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Act like a helpful tutor and exlain me : Give step-by-step solution with explanation and final answer:An adiabatic gas turbine expands air at 1 3 0 0 kPa and 5 0 0 ° C to 1 0 0 kPa and 1 2 7 ° C . Air enters the turbine through a 0 . 2 m ^ 2 opening with an average velocity of 4 0 m / s , and exhausts through a 1 m ^ 2 opening. Determine ( a ) the mass flow rate of air through the turbine and ( b ) the power produced by the turbine.

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Act like a helpful tutor and exlain me : Give step-by-step solution with explanation and final answer:An adiabatic gas turbine expands air at 1 3 0 0 kPa and 5 0 0 ° C to 1 0 0 kPa and 1 2 7 ° C . Air enters the turbine through a 0 . 2 m ^ 2 opening with an average velocity of 4 0 m / s , and exhausts through a 1 m ^ 2 opening. Determine ( a ) the mass flow rate of air through the turbine and ( b ) the power produced by the turbine.

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Asked by: manish kumar
Created at: 2025-10-07 15:04:27

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# Gas Turbine Expansion: Step-by-Step Solution We are given: - **Inlet conditions**: - Pressure, \( P_1 = 130 \) kPa - Temperature, \( T_1 = 500^\circ \mathrm{C} = 773.15 \) K - Area, \( A_1 = .2 \) m² - Velocity, \( V_1 = 40 \) m/s - **Exit conditions**: - Pressure, \( P_2 = 100 \) kPa - Temperature, \( T_2 = 127^\circ \mathrm{C} = 400.15 \) K - Area, \( A_2 = 1 \) m² - **The process is adiabatic** (no heat transfer). We are to find: 1. The **mass flow rate** of air (\( \dot{m} \)) 2. The **power produced** by the turbine (\( \dot{W}_{turbine} \)) --- ## Step 1: Find Mass Flow Rate (\( \dot{m} \)) The mass flow rate is: \[ \dot{m} = \rho_1 A_1 V_1 \] First, calculate the **density at inlet** (\( \rho_1 \)) using the ideal gas law: \[ \rho_1 = \frac{P_1}{R T_1} \] Where \( R = .287 \) kJ/kg·K \( = 287 \) J/kg·K Plug in values (convert kPa to Pa): - \( P_1 = 130 \) kPa \( = 1,300,000 \) Pa - \( T_1 = 773.15 \) K \[ \rho_1 = \frac{1,300,000}{287 \times 773.15} \approx \frac{1,300,000}{221,849} \approx 5.86 \text{ kg/m}^3 \] Now, calculate mass flow rate: \[ \dot{m} = 5.86 \times .2 \times 40 = 5.86 \times 8 = 46.88 \text{ kg/s} \] --- ## Step 2: Power Produced by the Turbine (\( \dot{W}_{turbine} \)) Use the **steady-flow energy equation** for an adiabatic turbine: \[ \dot{W}_{turbine} = \dot{m} \left[ (h_1 - h_2) + \frac{V_1^2 - V_2^2}{2} \right] \] ### 2.1. Find Exit Velocity (\( V_2 \)) First, find the **exit density** (\( \rho_2 \)): - \( P_2 = 100 \) kPa \( = 100,000 \) Pa - \( T_2 = 400.15 \) K \[ \rho_2 = \frac{100,000}{287 \times 400.15} \approx \frac{100,000}{114,843} \approx .87 \text{ kg/m}^3 \] The exit mass flow rate is also: \[ \dot{m} = \rho_2 A_2 V_2 \implies V_2 = \frac{\dot{m}}{\rho_2 A_2} \] \[ V_2 = \frac{46.88}{.87 \times 1} \approx 53.9 \text{ m/s} \] --- ### 2.2. Find Enthalpy Change (\( h_1 - h_2 \)) For air, \( h = C_p T \), where \( C_p = 1.005 \) kJ/kg·K. \[ h_1 - h_2 = C_p (T_1 - T_2) \] \[ = 1.005 \times (773.15 - 400.15) = 1.005 \times 373 = 374.87 \text{ kJ/kg} \] --- ### 2.3. Find Kinetic Energy Change \[ \frac{V_1^2 - V_2^2}{2} = \frac{40^2 - 53.9^2}{2} \] \[ 40^2 = 160,\quad 53.9^2 \approx 2906.5 \] \[ \Rightarrow \frac{160 - 2906.5}{2} = \frac{-1306.5}{2} = -653.25 \text{ (m}^2\text{/s}^2) \] Convert to kJ/kg: \( 1 \text{ kJ/kg} = 100 \text{ m}^2/\text{s}^2 \): \[ \text{Kinetic energy change} = -.653 \text{ kJ/kg} \] --- ### 2.4. Total Work Output \[ \dot{W}_{turbine} = \dot{m} \left[ (h_1 - h_2) + \left( \frac{V_1^2 - V_2^2}{2 \times 100} \right) \right] \] \[ = 46.88 \left[ 374.87 - .653 \right] = 46.88 \times 374.22 = 17,554 \text{ kW} \] --- ## **Final Answers** **(a) Mass flow rate:** \[ \boxed{46.9 \ \text{kg/s}} \] **(b) Power produced by the turbine:** \[ \boxed{17,550 \ \text{kW}} \] --- ### **Summary Table** | Quantity | Value | |-----------------------|----------------| | Mass flow rate (\(\dot{m}\)) | 46.9 kg/s | | Power output (\(\dot{W}_{turbine}\)) | 17,550 kW | --- **Note:** - All values rounded appropriately. - If you have access to air property tables, you could use more accurate enthalpy values. - The kinetic energy term is small compared to the enthalpy term, but should be included for accuracy.

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