The average speed of a gas is given by the formula:
$v_{\text{avg}} \propto \sqrt{\dfrac{T}{M}}$ Where: - $v_{\text{avg}}$ is the average speed of the gas molecules, - $T$ is the temperature in Kelvin, - $M$ is the molar mass of the gas.
We are told that the average speed of $H_2$ at $T_1$ is equal to the average speed of $O_2$ at $T_2$.
So, according to the equation above:
$\sqrt{\dfrac{T_1}{M_{H_2}}} = \sqrt{\dfrac{T_2}{M_{O_2}}}$ Squaring both sides:
$\dfrac{T_1}{M_{H_2}} = \dfrac{T_2}{M_{O_2}}$
The molar mass of $H_2$ is 2 g/mol, and the molar mass of $O_2$ is 32 g/mol, so:
$\dfrac{T_1}{2} = \dfrac{T_2}{32}$
Cross-multiplying:
$T_1 \cdot 32 = T_2 \cdot 2$
Solving for the ratio of temperatures:
$\dfrac{T_1}{T_2} = \dfrac{2}{32} = \dfrac{1}{16}$ So, the ratio $T_1 : T_2$ is:
Answer: 1:16
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).
A beam of light of wavelength \(\lambda\) falls on a metal having work function \(\phi\) placed in a magnetic field \(B\). The most energetic electrons, perpendicular to the field, are bent in circular arcs of radius \(R\). If the experiment is performed for different values of \(\lambda\), then the \(B^2 \, \text{vs} \, \frac{1}{\lambda}\) graph will look like (keeping all other quantities constant).