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As noted in the text, the speed distribution of molecules in the Earth's atmosphere has a significant impact on its composition. a) What is the average speed of a nitrogen molecule in the atmosphere, at a temperature of \(18.0^{\circ} \mathrm{C}\) and a (partial) pressure of \(78.8 \mathrm{kPa} ?\) b) What is the average speed of a hydrogen molecule at the same temperature and pressure?

Short Answer

Expert verified
(Please provide your answer in m/s) Answer: The average speed of a nitrogen molecule in the atmosphere, at a temperature of 18.0°C and a (partial) pressure of 78.8 kPa is approximately 515.4 m/s. The average speed of a hydrogen molecule at the same temperature and pressure is approximately 1827.1 m/s.

Step by step solution

01

Convert temperature to Kelvin

To convert the temperature from Celsius to Kelvin, use the formula: \(T(K) = T(^\circ C) + 273.15\) For this problem, we have: \(T(K) = 18.0^\circ C + 273.15 = 291.15 \ K\)
02

Calculate the mass of nitrogen and hydrogen molecules

To find the mass of one molecule of each gas, we can use the molar mass and the Avogadro constant: \(m_1 = \dfrac{M_1}{N_A}\) Here, \(m_1\) is the mass of a single molecule, \(M_1\) is the molar mass, and \(N_A\) is the Avogadro constant (\(6.022 \times 10^{23}\ \text{mol}^{-1}\)). For nitrogen (N2) and hydrogen (H2) we have the following molar masses: - Nitrogen (N2): \(M_1 = 2 \times 14.01\ \text{g/mol} = 28.02\ \text{g/mol}\) - Hydrogen (H2): \(M_1 = 2 \times 1.01\ \text{g/mol} = 2.02\ \text{g/mol}\) Now, we can calculate the mass of a single molecule (in kilograms) for each gas: - Nitrogen: \(m_{N2} = \dfrac{28.02\ \text{g/mol}}{6.022 \times 10^{23}\ \text{mol}^{-1}} = 4.65 \times 10^{-26}\ \text{kg}\) - Hydrogen: \(m_{H2} = \dfrac{2.02\ \text{g/mol}}{6.022 \times 10^{23}\ \text{mol}^{-1}} = 3.36 \times 10^{-27}\ \text{kg}\)
03

Calculate the average speed of nitrogen and hydrogen molecules

Now, we can use the formula for the average speed of a gas molecule and substitute the values we have: \(u_{avg} = \sqrt{\dfrac{8kT}{\pi m}}\) For nitrogen (N2) and hydrogen (H2) we get: - Nitrogen: \(u_{avg_{N2}} = \sqrt{\dfrac{8 \times 1.38 \times 10^{-23}\ \text{J/K} \times 291.15\ \text{K}}{\pi \times 4.65 \times 10^{-26}\ \text{kg}}} = 515.4\ \text{m/s}\) - Hydrogen: \(u_{avg_{H2}} = \sqrt{\dfrac{8 \times 1.38 \times 10^{-23}\ \text{J/K} \times 291.15\ \text{K}}{\pi \times 3.36 \times 10^{-27}\ \text{kg}}} = 1827.1\ \text{m/s}\)
04

Write the final answers

The average speed of a nitrogen molecule in the atmosphere, at a temperature of \(18.0^{\circ} \mathrm{C}\) and a (partial) pressure of \(78.8\ \mathrm{kPa}\) is approximately \(515.4\ \text{m/s}\). The average speed of a hydrogen molecule at the same temperature and pressure is approximately \(1827.1\ \text{m/s}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Molar Mass
Molar mass is a crucial concept in chemistry, referring to the weight of one mole of a substance. It is expressed in grams per mole (g/mol) and is directly related to the mass of individual atoms or molecules. In our textbook exercise, understanding molar mass allows us to compare different gases, like nitrogen and hydrogen.

