2 : 7
Step 1: Let \( c_1 \) and \( c_2 \) be the specific heat capacities of the liquids mixed. Since no heat is lost to the environment, the heat lost by the hotter liquid equals the heat gained by the cooler one.
Step 2: Set up the equation based on heat transfer: \( m \cdot c_1 \cdot (47 - 35) = m \cdot c_2 \cdot (35 - 27) \).
Step 3: Simplify to find the ratio \( \frac{c_1}{c_2} = \frac{8}{12} = \frac{2}{3} \).
Step 4: Thus, the ratio of their specific heat capacities is \( 3:2 \) (inverse of \( \frac{2}{3} \)).
The ratio of the fundamental vibrational frequencies \( \left( \nu_{^{13}C^{16}O} / \nu_{^{12}C^{16}O} \right) \) of two diatomic molecules \( ^{13}C^{16}O \) and \( ^{12}C^{16}O \), considering their force constants to be the same, is ___________ (rounded off to two decimal places).}
A heat pump, operating in reversed Carnot cycle, maintains a steady air temperature of 300 K inside an auditorium. The heat pump receives heat from the ambient air. The ambient air temperature is 280 K. Heat loss from the auditorium is 15 kW. The power consumption of the heat pump is _________ kW (rounded off to 2 decimal places).
Let \( I = \int_{-\frac{\pi}{4}}^{\frac{\pi}{4}} \frac{\tan^2 x}{1+5^x} \, dx \). Then: