Problem 34
Question
A player bounces a basketball on the floor, compressing it to 80.0\(\%\) of its original volume. The air (assume it is essentially \(\mathrm{N}_{2}\) gas) inside the ball is originally at a temperature of \(20.0^{\circ} \mathrm{C}\) and a pressure of 2.00 atm. The ball's inside diameter is 23.9 \(\mathrm{cm}\) . (a) What temperature does the air in the ball reach at its maximum compression? Assume the compression is adiabatic and treat the gas as ideal. (b) By how much does the internal energy of the air change between the ball's original state and its maximum compression?
Step-by-Step Solution
Verified Answer
(a) The air temperature reaches approximately 312.47 K. (b) The change in internal energy is about 29.59 J.
1Step 1: Convert Initial Information into Standard Units
First, we need to convert all given data into standard units. The initial temperature of the gas is given as \(20.0^{\circ}\mathrm{C}\), which converts to Kelvin using the formula \(T(K) = T(^{\circ}C) + 273.15\). So, the initial temperature is \(293.15\, K\). The original pressure of the gas is \(2.00\, atm\), which is approximately \(2.00 \times 101325\, Pa = 202650\, Pa\). The diameter of the basketball is \(23.9\, cm\), which is equivalent to \(0.239\, m\).
2Step 2: Calculate Original Volume of the Gas
Using the formula for the volume of a sphere, \(V = \frac{4}{3}\pi r^3\), where \(r\) is the radius of the ball. The radius in meters is half the diameter, so \(r = 0.239/2\, m = 0.1195\, m\).Thus, the original volume \(V_{1}\) is \(\frac{4}{3} \pi (0.1195)^{3} \approx 0.00715\, m^3\).
3Step 3: Determine Compressed Volume of the Gas
When compressed to 80\% of its original volume, the new volume \(V_2\) will be \(80\%\) of \(0.00715\, m^3\).Calculate \(V_2 = 0.80 \times 0.00715\, m^3 \approx 0.00572\, m^3\).
4Step 4: Apply Adiabatic Process to Find New Temperature
For an adiabatic process of an ideal gas, \(PV^\gamma = \text{constant}\) and \(T_2 = T_1 \left( \frac{V_1}{V_2} \right)^{\gamma - 1}\). For nitrogen (\(N_2\)), \(\gamma \approx 1.4\).Calculate the new temperature \(T_2 = 293.15 \left( \frac{0.00715}{0.00572} \right)^{0.4} \approx 312.47\, K\).
5Step 5: Calculate Change in Internal Energy
The change in internal energy for a diatomic ideal gas like \(N_2\) can be found using \(\Delta U = nC_v(T_2 - T_1)\), where \(C_v = \frac{5}{2}R\). First, find \(n\) using \(PV = nRT\), with the initial conditions: \(n = \frac{202650 \times 0.00715}{8.314 \times 293.15} \approx 0.0595\, mol\).Then, \(\Delta U = 0.0595 \times \frac{5}{2} \times 8.314 \times (312.47 - 293.15) \approx 29.59\, J\).
Key Concepts
Ideal Gas LawThermodynamicsChange in Internal Energy
Ideal Gas Law
The Ideal Gas Law is a fundamental equation in chemistry and physics that describes the behavior of an ideal gas. It's given by the equation \( PV = nRT \), where:
- \( P \) is the pressure of the gas.
- \( V \) is the volume it occupies.
- \( n \) is the number of moles of the gas.
- \( R \) is the ideal gas constant (8.314 J/(mol·K)).
- \( T \) is the temperature in Kelvin.
Thermodynamics
Thermodynamics is the branch of physics concerned with heat, temperature, and their relation to energy and work. It encompasses principles that describe how energy is transferred and transformed. A key concept in thermodynamics is the adiabatic process, where no heat is transferred into or out of the system.
In the context of a bouncing basketball, when you compress it quickly, the process is considered adiabatic. During such a process:
In the context of a bouncing basketball, when you compress it quickly, the process is considered adiabatic. During such a process:
- The internal energy of the system changes, but it does so without heat exchange with the environment.
- For an ideal gas, this results in a change in temperature and pressure directly linked to changes in volume.
Change in Internal Energy
The change in internal energy \( \Delta U \) of a system is a core concept in thermodynamics, especially involving ideal gases. It's calculated using the equation \( \Delta U = nC_v(T_2 - T_1) \), where:
- \( n \) is the number of moles of gas.
- \( C_v \) is the molar heat capacity at constant volume.
- \( T_2 \) and \( T_1 \) are the final and initial temperatures, respectively.
Other exercises in this chapter
Problem 31
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