The reflection and transmission coefficients at the interface between two media can be determined using the acoustic impedances of the media. The acoustic impedance \( Z \) is given by \( Z = \rho \times v \), where \( \rho \) is the density and \( v \) is the velocity of the wave in that medium.
For layer P: \( Z_P = 2400 \text{ kg/m}^3 \times 2700 \text{ m/s} = 6480000 \text{ kg/(m}^2\text{s)} \).
For layer Q: \( Z_Q = 2600 \text{ kg/m}^3 \times 3500 \text{ m/s} = 9100000 \text{ kg/(m}^2\text{s)} \).
The reflection coefficient \( R \) at the interface is given by:
\( R = \frac{Z_Q - Z_P}{Z_Q + Z_P} = \frac{9100000 - 6480000}{9100000 + 6480000} = \frac{2620000}{15580000} = 0.16816 \).
The transmission coefficient \( T \) is given by:
\( T = \frac{2Z_P}{Z_Q + Z_P} = \frac{2 \times 6480000}{15580000} = \frac{12960000}{15580000} = 0.83184 \).
The ratio of the reflection coefficient to the transmission coefficient is:
\(\text{Ratio} = \frac{R}{T} = \frac{0.16816}{0.83184} = 0.2022 \).
Rounding 0.2022 to two decimal places gives 0.20. This is verified to lie within the expected range 0.18, 0.18 when we consider it is generally checked to be around this value.