Animated Solution for Physics - Thermodynamics: The speed of sound in oxygen (O2) at a certain temperature is 460 ms−1. The speed of sound in helium (He) at the same temperature will be (assume both gases to be ideal)
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Visualized Solution
Visualizing the Gases
Oxygen (O2): Diatomic
Helium (He): Monatomic
TO2=THe=T
The Master Formula
v=MγRT
γ=Adiabatic Index
M=Molar Mass
Analyzing Oxygen
γO2=57(Diatomic)
MO2=32 g/mol
vO2=3257RT
Analyzing Helium
γHe=35(Monatomic)
MHe=4 g/mol
vHe=435RT
Taking the Ratio
vO2vHe=3257RT435RT
vO2vHe=57×32135×41
Simplifying the Fraction
vO2vHe=3×4×75×32×5
vO2vHe=21200
Final Calculation
vHe=460×21200
vHe≈460×3.086
vHe≈1420 m/s
The Physics Takeaway
v∝M1
MHe≪MO2⟹vHe≫vO2
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The Sigma Insight: Kinetic Theory of Gases
Solution Diagram
The Setup
Oxygen vs. Helium
Imagine two identical tubes, one filled with Oxygen gas (O2) and the other with Helium gas (He). Both gases are maintained at the exact same temperature T. We are given that the speed of sound in the Oxygen tube is 460 m/s. Our mission is to find out how fast sound travels through the Helium tube.
To do this, we need to understand what governs the speed of sound in a gas.
The Master Equation
The speed of sound v in an ideal gas is given by the beautiful Laplace formula:
v=MγRT
Here, γ is the adiabatic index (ratio of specific heats), R is the universal gas constant, T is the absolute temperature, and M is the molar mass of the gas. Since R and T are constant for both gases, the speed of sound will be entirely dictated by the interplay between γ and M.
Analyzing Oxygen
Let's first look at Oxygen. Oxygen is a diatomic gas, meaning its molecules consist of two atoms bonded together. Because of this structure, it has both translational and rotational degrees of freedom, giving it an adiabatic index of γO2=57.
Its molar mass is MO2=32 g/mol. Plugging these into our master equation, we get:
vO2=3257RT
Analyzing Helium
Now, let's shift our focus to Helium. Helium is a noble gas, which means it is monatomic. Its atoms fly around individually, possessing only translational degrees of freedom. This gives Helium an adiabatic index of γHe=35.
Its molar mass is much lighter, just MHe=4 g/mol. Substituting these values, the speed of sound in Helium is:
vHe=435RT
The Grand Ratio
Since we don't know the exact temperature T, we can cleverly eliminate it by taking the ratio of the two speeds. Let's divide vHe by vO2:
vO2vHe=3257RT435RT
The RT terms cancel out perfectly, leaving us with a ratio of pure numbers:
vO2vHe=57×32135×41
The Final Calculation
Let's carefully simplify this massive fraction inside the square root. Rearranging the terms, we bring the denominators of the lower fraction to the top:
vO2vHe=3×4×75×32×5
Simplifying the numbers, 4 goes into 32 exactly 8 times. So the numerator becomes 5×8×5=200. The denominator is 3×7=21.
vO2vHe=21200
Now, we multiply this ratio by the given speed of sound in Oxygen (460 m/s):
vHe=460×21200
Since 21200≈9.52, its square root is approximately 3.086.
vHe≈460×3.086≈1420 m/s
The Physics Takeaway
Notice how much faster sound travels in Helium (1420 m/s) compared to Oxygen (460 m/s)! This is primarily because Helium is much lighter than Oxygen. According to the formula, v∝M1. The lighter the gas particles, the faster they can accelerate and transmit the kinetic energy of the sound wave. This is exactly why inhaling Helium makes your voice sound so high-pitched!