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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 must first calculate the total energy supplied by the heater. This is given by:

Q=PimestQ = P imes t where:

  • P=12WP = 12 \, \text{W} (power of the heater)
  • t=890st = 890 \, \text{s} (time duration)

Thus,

Q=12W×890s=10680JQ = 12 \, \text{W} \times 890 \, \text{s} = 10680 \, \text{J}

Next, we can express the energy in terms of the mass of nitrogen and its specific heat capacity:

Q=mcΔTQ = m c \Delta T where:

  • m=0.050kgm = 0.050 \, \text{kg}
  • cc is the specific heat capacity we want to find.
  • ΔT=77K70K=7K\Delta T = 77 \, \text{K} - 70 \, \text{K} = 7 \, \text{K}

Rearranging the equation for cc, we have:

c=QmΔTc = \frac{Q}{m \Delta T}

Substituting the values:

c=10680J0.050kg×7K=30600Jkg1K1c = \frac{10680 \, \text{J}}{0.050 \, \text{kg} \times 7 \, \text{K}} = 30600 \, \text{J} \, \text{kg}^{-1} \, \text{K}^{-1}

Therefore, the specific heat capacity of liquid nitrogen is approximately 30600J kg1K130600 \, \text{J kg}^{-1} \text{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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Answer

To find the work done during the expansion of the nitrogen gas, we can use the formula:

W=PΔVW = P \Delta V

Where:

  • P=1.0×106PaP = 1.0 \times 10^6 \, \text{Pa} (constant pressure)

To find the volume change, we will compare the densities of nitrogen in its liquid and gaseous states:

  • Density of liquid nitrogen: ρliquid=810kg m3\rho_{liquid} = 810 \, \text{kg m}^{-3}
  • Density of nitrogen gas: ρgas=3.8kg m3\rho_{gas} = 3.8 \, \text{kg m}^{-3}

Using the equation for density (ρ=mV\rho = \frac{m}{V}), we can find the respective volumes:

For the liquid nitrogen:

Vliquid=mρliquid=0.050kg810kg m36.17×105m3V_{liquid} = \frac{m}{\rho_{liquid}} = \frac{0.050 \, \text{kg}}{810 \, \text{kg m}^{-3}} \approx 6.17 \times 10^{-5} \, \text{m}^3

For the nitrogen gas:

Vgas=mρgas=0.050kg3.8kg m30.01316m3V_{gas} = \frac{m}{\rho_{gas}} = \frac{0.050 \, \text{kg}}{3.8 \, \text{kg m}^{-3}} \approx 0.01316 \, \text{m}^3

Thus, the change in volume (ΔV\Delta V) is:

ΔV=VgasVliquid0.01316m36.17×105m30.01310m3\Delta V = V_{gas} - V_{liquid} \approx 0.01316 \, \text{m}^3 - 6.17 \times 10^{-5} \, \text{m}^3 \approx 0.01310 \, \text{m}^3

Calculating the work done:

W=1.0×106Pa×0.01310m313100JW = 1.0 \times 10^6 \, \text{Pa} \times 0.01310 \, \text{m}^3 \approx 13100 \, \text{J}

Thus, the work done is W13100JW \approx 13100 \, \text{J}.

Step 3

The energy required to change the state of the nitrogen from a liquid to a gas is Y.

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Answer

The energy required to change the state of nitrogen from a liquid to a gas can be calculated using the specific latent heat of vaporization:

Y=mLY = m L where:

  • m=0.050kgm = 0.050 \, \text{kg} (mass of the nitrogen)
  • L=2.0×105J kg1L = 2.0 \times 10^5 \, \text{J kg}^{-1} (latent heat of vaporization)

Thus,

Y=0.050kg×2.0×105J kg1=10000JY = 0.050 \, \text{kg} \times 2.0 \times 10^5 \, \text{J kg}^{-1} = 10000 \, \text{J}

Therefore, the energy required to change the state of nitrogen is Y10000JY \approx 10000 \, \text{J}.

Step 4

Deduce which is greater, X or Y.

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Answer

From our calculations:

  • The work done by nitrogen (X13100JX \approx 13100 \, \text{J})
  • The energy required to change the state of nitrogen (Y10000JY \approx 10000 \, \text{J})

We can see that:

  • X>YX > Y

Thus, the work done by the nitrogen in the cylinder when expanding is greater than the energy required to change its state.

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