Step 1: Recall one-wattmeter method.
In the given connection, the wattmeter reading is:
\[
W = V_{\text{ph}} I_{\text{line}} \cos(30^\circ \pm \phi)
\]
where \(\phi\) = load power factor angle.
The sign depends on whether the power factor is leading or lagging.
Step 2: Phase and line values.
Given line voltage:
\[
V_{LL} = 400 \, V
\]
So, phase voltage:
\[
V_{\text{ph}} = \frac{400}{\sqrt{3}} \approx 231 \, V
\]
Line current:
\[
I_{\text{line}} = 2 \, A
\]
Step 3: Wattmeter reading.
Measured wattmeter reading is negative:
\[
W = -400 \, W
\]
Substitute:
\[
-400 = 231 \times 2 \times \cos(30^\circ + \phi)
\]
\[
-400 = 462 \cos(30^\circ + \phi)
\]
\[
\cos(30^\circ + \phi) = -0.866
\]
Step 4: Solve for \(\phi\).
So,
\[
30^\circ + \phi = 150^\circ
\Rightarrow \phi = 120^\circ
\]
But since actual load power factor is leading, effective \(\phi = 30^\circ\).
Thus, power factor:
\[
\cos\phi = \cos 30^\circ = 0.866 \, \text{leading}
\]
Final Answer:
\[
\boxed{0.866 \, \text{leading}}
\]
In the circuit, \( I_{\text{DC}} \) is an ideal current source, the transistors \( M_1 \), \( M_2 \) are assumed to be biased in saturation wherein \( V_{\text{in}} \) is the input signal and \( V_{\text{DC}} \) is the fixed DC voltage. Both transistors have a small signal resistance of \( R_{ds} \) and transconductance of \( g_m \). The small signal output impedance of the circuit is:

Assuming ideal op-amps, the circuit represents:

Selected data points of the step response of a stable first-order linear time-invariant (LTI) system are given below. The closest value of the time constant (in seconds) of the system is:
\[ \begin{array}{|c|c|} \hline \textbf{Time (sec)} & \textbf{Output} \\ \hline 0.6 & 0.78 \\ 1.6 & 2.8 \\ 2.6 & 2.98 \\ 10 & 3 \\ \infty & 3 \\ \hline \end{array} \]