Problem 107
Question
The average translatory energy and rms speed of molecules in a sample of oxygen gas at \(300 \mathrm{~K}\) are \(5.21 \times 10^{-21} \mathrm{~J}\) and \(484 \mathrm{~ms}^{-1}\) respectively. The sorresponding values at \(600 \mathrm{~K}\) are nearly (assuming deal gas behaviour) (a) \(\left.12.42 \times 10^{-21}\right\rfloor, 968 \mathrm{~ms}^{-1}\) (b) \(7.78 \times 10^{-21} \mathrm{~J}, 684 \mathrm{~ms}^{-1}\) (c) \(6.21 \times 10^{-21} \mathrm{~J}, 968 \mathrm{~ms}^{-1}\) (d) \(12.42 \times 10^{-21} \mathrm{~J}, 684 \mathrm{~ms}^{-1}\)
Step-by-Step Solution
Verified Answer
The calculated energy is incorrect; rms speed at 600 K is 684 ms^{-1}. Option d has correct rms speed.
1Step 1: Understanding the formula for translational energy
The average translatory kinetic energy (E) of gas molecules at temperature (T) can be calculated using the formula: \[ E = \frac{3}{2}kT \]where \(k\) is the Boltzmann constant \(1.38 \times 10^{-23} \mathrm{~JK}^{-1}\). Since the energy is proportional to temperature in Kelvin, if the initial energy at \(300 \mathrm{~K}\) is \(5.21 \times 10^{-21} \mathrm{~J}\), doubling the temperature to \(600 \mathrm{~K}\) should double the energy.
2Step 2: Calculating the translational energy at 600 K
Since the energy at \(300 \mathrm{~K}\) is \(5.21 \times 10^{-21} \mathrm{~J}\), the energy at \(600 \mathrm{~K}\) can be calculated by direct proportion:\[ E_{600} = 2 \times 5.21 \times 10^{-21} \mathrm{~J} = 10.42 \times 10^{-21} \mathrm{~J} \].
3Step 3: Understanding the formula for rms speed
The root-mean-square (rms) speed (v) of the gas molecules is given by the formula: \[ v = \sqrt{\frac{3kT}{m}} \]where \(m\) is the molar mass of the gas, which remains constant. The rms speed is proportional to the square root of the temperature, as \(v \propto \sqrt{T}\).
4Step 4: Calculating the rms speed at 600 K
The initial rms speed is \(484 \mathrm{~ms}^{-1}\) at \(300 \mathrm{~K}\). At \(600 \mathrm{~K}\), which is double the temperature, the new speed is:\[ v_{600} = 484 \times \sqrt{\frac{600}{300}} = 484 \times \sqrt{2} \approx 684 \mathrm{~ms}^{-1} \].
5Step 5: Matching calculated values with options
From our calculations, at \(600 \mathrm{~K}\), the translational energy is \(10.42 \times 10^{-21} \mathrm{~J}\), and the rms speed is approximately \(684 \mathrm{~ms}^{-1}\). Among the given options, \( (d) 12.42 \times 10^{-21} \mathrm{~J}, 684 \mathrm{~ms}^{-1} \) has the correct rms speed, but incorrect energy. Hence, correct values do not directly match any options, suggesting possible typographical or miscalculation in options.
Key Concepts
Translational Kinetic EnergyRMS SpeedIdeal Gas Law
Translational Kinetic Energy
In the realm of thermodynamics, translational kinetic energy is a fundamental concept that relates to the motion of particles. When we talk about gases, this energy is the motion of the molecules moving in space without spinning or vibrating. The formula to compute the average translational kinetic energy of a gas molecule is:\[ E = \frac{3}{2} kT \]In this equation, \(E\) represents the energy, \(k\) is the Boltzmann constant \(1.38 \times 10^{-23} \mathrm{~JK}^{-1}\), and \(T\) is the absolute temperature in Kelvins.
- Translational kinetic energy is directly proportional to temperature.
- As temperature doubles, the translational kinetic energy also doubles.
RMS Speed
Root-mean-square speed is an important parameter when discussing gas molecules' movement. The rms speed, often denoted as \(v\), provides insight into the distribution of molecular speeds at a given temperature. It can be calculated using the formula:\[ v = \sqrt{\frac{3kT}{m}} \]Here, \(k\) is again the Boltzmann constant, \(T\) is the temperature, and \(m\) is the mass of a single molecule. For practical calculations, the molar mass of the gas is often used.
- The rms speed is directly related to the square root of temperature.
- Raising the temperature results in an increase in rms speed according to the relation \(v \propto \sqrt{T}\).
Ideal Gas Law
The ideal gas law is a cornerstone of thermodynamics that relates the macroscopic properties of an ideal gas. It is expressed as:\[ PV = nRT \]In this equation:
- \(P\) is the pressure of the gas.
- \(V\) is the volume.
- \(n\) represents the number of moles.
- \(R\) is the ideal gas constant.
- \(T\) is the absolute temperature measured in Kelvins.
Other exercises in this chapter
Problem 103
An oxygen cylinder of volume \(30 \mathrm{~L}\) has an initial gauge pressure of \(15 \mathrm{~atm}\) and a temperature of \(27^{\circ} \mathrm{C}\). After some
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The average energy and the rms speed of molecules in a sample of oxygen gas at \(400 \mathrm{~K}\) are \(7.21 \times 10^{-21} \mathrm{~J}\) and \(524 \mathrm{~m
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The average energy and the rms speed of molecules in a sample of oxygen gas at \(400 \mathrm{~K}\) are \(7.21 \times 10^{-21} \mathrm{~J}\) and \(524 \mathrm{~m
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