Problem 97
Question
The root mean square velocity of one mole of a monoatomic gas having molar mass \(\mathrm{M}\) is \(\mathrm{u}_{\mathrm{rms}}\) ' The relation between the average kinetic energy (E) of the gas and \(u_{\text {rms }}\) is (a) \(\mathrm{u}_{\mathrm{nms}}=\sqrt{(3 \mathrm{E} / 2 \mathrm{M})}\) (b) \(\mathrm{u}_{\mathrm{rms}}=\sqrt{(2 \mathrm{E} / 3 \mathrm{M})}\) (c) \(\mathrm{u}_{\mathrm{rms}}=\sqrt{(2 \mathrm{E} / \mathrm{M})}\) (d) \(\mathrm{u}_{\mathrm{rms}}=\sqrt{(\mathrm{E} / 3 \mathrm{M})}\)
Step-by-Step Solution
Verified Answer
The correct relation is (c) \( \mathrm{u}_{\mathrm{rms}}=\sqrt{\frac{2 \mathrm{E}}{\mathrm{M}}} \).
1Step 1: Recall the formulas
The root mean square velocity \( u_{rms} \) of a gas is given by \( u_{rms} = \sqrt{\frac{3kT}{m}} \) where \( k \) is the Boltzmann constant, \( T \) is the temperature, and \( m \) is the mass of one molecule of gas. For one mole, \( M \) is the molar mass such that \( m = \frac{M}{N_A} \), where \( N_A \) is Avogadro's number.
2Step 2: Relate kinetic energy to temperature
The average kinetic energy of one mole of a monoatomic gas is given by \( E = \frac{3}{2}RT \), where \( R \) is the ideal gas constant. For an individual molecule, \( E_{molecule} = \frac{3}{2}kT \).
3Step 3: Substitute temperature in terms of kinetic energy
Since for one mole \( E = \frac{3}{2}RT \), we can express temperature as \( T = \frac{2E}{3R} \). Substituting this into the formula for \( u_{rms} \), we get \( u_{rms} = \sqrt{\frac{3k(\frac{2E}{3R})}{m}} = \sqrt{\frac{2Ek}{mR}} \).
4Step 4: Simplify using mass relations
Replace \( m \) with \( \frac{M}{N_A} \), thus: \( u_{rms} = \sqrt{\frac{2E \cdot k \cdot N_A}{M \cdot R}} \). Since \( R = kN_A \), the formula simplifies to \( u_{rms} = \sqrt{\frac{2E}{M}} \).
5Step 5: Verify the correct expression with given options
The expression \( u_{rms} = \sqrt{\frac{2E}{M}} \) matches option (c) of the given options in the exercise.
Key Concepts
Root Mean Square VelocityAverage Kinetic EnergyMolar Mass
Root Mean Square Velocity
Understanding root mean square velocity involves grasping how the particles in a gas move at various speeds due to thermal energy. This concept is crucial in the kinetic theory of gases, which helps explain the motion of gas particles.
The root mean square velocity, often abbreviated as \( u_{rms} \), is a way to quantify the average speed of particles. Mathematically, it is defined by the formula:
\[ u_{rms} = \sqrt{\frac{3kT}{m}} \]
where:
Understanding \( u_{rms} \) gives insight into how fast gas particles, on average, are moving and is an essential aspect of studying gas behaviors under various conditions.
The root mean square velocity, often abbreviated as \( u_{rms} \), is a way to quantify the average speed of particles. Mathematically, it is defined by the formula:
\[ u_{rms} = \sqrt{\frac{3kT}{m}} \]
where:
- \( k \) is the Boltzmann constant, which relates the kinetic energy of particles to their temperature in kelvins.
- \( T \) stands for the temperature of the gas.
- \( m \) is the mass of a single molecule of the gas.
Understanding \( u_{rms} \) gives insight into how fast gas particles, on average, are moving and is an essential aspect of studying gas behaviors under various conditions.
Average Kinetic Energy
The average kinetic energy of gas molecules is foundational to understanding the kinetic theory of gases. This energy is due to the constant, random motion of particles in a gas and can be directly related to the temperature of the gas.
The average kinetic energy \( E \) of a monoatomic gas is given by the equation:
\[ E = \frac{3}{2}RT \]
where:
In simpler terms, as the temperature increases, the kinetic energy of the gas particles also increases, causing them to move faster. This concept is crucial for predicting how gases behave at various temperatures and pressures, illustrating why gases expand when heated and contract when cooled.
The average kinetic energy \( E \) of a monoatomic gas is given by the equation:
\[ E = \frac{3}{2}RT \]
where:
- \( R \) is the ideal gas constant, linking the microscopic and macroscopic states of a gas.
- \( T \) is the absolute temperature measured in kelvins.
In simpler terms, as the temperature increases, the kinetic energy of the gas particles also increases, causing them to move faster. This concept is crucial for predicting how gases behave at various temperatures and pressures, illustrating why gases expand when heated and contract when cooled.
Molar Mass
Molar mass is a key concept often encountered in chemistry and physics when dealing with large numbers of atoms or molecules, like in gases. It represents the mass of one mole of a substance, typically expressed in grams per mole.
In terms of gases, the molar mass \( M \) is vital for calculating various properties, such as the root mean square velocity and average kinetic energy.
For instance, in the root mean square velocity formula, we substitute the molecular mass with molar mass by using the relation:
\[ m = \frac{M}{N_A} \]
where:
In terms of gases, the molar mass \( M \) is vital for calculating various properties, such as the root mean square velocity and average kinetic energy.
For instance, in the root mean square velocity formula, we substitute the molecular mass with molar mass by using the relation:
\[ m = \frac{M}{N_A} \]
where:
- \( M \) is the molar mass.
- \( N_A \) is Avogadro's number, which provides the scale to move from microscopic to macroscopic quantities.
Other exercises in this chapter
Problem 94
One litre of gas \(\mathrm{A}\) at \(2 \mathrm{~atm}\) pressure at \(27^{\circ} \mathrm{C}\) and two litres of gas \(\mathrm{B}\) at 3 atm pressure at \(127^{\c
View solution Problem 96
The maximum number of molecules is present in (a) \(15 \mathrm{~L}\) of \(\mathrm{H}_{2}\) gas at STP (b) \(5 \mathrm{~L}\) of \(\mathrm{N}_{2}\) gas at \(\math
View solution Problem 99
At a certain temperature for which \(\mathrm{RT}=25 \mathrm{~L}\) atm. \(\mathrm{mol}^{-1}\), the density of a gas, in \(\mathrm{g} \mathrm{L}^{-1}\), is \(\mat
View solution Problem 100
At \(100^{\circ} \mathrm{C}\) and \(1 \mathrm{~atm}\), if the density of liquid water is \(1.0 \mathrm{~g} \mathrm{~cm}^{-3}\) and that of water vapour is \(0.0
View solution