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When 1,2 kg of this gas is heated from 15°C to 210°C at constant pressure, the heat required is 160 kJ. If the characteristic gas constant is R = 0,242 kJ/kg.K, determine the:

Physics

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2 parts
12.1

0.684 kJ/(kg⋅K)0.684 \text{ kJ/(kg} \cdot \text{K)}

12.2

0.442 kJ/(kg⋅K)0.442 \text{ kJ/(kg} \cdot \text{K)}

Step-by-step solution

5 steps

Here are the solutions to the problems:

10. Determine the value of the index of expansion nn.

Step 1: Write down the given values and the polytropic process equation.
The process follows the law P1V1n=P2V2nP_1 V_1^n = P_2 V_2^n.
Given:
P1=480 kPaP_1 = 480 \text{ kPa}
V1=4.4 m3V_1 = 4.4 \text{ m}^3
P2=156.88 kPaP_2 = 156.88 \text{ kPa}
V2=10.4 m3V_2 = 10.4 \text{ m}^3

Step 2: Rearrange the equation to solve for nn.

P1P2=(V2V1)n\frac{P_1}{P_2} = \left(\frac{V_2}{V_1}\right)^n

Taking the natural logarithm of both sides:

ln⁡(P1P2)=nln⁡(V2V1)\ln\left(\frac{P_1}{P_2}\right) = n \ln\left(\frac{V_2}{V_1}\right) n=ln⁡(P1P2)ln⁡(V2V1)n = \frac{\ln\left(\frac{P_1}{P_2}\right)}{\ln\left(\frac{V_2}{V_1}\right)}

Step 3: Substitute the given values and calculate nn.

n=ln⁡(480 kPa156.88 kPa)ln⁡(10.4 m34.4 m3)n = \frac{\ln\left(\frac{480 \text{ kPa}}{156.88 \text{ kPa}}\right)}{\ln\left(\frac{10.4 \text{ m}^3}{4.4 \text{ m}^3}\right)} n=ln⁡(3.060938)ln⁡(2.363636)n = \frac{\ln(3.060938)}{\ln(2.363636)} n=1.11890.8603n = \frac{1.1189}{0.8603} n≈1.30n \approx 1.30

The value of the index of expansion is 1.30\boxed{1.30}.

11. Calculate the value of the characteristic gas constant RR.

Step 1: Convert temperature to Kelvin and pressure to Pascals.
Given:
P=120 kPa=120×103 PaP = 120 \text{ kPa} = 120 \times 10^3 \text{ Pa}
T=20∘C=20+273.15=293.15 KT = 20^\circ \text{C} = 20 + 273.15 = 293.15 \text{ K}
ρ=1.68 kg/m3\rho = 1.68 \text{ kg/m}^3

Step 2: Use the ideal gas law in terms of density to find RR.
The ideal gas law is P=ρRTP = \rho R T.
Rearrange to solve for RR:

R=PρTR = \frac{P}{\rho T}

Step 3: Substitute the values and calculate RR.

R=120×103 Pa(1.68 kg/m3)(293.15 K)R = \frac{120 \times 10^3 \text{ Pa}}{(1.68 \text{ kg/m}^3)(293.15 \text{ K})} R=120000492.492R = \frac{120000}{492.492} R≈243.66 J/(kg⋅K)R \approx 243.66 \text{ J/(kg} \cdot \text{K)}

Converting to kJ/(kg⋅K)\text{kJ/(kg} \cdot \text{K)}:

R≈0.24366 kJ/(kg⋅K)R \approx 0.24366 \text{ kJ/(kg} \cdot \text{K)}

The characteristic gas constant is 0.244 kJ/(kg⋅K)\boxed{0.244 \text{ kJ/(kg} \cdot \text{K)}}.

12. Determine the specific heat capacities.

Given:
m=1.2 kgm = 1.2 \text{ kg}
T1=15∘C=15+273.15=288.15 KT_1 = 15^\circ \text{C} = 15 + 273.15 = 288.15 \text{ K}
T2=210∘C=210+273.15=483.15 KT_2 = 210^\circ \text{C} = 210 + 273.15 = 483.15 \text{ K}
Q=160 kJQ = 160 \text{ kJ} (at constant pressure)
R=0.242 kJ/(kg⋅K)R = 0.242 \text{ kJ/(kg} \cdot \text{K)}

Part 12.1· 3 steps

Specific heat capacity of the gas at constant pressure (cpc_p).

  1. Calculate the change in temperature (ΔT\Delta T).

    ΔT=T2−T1=483.15 K−288.15 K=195 K\Delta T = T_2 - T_1 = 483.15 \text{ K} - 288.15 \text{ K} = 195 \text{ K}
  2. Use the formula for heat transfer at constant pressure to find cpc_p.

    Q=mcpΔTQ = m c_p \Delta T

    Rearrange to solve for cpc_p:

    cp=QmΔTc_p = \frac{Q}{m \Delta T}
  3. Substitute the values and calculate cpc_p.

    cp=160 kJ(1.2 kg)(195 K)c_p = \frac{160 \text{ kJ}}{(1.2 \text{ kg})(195 \text{ K})} cp=160234c_p = \frac{160}{234} cp≈0.684 kJ/(kg⋅K)c_p \approx 0.684 \text{ kJ/(kg} \cdot \text{K)}

    The specific heat capacity at constant pressure is 0.684 kJ/(kg⋅K)\boxed{0.684 \text{ kJ/(kg} \cdot \text{K)}}.

Part 12.2

0.442 kJ/(kg⋅K)0.442 \text{ kJ/(kg} \cdot \text{K)}

Specific heat capacity of the gas at constant volume (cvc_v).

  1. Use Mayer's relation, which connects cpc_p, cvc_v, and RR.

    cp−cv=Rc_p - c_v = R

    Rearrange to solve for cvc_v:

    cv=cp−Rc_v = c_p - R
  2. Substitute the calculated cpc_p from 12.1 and the given RR.

    cv=0.68376 kJ/(kg⋅K)−0.242 kJ/(kg⋅K)c_v = 0.68376 \text{ kJ/(kg} \cdot \text{K)} - 0.242 \text{ kJ/(kg} \cdot \text{K)} cv=0.44176 kJ/(kg⋅K)c_v = 0.44176 \text{ kJ/(kg} \cdot \text{K)}

    The specific heat capacity at constant volume is 0.442 kJ/(kg⋅K)\boxed{0.442 \text{ kJ/(kg} \cdot \text{K)}}.

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