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Figure 4 shows a gas strut supporting the lid of a trailer - AQA - A-Level Physics - Question 3 - 2017 - Paper 6

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Figure 4 shows a gas strut supporting the lid of a trailer. A fixed mass of nitrogen gas is sealed into the cylinder of the strut. The gas is initially at a pressu... show full transcript

Worked Solution & Example Answer:Figure 4 shows a gas strut supporting the lid of a trailer - AQA - A-Level Physics - Question 3 - 2017 - Paper 6

Step 1

Calculate the pressure and temperature of the gas at the end of the compression assuming the compression to be an adiabatic process.

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Answer

To find the final pressure and temperature after adiabatic compression, we can use the formulas for adiabatic processes:

  1. The pressure-volume relationship: P_1 V_1^{ rac{eta}{eta-1}} = P_2 V_2^{ rac{eta}{eta-1}}
  2. The temperature-volume relationship: T_1 V_1^{eta - 1} = T_2 V_2^{eta - 1}

Where:

  • P1=1.2×106PaP_1 = 1.2 \times 10^6 \, \text{Pa} (initial pressure)
  • V1=9.0×105m3V_1 = 9.0 \times 10^{-5} \, \text{m}^3 (initial volume)
  • V2=6.8×103m3V_2 = 6.8 \times 10^{-3} \, \text{m}^3 (final volume)
  • T1=290KT_1 = 290 \, \text{K} (initial temperature)
  • eta = 1.4 (adiabatic index for nitrogen)

Step 1: Calculate final pressure P2P_2:

P2=P1(V1V2)βP_2 = P_1 \left( \frac{V_1}{V_2} \right)^{\beta} P2=1.2×106(9.0×1056.8×103)1.4P_2 = 1.2 \times 10^6 \left( \frac{9.0 \times 10^{-5}}{6.8 \times 10^{-3}} \right)^{1.4}

Calculating this gives: P22.05×106PaP_2 \approx 2.05 \times 10^6 \, \text{Pa}

Step 2: Calculate final temperature T2T_2:

T2=T1(V1V2)β1T_2 = T_1 \left( \frac{V_1}{V_2} \right)^{\beta - 1} T2=290(9.0×1056.8×103)0.4T_2 = 290 \left( \frac{9.0 \times 10^{-5}}{6.8 \times 10^{-3}} \right)^{0.4}

Calculating this gives: T2336KT_2 \approx 336 \, \text{K}

Thus, the final pressure is approximately 2.05×106Pa2.05 \times 10^6 \, \text{Pa} and the final temperature is approximately 336K336 \, \text{K}.

Step 2

Explain why the rapid compression of the gas can be assumed to be an adiabatic process.

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Answer

The rapid compression of the gas can be assumed to be an adiabatic process because:

  1. Insufficient Time for Heat Transfer: During rapid compression, there is not enough time for heat transfer to occur between the gas and its surroundings. Therefore, any internal energy change occurs without heat exchange.

  2. Adiabatic Condition: In adiabatic processes, the heat transfer QQ is zero. Since the process is quick, we can consider it adiabatic, adhering to the relation Q=0Q = 0.

This means that any increase in temperature during compression results solely from work done on the gas.

Step 3

When the lid is closed slowly, the compression can be assumed to be isothermal.

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Answer

In isothermal compression:

  1. Equilibrium: The gas can remain in thermal equilibrium with its surroundings since the process is slow, allowing heat to be absorbed or released as required. Therefore, the temperature can be kept constant.

  2. Work Done: The work done on the gas during isothermal compression can be determined using the formula: W=nRTln(VfVi)W = nRT \ln\left( \frac{V_f}{V_i} \right) where nn is the number of moles, RR is the universal gas constant, and TT is the constant temperature.

By this comparison, the work done in isothermal compression is generally less than in adiabatic compression due to the energy exchange with the surroundings.

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