
- \(22.5 \text{ } \mu\text{C}\)
Solution
- Total Charge:
Equation
\[Q_{total} = Q_1 + Q_2 = 10 \text{ } \mu\text{C} + 20 \text{ } \mu\text{C} = 30 \text{ } \mu\text{C}\]
- Flux Distribution:
Both charges are located on the \(z = 0\) plane. The plane of interest is \(z = 20\), which is parallel to the plane containing the charges.
By symmetry (assuming the plane \(z=20\) is infinite), the total electric flux emanating from the charges divides equally into two halves:
- Half goes towards the positive \(z\)-direction (\(z > 0\)).
- Half goes towards the negative \(z\)-direction (\(z < 0\)).
- Flux Calculation:
According to Gauss's Law, the total flux is equal to the enclosed charge. For an infinite plane at \(z=20\) enclosing the upper half-space of the charges at \(z=0\), the flux passing through it is:
Equation
\[\Psi_{z=20} = \frac{1}{2} Q_{total}\]
Equation
\[\Psi_{z=20} = \frac{1}{2} (30 \text{ } \mu\text{C}) = 15.0 \text{ } \mu\text{C}\]
C
Final Answer
Correct answer: C.