Nitrogen, with a chemical symbol N2, has a molar mass of 28.02 g/mol, calculated by doubling the atomic mass of nitrogen, as it is diatomic. Hydrogen's diatomic form, H2, is much lighter, having a molar mass of only 2.02 g/mol. Why is this important? It helps us determine the mass of an individual gas molecule when combined with Avogadro's constant, which is necessary to calculate the average molecular speed.
Avogadro's Constant
Avogadro's constant, denoted as NA, is a fundamental number in chemistry that represents the quantity of atoms or molecules in one mole of a substance. This constant, approximately 6.022 x 1023 mol−1, is named after the italian scientist Amedeo Avogadro. It serves as a bridge between the macroscopic scale of substances we handle everyday and the microscopic scale of atoms and molecules.

In our exercise, we use this constant to find the mass of one nitrogen or hydrogen molecule from their respective molar masses. By dividing the molar mass by Avogadro's constant, we convert from the macroscale (grams per mole) to the microscale (kilograms per molecule), which is required to further investigate their behaviors as individual gas molecules.
Kinetic Molecular Theory
Kinetic Molecular Theory (KMT) gives us a framework to understand the behavior of gases at the molecular level. It explains the properties of gases in terms of the energy their molecules contain and how they move. Some fundamental points of KMT include the constant, random motion of gas molecules and the negligible volume of the molecules compared to the space they occupy.

Moreover, KMT tells us that the temperature of a gas is a measure of the average kinetic energy of its molecules. Consequently, at a given temperature, lighter gas molecules, like hydrogen, move faster on average than heavier ones, like nitrogen. This concept explains our findings in the exercise, where despite the same temperature, hydrogen molecules have a significantly higher average speed.
Gas Molecule Velocity Calculation
To calculate the average velocity of gas molecules, we use an equation derived from the Kinetic Molecular Theory. The equation is
\( u_{avg} = \sqrt{\dfrac{8kT}{\pi m}} \)
, where
  • \(u_{avg}\) is the average speed,
  • k is the Boltzmann's constant,
  • T is the temperature in Kelvin,
  • m is the mass of a single molecule.
This equation embodies the direct relationship between energy (as temperature) and the motion of molecules. In this problem, upon substituting in the calculated mass of nitrogen and hydrogen molecules, we found their average speeds, considering the temperature in Kelvin. The lighter hydrogen molecules travel at a greater speed due to their smaller mass, demonstrating an inverse relationship between mass and average velocity.

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Most popular questions from this chapter

The Maxwell speed distribution assumes that the gas is in equilibrium. Thus, if a gas, all of whose molecules were moving at the same speed, were given enough time, they would eventually come to satisfy the speed distribution. But the kinetic theory derivations in the text assumed that when a gas molecule hits the wall of a container, it bounces back with the same energy it had before the collision and that gas molecules exert no forces on each other. If gas molecules exchange energy neither with the walls of their container nor with each other, how can they ever come to equilibrium? Is it not true that if they all had the same speed initially, some would have to slow down and others speed up, according to the Maxwell speed distribution?

Two identical containers hold equal masses of gas, oxygen in one and nitrogen in the other. The gases are held at the same temperature. How does the pressure of the oxygen compare to that of the nitrogen? a) \(p_{\mathrm{O}}>p_{\mathrm{N}}\) b) \(p_{\mathrm{O}}=p_{\mathrm{N}}\) c) \(p_{\mathrm{O}}

A tire has a gauge pressure of \(300 . \mathrm{kPa}\) at \(15.0^{\circ} \mathrm{C}\). What is the gauge pressure at \(45.0^{\circ} \mathrm{C}\) ? Assume that the change in volume of the tire is negligible.

In a diesel engine, the fuel-air mixture is compressed rapidly. As a result, the temperature rises to the spontaneous combustion temperature for the fuel, causing the fuel to ignite. How is the temperature rise possible, given the fact that the compression occurs so rapidly that there is not enough time for a significant amount of heat to flow into or out of the fuel-air mixture?

Suppose \(15.0 \mathrm{~L}\) of an ideal monatomic gas at a pressure of \(1.50 \cdot 10^{5} \mathrm{kPa}\) is expanded adiabatically (no heat transfer) until the volume is doubled. a) What is the pressure of the gas at the new volume? b) If the initial temperature of the gas was \(300 . \mathrm{K},\) what is its final temperature after the expansion?

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