We are given two capacitors, \( C_1 \) (air capacitor) and \( C_2 \) (capacitor filled with a dielectric medium of dielectric constant 5), connected in series to a voltage source of 12V.
The voltage across each capacitor in a series combination is inversely proportional to their capacitances. The total capacitance \( C_{\text{total}} \) of capacitors in series is given by:
\[ \frac{1}{C_{\text{total}}} = \frac{1}{C_1} + \frac{1}{C_2} \]
For \( C_1 \), the capacitance is that of an air capacitor, and for \( C_2 \), the capacitance increases due to the dielectric medium. The capacitance of \( C_2 \) is given by:
\[ C_2 = \kappa \cdot C_1 = 5 \cdot C_1 \]
Substitute \( C_2 = 5 \cdot C_1 \) into the total capacitance equation:
\[ \frac{1}{C_{\text{total}}} = \frac{1}{C_1} + \frac{1}{5C_1} = \frac{6}{5C_1} \]
Thus, the total capacitance is:
\[ C_{\text{total}} = \frac{5}{6} C_1 \]
Now, the voltage drop across each capacitor is proportional to the inverse of its capacitance. The voltage drop across \( C_1 \) is:
\[ V_1 = V \cdot \frac{C_2}{C_{\text{total}}} = 12 \cdot \frac{5C_1}{6C_1} = 10V \]
And the voltage drop across \( C_2 \) is:
\[ V_2 = V - V_1 = 12V - 10V = 2V \]
Thus, the voltage drops across the two capacitors are:
Correct Answer: (1) 2V and 10V
Let \( C_1 \) be the air capacitor with capacitance \( C \), and \( C_2 \) be the identical capacitor with dielectric, so its capacitance becomes \( 5C \). In series connection, the charge \( Q \) on both capacitors is the same. The voltage across a capacitor is given by: \[ V = \frac{Q}{C} \] Let the voltages across \( C_1 \) and \( C_2 \) be \( V_1 \) and \( V_2 \). Since they are in series, \[ V_1 + V_2 = 12\ V \] Also, \[ V_1 = \frac{Q}{C}, \quad V_2 = \frac{Q}{5C} \Rightarrow \frac{V_1}{V_2} = \frac{\frac{Q}{C}}{\frac{Q}{5C}} = 5 \Rightarrow V_1 = 5 V_2 \] Substitute in total voltage: \[ V_1 + V_2 = 12 \Rightarrow 5V_2 + V_2 = 12 \Rightarrow 6V_2 = 12 \Rightarrow V_2 = 2\ V,\quad V_1 = 10\ V \] So, the potential drops are 10 V across the air capacitor and 2 V across the dielectric-filled capacitor.
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
Kepler's second law (law of areas) of planetary motion leads to law of conservation of