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 \( 6 \, \text{V} \).