300 K
Finding the Temperature at Which the RMS Velocity of SO2 Matches the Most Probable Velocity of O2
Step 1: Formula for RMS Velocity of a Gas
The root mean square (RMS) velocity is given by the formula:
vrms = √(3kT/m)
where:
k is the Boltzmann constant
T is the temperature in Kelvin
m is the molar mass of the gas
For sulfur dioxide (SO2), at 400 K, the RMS velocity is given by:
vrms,SO₂ = √(3kTSO₂/mSO₂)
Step 2: Formula for Most Probable Velocity of a Gas
The most probable velocity (vmp) is given by:
vmp = √(2kT/m)
For oxygen (O2), the most probable velocity is given by:
vmp,O₂ = √(2kTO₂/mO₂)
Step 3: Setting the RMS Velocity of SO2 Equal to the Most Probable Velocity of O2
We equate the two velocities:
√(3kTSO₂/mSO₂) = √(2kTO₂/mO₂)
Step 4: Simplifying the Equation
Canceling out k and squaring both sides:
(3TSO₂/mSO₂) = (2TO₂/mO₂)
(TSO₂/TO₂) = (2mSO₂)/(3mO₂)
Step 5: Using Molecular Masses
The molar masses are:
SO2: 64 g/mol
O2: 32 g/mol
Substituting:
(TSO₂/TO₂) = (2 × 64)/(3 × 32) = 128/96 = 4/3
Step 6: Solving for TO₂
Given TSO₂ = 400 K:
400/TO₂ = 4/3
TO₂ = (3 × 400) / 4 = 300 K
Final Answer:
The temperature at which the RMS velocity of SO2 at 400 K matches the most probable velocity of O2 is:
300 K
Match the LIST-I with LIST-II:
Choose the correct answer from the options given below :
A constant force of \[ \mathbf{F} = (8\hat{i} - 2\hat{j} + 6\hat{k}) \text{ N} \] acts on a body of mass 2 kg, displacing it from \[ \mathbf{r_1} = (2\hat{i} + 3\hat{j} - 4\hat{k}) \text{ m to } \mathbf{r_2} = (4\hat{i} - 3\hat{j} + 6\hat{k}) \text{ m}. \] The work done in the process is:
A ball 'A' of mass 1.2 kg moving with a velocity of 8.4 m/s makes a one-dimensional elastic collision with a ball 'B' of mass 3.6 kg at rest. The percentage of kinetic energy transferred by ball 'A' to ball 'B' is:
A metre scale is balanced on a knife edge at its centre. When two coins, each of mass 9 g, are kept one above the other at the 10 cm mark, the scale is found to be balanced at 35 cm. The mass of the metre scale is:
A body of mass \( m \) and radius \( r \) rolling horizontally with velocity \( V \), rolls up an inclined plane to a vertical height \( \frac{V^2}{g} \). The body is: