Using the Formula for Root Mean Square (r.m.s.) Velocity: The r.m.s. velocity \( v_{rms} \) for a gas is given by:
\[ v_{rms} = \sqrt{\frac{3RT}{M}} \]
where \( R \) is the gas constant, \( T \) is the temperature, and \( M \) is the molar mass of the gas.
Set up the Equation for Hydrogen and Oxygen: To find the temperature at which the r.m.s. velocity of hydrogen equals that of oxygen at 47°C, we set:
\[ \sqrt{\frac{3RT_{H_2}}{M_{H_2}}} = \sqrt{\frac{3RT_{O_2}}{M_{O_2}}} \]
Isolate \( T_{H_2} \): Square both sides to remove the square root:
\[ \frac{3RT_{H_2}}{M_{H_2}} = \frac{3RT_{O_2}}{M_{O_2}} \]
Simplify by canceling \( 3R \) on both sides:
\[ T_{H_2} = T_{O_2} \times \frac{M_{H_2}}{M_{O_2}} \]
Substitute Values for Molar Mass and Temperature: Given \( T_{O_2} = 47°C = 320 \, K \),
\[ T_{H_2} = 320 \times \frac{2}{32} = 20 \, K \]
To find the temperature at which the root mean square (r.m.s.) velocity of a hydrogen molecule equals that of an oxygen molecule at 47°C, we use the formula for r.m.s. velocity:
\(v_{\text{rms}} = \sqrt{\frac{3kT}{m}}\)
where:
Given that the r.m.s velocity of the hydrogen molecule is equal to that of the oxygen molecule, we can set up the equation:
\(\sqrt{\frac{3kT_{\text{H}_2}}{m_{\text{H}_2}}} = \sqrt{\frac{3kT_{\text{O}_2}}{m_{\text{O}_2}}}\)
From this equation, we cancel out the common terms:
\(\frac{T_{\text{H}_2}}{m_{\text{H}_2}} = \frac{T_{\text{O}_2}}{m_{\text{O}_2}}\)
Rearranging gives us:
\(T_{\text{H}_2} = T_{\text{O}_2} \times \frac{m_{\text{H}_2}}{m_{\text{O}_2}}\)
The molecular masses are:
The temperature of the oxygen molecule, \(T_{\text{O}_2}\), must be in Kelvin. 47°C is converted to Kelvin as follows:
\(T_{\text{O}_2} = 47 + 273 = 320 \text{ K}\)
Substituting these values into the equation:
\(T_{\text{H}_2} = 320 \times \frac{2}{32}\)
Simplifying gives:
\(T_{\text{H}_2} = 320 \times \frac{1}{16} = 20 \text{ K}\)
Therefore, the correct answer is 20 K.
In the given figure, the blocks $A$, $B$ and $C$ weigh $4\,\text{kg}$, $6\,\text{kg}$ and $8\,\text{kg}$ respectively. The coefficient of sliding friction between any two surfaces is $0.5$. The force $\vec{F}$ required to slide the block $C$ with constant speed is ___ N.
(Given: $g = 10\,\text{m s}^{-2}$) 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).

The gas laws were developed at the end of the 18th century, when scientists began to realize that relationships between pressure, volume and temperature of a sample of gas could be obtained which would hold to approximation for all gases.