The initial energy stored in the charged capacitor is given by the formula:
\(E_i = \frac{1}{2} C V^2\)
Substitute the values:
\(E_i = \frac{1}{2} \times 900 \times 10^{-6} \times (100)^2 = 4.5 \, \text{J}\)
After connecting the uncharged capacitor, the total charge gets shared between the two capacitors. The final voltage across each capacitor becomes half of the initial voltage because the two capacitors are identical:
\(V_f = \frac{V_i}{2} = \frac{100}{2} = 50 \, \text{V}\)
The final energy stored in each capacitor is:
\(E_f = \frac{1}{2} C V_f^2 = \frac{1}{2} \times 900 \times 10^{-6} \times (50)^2 = 2.25 \, \text{J}\)
The total final energy in both capacitors is:
\(2 \times E_f = 2 \times 2.25 = 4.5 \, \text{J}\)
The energy loss during this process is the difference between the initial and final energy, which is:
\(\Delta E = E_i - 2 \times E_f = 4.5 - 4.5 = 0 \, \text{J}\)
The energy loss is measured as \(x \times 10^{-2}\ J\), where \(x = 225.\)
Derive an expression for energy stored in a charged capacitor. A spherical metal ball of radius 15 cm carries a charge of 2μC. Calculate the electric field at a distance of 20 cm from the center of the sphere.
If \[ \frac{dy}{dx} + 2y \sec^2 x = 2 \sec^2 x + 3 \tan x \cdot \sec^2 x \] and
and \( f(0) = \frac{5}{4} \), then the value of \[ 12 \left( y \left( \frac{\pi}{4} \right) - \frac{1}{e^2} \right) \] equals to: