Problem 13
Question
One of the cylinders of an automobile engine has a volume of \(400 . \mathrm{cm}^{3} .\) The engine takes in air at a pressure of 1.00 atm and a temperature of \(15^{\circ} \mathrm{C}\) and compresses the air to a volume of \(50.0 \mathrm{cm}^{3}\) at \(77^{\circ} \mathrm{C} .\) What is the final pressure of the gas in the cylinder? (The ratio of before and after volumesin this case, 400: 50 or \(8: 1-\) is called the compression ratio.
Step-by-Step Solution
Verified Answer
The final pressure is approximately 9.72 atm.
1Step 1: Understand the Problem and Given Data
You start with the initial state of an ideal gas in the cylinder with a volume of \( V_1 = 400 \, \text{cm}^3 \), pressure \( P_1 = 1.00 \, \text{atm} \), and temperature \( T_1 = 15^{\circ} \text{C} \). This gas is compressed to a volume of \( V_2 = 50 \, \text{cm}^3 \) and temperature \( T_2 = 77^{\circ} \text{C} \). We need to calculate the final pressure \( P_2 \).
2Step 2: Convert Temperatures to Kelvin
The gas law calculations require temperature in Kelvin. Convert the initial and final temperatures: \[ T_1 = 15 + 273.15 = 288.15 \, \text{K} \] \[ T_2 = 77 + 273.15 = 350.15 \, \text{K} \]
3Step 3: Use the Ideal Gas Law Relation
The ideal gas law states that \( PV = nRT \). For a given amount of gas, \[ \frac{P_1 V_1}{T_1} = \frac{P_2 V_2}{T_2} \]. Rearrange to find \( P_2 \): \[ P_2 = P_1 \times \frac{V_1}{V_2} \times \frac{T_2}{T_1} \].
4Step 4: Substitute Known Values
Substitute the known values into the equation: \[ P_2 = 1.00 \times \frac{400}{50} \times \frac{350.15}{288.15} \].
5Step 5: Calculate the Final Pressure
Calculate \( P_2 \): - Calculate the volume ratio: \( \frac{400}{50} = 8 \).- Calculate the temperature ratio: \( \frac{350.15}{288.15} \approx 1.215 \).- Therefore, \( P_2 = 1.00 \times 8 \times 1.215 \approx 9.72 \, \text{atm} \).
Key Concepts
Compression RatioGas Pressure CalculationTemperature Conversion to Kelvin
Compression Ratio
In the context of an engine, the compression ratio is a critical concept that helps in understanding how much the air-fuel mixture is compressed in a cylinder. It is the ratio of the volume of the cylinder when the piston is at its lowest point (bottom dead center) to the volume when the piston is at its highest point (top dead center). This is an important factor in engine efficiency.
For the given problem, the initial and final volumes are essential to compute the compression ratio. The volumes are 400 cm³ to 50 cm³ respectively. Thus, the compression ratio can be calculated as:
For the given problem, the initial and final volumes are essential to compute the compression ratio. The volumes are 400 cm³ to 50 cm³ respectively. Thus, the compression ratio can be calculated as:
- Initial volume = 400 cm³ (when the piston is at bottom dead center)
- Compressed volume = 50 cm³ (when the piston is at top dead center)
Gas Pressure Calculation
Understanding how to calculate the pressure of a gas after compression involves utilizing the Ideal Gas Law. This law combines pressure, volume, and temperature to describe the state of an ideal gas. In this scenario, we calculate the final pressure after compression using this key equation:
By rearranging this equation, we solve for the final pressure \( P_2 \) as follows:
- Ideal Gas Law: \( PV = nRT \)
By rearranging this equation, we solve for the final pressure \( P_2 \) as follows:
- \( P_2 = P_1 \times \frac{V_1}{V_2} \times \frac{T_2}{T_1} \)
Temperature Conversion to Kelvin
Converting temperatures to Kelvin is crucial when dealing with the Ideal Gas Law because it is based on absolute temperature. The Kelvin scale starts at absolute zero, the point at which particle motion stops, making it ideal for gas calculations.
To convert Celsius to Kelvin, simply add 273.15 to the Celsius temperature.
In this problem:
To convert Celsius to Kelvin, simply add 273.15 to the Celsius temperature.
In this problem:
- Initial temperature: 15°C becomes \( 15 + 273.15 = 288.15 \, K \)
- Final temperature: 77°C becomes \( 77 + 273.15 = 350.15 \, K \)
Other exercises in this chapter
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