The apparent frequency (\( f_{\text{app}} \)) heard by the passenger in car \( Q \), when both cars are moving in the same direction, is given by:
\[ f_{\text{app}} = \frac{V_s + V_Q}{V_s + V_P} \cdot f. \]
Here:
Substitute \( V_s = 360 \, \text{m/s} \), \( V_Q = 40 \, \text{m/s} \), \( V_P = 20 \, \text{m/s} \), and \( f = 400 \, \text{Hz} \):
\[ f_{\text{app}} = \frac{360 + 40}{360 + 20} \cdot 400. \]
Simplify the expression:
\[ f_{\text{app}} = \frac{400}{380} \cdot 400. \]
Calculate \( f_{\text{app}} \):
\[ f_{\text{app}} = \frac{400 \times 400}{380} \approx 421 \, \text{Hz}. \]
The frequency heard by the passenger of car \( Q \) is approximately \( 421 \, \text{Hz} \).

The term independent of $ x $ in the expansion of $$ \left( \frac{x + 1}{x^{3/2} + 1 - \sqrt{x}} \cdot \frac{x + 1}{x - \sqrt{x}} \right)^{10} $$ for $ x>1 $ is:

Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.
If $ \theta \in [-2\pi,\ 2\pi] $, then the number of solutions of $$ 2\sqrt{2} \cos^2\theta + (2 - \sqrt{6}) \cos\theta - \sqrt{3} = 0 $$ is: