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Figure 1 shows a perfectly insulated cylinder containing 0.050 kg of liquid nitrogen at a temperature of 70 K - AQA - A-Level Physics - Question 1 - 2019 - Paper 2

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Figure 1 shows a perfectly insulated cylinder containing 0.050 kg of liquid nitrogen at a temperature of 70 K. A heater transfers energy at a constant rate of 12 W t... show full transcript

Worked Solution & Example Answer:Figure 1 shows a perfectly insulated cylinder containing 0.050 kg of liquid nitrogen at a temperature of 70 K - AQA - A-Level Physics - Question 1 - 2019 - Paper 2

Step 1

Calculate the specific heat capacity of liquid nitrogen

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Answer

To find the specific heat capacity of liquid nitrogen, we first need to calculate the total energy supplied by the heater:

P=12W,t=890sP = 12 \, \text{W}, \quad t = 890 \, \text{s}

The total energy ( Q) supplied is:

Q=P×t=12×890=10680JQ = P \times t = 12 \times 890 = 10 680 \, \text{J}

Since the nitrogen is heated from 70 K to its boiling point of 77 K, the temperature change (ΔT) is:

ΔT=7770=7 K\Delta T = 77 - 70 = 7 \ \, \text{K}

Using the formula for specific heat capacity (c):

Q=mcΔTQ = m \cdot c \cdot \Delta T

Where:

  • m = mass of liquid nitrogen = 0.050 kg
  • Q = total energy = 10 680 J

Rearranging gives:

c=QmΔT=106800.0507=106800.35=30600J kg1K1c = \frac{Q}{m \cdot \Delta T} = \frac{10 680}{0.050 \cdot 7} = \frac{10 680}{0.35} = 30 600 \, \text{J kg}^{-1} \text{K}^{-1}

Thus, the specific heat capacity of liquid nitrogen is approximately 30 600 J kg^-1 K^-1.

Step 2

The work done by the nitrogen in the cylinder when expanding due to a change of state is X.

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The energy required to change the state of the nitrogen from a liquid to a gas is given by the latent heat of vaporisation:

Y=mLwhereL=2.0×105Jkg1Y = m \cdot L \, \text{where} \, L = 2.0 \times 10^5 J kg^{-1} Substituting the mass:

Y=0.0502.0×105=10000JY = 0.050 \cdot 2.0 \times 10^5 = 10 000 \, \text{J}

The work done during expansion (X) can be calculated using the formula:

X=PΔVX = P \Delta V

Here, the change in volume (ΔV) is due to the density changes:

  • Density of liquid nitrogen = 810 kg m^-3
  • Density of nitrogen gas = 3.8 kg m^-3

Calculating the volumes:

Volume of liquid nitrogen: Vliquid=mdensityliquid=0.050810=6.17×105m3V_{liquid} = \frac{m}{density_{liquid}} = \frac{0.050}{810} = 6.17 \times 10^{-5} \, \text{m}^3

Volume of nitrogen gas: Vgas=mdensitygas=0.0503.8=0.01316m3V_{gas} = \frac{m}{density_{gas}} = \frac{0.050}{3.8} = 0.01316 \, \text{m}^3

Thus,

ΔV=VgasVliquid=0.013166.17×1050.0131m3\Delta V = V_{gas} - V_{liquid} = 0.01316 - 6.17 \times 10^{-5} \approx 0.0131 \, \text{m}^3

Now using the pressure given: X=(1.0×105)(0.0131)1310JX = (1.0 \times 10^5) \cdot (0.0131) \approx 1 310 \, \text{J}

Comparing X and Y, we see: Y (10 000 J) is greater than X (1 310 J). Therefore, Y is greater than X.

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