We are given that the relative permittivity of the dielectric is a function of the applied voltage, \( \epsilon = 2U \).
Let the initial voltage across the capacitor without the dielectric be \( U_0 = 78 \, \text{V} \).
The initial energy stored in the capacitor without the dielectric is given by: \[ U_{\text{initial}} = \frac{1}{2} C U_0^2 \]
Now, when the capacitor with the dielectric is connected to this uncharged capacitor, the voltage across both capacitors will become equal due to charge conservation.
Let's say the final voltage across both capacitors is \( U_f \). The energy after the connection is: \[ U_{\text{final}} = \frac{1}{2} C \epsilon(U_f) U_f^2 \] Since the charge on both capacitors is conserved, we have: \[ C U_0 = C \epsilon(U_f) U_f \] Substitute the value \( \epsilon(U_f) = 2 U_f \): \[ C U_0 = C \cdot 2 U_f^2 \] \[ U_0 = 2 U_f^2 \] \[ U_f^2 = \frac{U_0}{2} \] \[ U_f = \sqrt{\frac{U_0}{2}} = \sqrt{\frac{78}{2}} = 6 \, \text{V} \] Thus, the final voltage across the capacitors is \( 6 \, \text{V} \).
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: