To determine the power dissipation in the circuit, we start by calculating the impedance \( Z \) of the series combination of the resistor and the capacitor. The impedance \( Z \) is given by:
\[ Z = \sqrt{R^2 + X_C^2} \]
where \( R = 4 \, \Omega \) and \( X_C = 4 \sqrt{3} \, \Omega \). Compute \( Z \):
\[ Z = \sqrt{4^2 + (4\sqrt{3})^2} = \sqrt{16 + 48} = \sqrt{64} = 8 \, \Omega \]
The peak voltage \( V_0 = 8 \sqrt{2} \, \text{V} \). To find the RMS voltage \( V_{\text{RMS}} \), use:
\[ V_{\text{RMS}} = \frac{V_0}{\sqrt{2}} = \frac{8\sqrt{2}}{\sqrt{2}} = 8 \, \text{V} \]
The RMS current \( I_{\text{RMS}} \) is:
\[ I_{\text{RMS}} = \frac{V_{\text{RMS}}}{Z} = \frac{8}{8} = 1 \, \text{A} \]
Power dissipation in the resistor, \( P \), is given by:
\[ P = I_{\text{RMS}}^2 \cdot R = 1^2 \cdot 4 = 4 \, \text{W} \]
The computed power dissipation is \( 4 \, \text{W} \), which falls within the given range of 4 to 4. Thus, the final answer is \( \textbf{4 W} \).
The impedance $Z$ of the circuit is:
\(Z = \sqrt{R^2 + X_C^2} = \sqrt{4^2 + (4\sqrt{3})^2} = \sqrt{16 + 48} = \sqrt{64} = 8 \, \Omega.\)
The RMS voltage is:
\(V_\text{rms} = \frac{V_\text{peak}}{\sqrt{2}} = \frac{8\sqrt{2}}{\sqrt{2}} = 8 \, \text{V}.\)
The RMS current is: \(I_\text{rms} = \frac{V_\text{rms}}{Z} = \frac{8}{8} = 1 \, \text{A}.\)
Power dissipation in the resistor is: \(P = I_\text{rms}^2 R = 1^2 \times 4 = 4 \, \text{W}.\)
Let \( C_{t-1} = 28, C_t = 56 \) and \( C_{t+1} = 70 \). Let \( A(4 \cos t, 4 \sin t), B(2 \sin t, -2 \cos t) \text{ and } C(3r - n_1, r^2 - n - 1) \) be the vertices of a triangle ABC, where \( t \) is a parameter. If \( (3x - 1)^2 + (3y)^2 = \alpha \) is the locus of the centroid of triangle ABC, then \( \alpha \) equals:
Designate whether each of the following compounds is aromatic or not aromatic.

The dimension of $ \sqrt{\frac{\mu_0}{\epsilon_0}} $ is equal to that of: (Where $ \mu_0 $ is the vacuum permeability and $ \epsilon_0 $ is the vacuum permittivity)