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.
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
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.