/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 2 What is the bulk modulus of oxyg... [FREE SOLUTION] | 91Ó°ÊÓ

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What is the bulk modulus of oxygen if \(32.0 \mathrm{~g}\) of oxygen occupies \(22.4 \mathrm{~L}\) and the speed of sound in the oxygen is \(317 \mathrm{~m} / \mathrm{s} ?\)

Short Answer

Expert verified
The bulk modulus of oxygen is approximately 143135 Pa.

Step by step solution

01

Understand the formula for Bulk Modulus

The bulk modulus \(B\) of a fluid (here, oxygen) is related to the speed of sound \(v\) in the fluid and its density \(\rho\) by the formula \(B = v^2 \cdot \rho\). So we need to find both the speed of sound in oxygen and the density of the oxygen in order to calculate the bulk modulus.
02

Calculate the density of oxygen

The density \(\rho\) of oxygen can be calculated using the formula \(\rho = \frac{m}{V}\), where \(m = 32.0 \text{ g} = 0.032 \text{ kg}\) is the mass of oxygen and \(V = 22.4 \text{ L} = 0.0224 \text{ m}^3\) is the volume it occupies. By substituting these values, we have:\[\rho = \frac{0.032}{0.0224} = 1.4286 \text{ kg/m}^3\]
03

Use the formula to find the Bulk Modulus

Now that we have the density \(\rho = 1.4286 \text{ kg/m}^3\) and the speed of sound \(v = 317 \text{ m/s}\), we use the formula for bulk modulus: \(B = v^2 \cdot \rho\). By substituting the values, we have:\[B = (317)^2 \times 1.4286 = 143134.9894 \text{ Pa}\]So the bulk modulus of oxygen is approximately \(143135 \text{ Pa}\).

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Key Concepts

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

Density of Oxygen
The density of a substance is its mass per unit volume and is an essential parameter in determining various physical properties. For oxygen, the density (\(\rho\)) is calculated using the formula: \( \rho = \frac{m}{V} \), where:
  • \(m\) is the mass of the oxygen, and
  • \(V\) is the volume that the oxygen occupies.
In the exercise, the mass of oxygen is \(32.0 \ \text{g} = 0.032 \ \text{kg}\), and the volume is \(22.4 \ \text{L} = 0.0224 \ \text{m}^3\). By substituting these values into the formula, we find:\[\rho = \frac{0.032}{0.0224} = 1.4286 \ \text{kg/m}^3\]This step gives us the density of oxygen, a critical factor when determining the bulk modulus.
Speed of Sound
The speed of sound in a medium is affected by the density and elasticity of that medium. It determines how fast sound waves can travel through the substance. In the context of the exercise, the speed of sound in oxygen is given as \(317 \ \text{m/s}\).
This value is necessary to calculate the bulk modulus of oxygen, as the speed of sound directly relates to the flexibility and compressibility of the fluid. In gases, particularly, the speed of sound can reveal much about their molecular interactions and pressure conditions.
Formula for Bulk Modulus
The bulk modulus (\(B\)) is a measure of a material's resistance to uniform compression. It's quantitatively defined for gases using the relationship with the speed of sound (\(v\)) and density (\(\rho\)):\[B = v^2 \cdot \rho\]This formula connects the physical characteristics of oxygen, using the speed of sound and its density.
To apply this formula, the values we have include the speed of sound \(v = 317 \ \text{m/s}\) and the density \(\rho = 1.4286 \ \text{kg/m}^3\), as previously calculated. Substituting into the formula gives:\[B = (317)^2 \times 1.4286 = 143134.9894 \ \text{Pa}\]This outcome denotes how oxygen reacts under pressure changes, providing insights into its physical properties at specific conditions.
Calculus of Density
Calculating density involves understanding the concept of mass distribution over a fixed volume. It requires basic algebra; however, each situation demands precision in measurement and unit conversion.
In the exercise context, converting mass from grams to kilograms and volume from liters to cubic meters is essential:
  • Mass: \(32.0 \ \text{g} = 0.032 \ \text{kg}\)
  • Volume: \(22.4 \ \text{L} = 0.0224 \ \text{m}^3\)
Performing these conversions ensures that the density calculation results in the appropriate unit system, maintaining accuracy. This meticulousness reflects in the final computation, where units align perfectly with those required for further analysis, such as in the bulk modulus calculation.

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Most popular questions from this chapter

An avalanche of sand along some rare desert sand dunes can produce a booming that is loud enough to be heard \(10 \mathrm{~km}\) away. The booming apparently results from a periodic oscillation of the sliding layer of sand \(-\) the layer's thickness expands and contracts. If the emitted frequency is \(90 \mathrm{~Hz}\), what are (a) the period of the thickness oscillation and (b) the wavelength of the sound?

A well with vertical sides and water at the bottom resonates at \(7.00 \mathrm{~Hz}\) and at no lower frequency. The air-filled portion of the well acts as a tube with one closed end (at the bottom) and one open end (at the top). The air in the well has a density of \(1.10 \mathrm{~kg} / \mathrm{m}^{3}\) and a bulk modulus of \(1.33 \times 10^{5} \mathrm{~Pa}\). How far down in the well is the water surface?

A pipe \(0.60 \mathrm{~m}\) long and closed at one end is filled with an unknown gas. The third lowest harmonic frequency for the pipe is \(750 \mathrm{~Hz}\). (a) What is the speed of sound in the unknown gas? (b) What is the fundamental frequency for this pipe when it is filled with the unknown gas?

One of the harmonic frequencies of tube \(A\) with two open ends is \(325 \mathrm{~Hz}\). The next-highest harmonic frequency is \(390 \mathrm{~Hz}\). (a) What harmonic frequency is next highest after the harmonic frequency \(195 \mathrm{~Hz}\) (b) What is the number of this next-highest harmonic? One of the harmonic frequencies of tube \(B\) with only one open end is \(1080 \mathrm{~Hz}\). The next-highest harmonic frequency is \(1320 \mathrm{~Hz}\). (c) What harmonic frequency is next highest after the harmonic frequency \(600 \mathrm{~Hz}\) ? (d) What is the number of this nexthighest harmonic?

Approximately a third of people with normal hearing have ears that continuously emit a low-intensity sound outward through the ear canal. A person with such spontaneous otoacoustic emission is rarely aware of the sound, except perhaps in a noisefree environment, but occasionally the emission is loud enough to be heard by someone else nearby. In one observation, the sound wave had a frequency of \(1665 \mathrm{~Hz}\) and a pressure amplitude of \(1.13 \times 10^{-3} \mathrm{~Pa}\). What were (a) the displacement amplitude and (b) the intensity of the wave emitted by the ear?

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