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Act like a helpful tutor and exlain me : Give step-by-step solution with explanation and final answer: do not draw the T-s diagram, solve completelyIn an ideal air-standard Diesel cycle, at the beginning of the isentropic compression, pressure is P; = 100kPa, temperature is T, = 25°C, and the volume is 3.7 liters. The compression ratio is 19.0. The temperature at the end of constant pressure heat addition is Ts = 1500K Using the ideal gas tables, a-> Draw the cycle on a T-s diagram b -> Complete the table below c -> Determine the thermal efficiency of the cycle poe fee [ow [ow [ow [oe ER A A A A ET A A A A I A A A A I A A RR EN E— [eu | 1 Ln ©]

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Act like a helpful tutor and exlain me : Give step-by-step solution with explanation and final answer: do not draw the T-s diagram, solve completelyUploaded ImageIn an ideal air-standard Diesel cycle, at the beginning of the isentropic compression, pressure is P; = 100kPa, temperature is T, = 25°C, and the volume is 3.7 liters. The compression ratio is 19.0. The temperature at the end of constant pressure heat addition is Ts = 1500K Using the ideal gas tables, a-> Draw the cycle on a T-s diagram b -> Complete the table below c -> Determine the thermal efficiency of the cycle poe fee [ow [ow [ow [oe ER A A A A ET A A A A I A A A A I A A RR EN E— [eu | 1 Ln ©]

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Asked by: manish kumar
Created at: 2025-10-05 22:45:17

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Let's solve the Diesel cycle problem step by step, using the **ideal gas tables** for air. --- ## **Given Data** - \( P_1 = 100 \) kPa - \( T_1 = 25^\circ C = 298\,K \) - \( V_1 = 3.7\,L = .0037\,m^3 \) - **Compression ratio**: \( r = \frac{V_1}{V_2} = 19. \) - \( T_3 = 150\,K \) (after heat addition at constant pressure) --- ## **Step 1: State Points Description** 1. **State 1**: Start of isentropic compression 2. **State 2**: End of isentropic compression (min volume) 3. **State 3**: End of constant-pressure heat addition (max temperature) 4. **State 4**: End of isentropic expansion --- ## **Step 2: Find Properties at Each State** ### **State 1** - \( P_1 = 100 \) kPa, \( T_1 = 298 \) K, \( V_1 = .0037 \) m³ Use **ideal gas equation** to find mass: \[ P_1 V_1 = m R T_1 \] \[ m = \frac{P_1 V_1}{R T_1} \] \[ R = .287 \frac{kJ}{kg \cdot K} \] \[ m = \frac{100 \times .0037}{.287 \times 298} = \frac{.37}{85.426} \approx .00433\,kg \] **Specific volume**: \[ v_1 = \frac{V_1}{m} = \frac{.0037}{.00433} \approx .854\, m^3/kg \] --- ### **State 2 (after isentropic compression)** - \( v_2 = v_1 / r = .854 / 19 = .04495\, m^3/kg \) For **isentropic compression** (\( s_2 = s_1 \)): \[ \frac{T_2}{T_1} = r^{k-1} \] For air, \( k = 1.4 \): \[ \frac{T_2}{298} = 19^{.4} \] \[ 19^{.4} \approx 2.92 \] \[ T_2 = 2.92 \times 298 \approx 869\,K \] \[ P_2 = P_1 \frac{T_2}{T_1} \frac{v_1}{v_2} \] But since \( v_1/v_2 = r \) and \( T_2/T_1 = r^{k-1} \): \[ P_2 = P_1 \cdot r^k = 100 \cdot 19^{1.4} \approx 100 \cdot 66.5 = 665\,kPa \] --- ### **State 3 (after constant-pressure heat addition)** - \( P_3 = P_2 \) - \( T_3 = 150\,K \) \[ \frac{v_3}{v_2} = \frac{T_3}{T_2} = \frac{150}{869} \approx 1.73 \] \[ v_3 = 1.73 \times v_2 = 1.73 \times .04495 \approx .0777\, m^3/kg \] --- ### **State 4 (after isentropic expansion)** Isentropic expansion back to \( v_4 = v_1 \): \[ \frac{T_4}{T_3} = \left( \frac{v_3}{v_4} \right)^{k-1} \] But \( v_4 = v_1 \), so: \[ \frac{T_4}{T_3} = \left( \frac{v_3}{v_1} \right)^{k-1} \] \[ v_3 = .0777, v_1 = .854 \] \[ \frac{v_3}{v_1} = .0777 / .854 = .091 \] \[ T_4 = T_3 \cdot (.091)^{.4} \] \[ (.091)^{.4} \approx .364 \] \[ T_4 = 150 \cdot .364 \approx 546\,K \] --- ## **Step 3: Fill the Table** | | P(kPa) | T(K) | \( v \) (\( m^3/kg \)) | \( u \) (kJ/kg) | \( s^ \) (kJ/kg·K) | |------|--------|------|------------------------|-----------------|---------------------| | 1 | 100 | 298 | .854 | \( u_1 \) | \( s^_1 \) | | 2 | 665 | 869 | .04495 | \( u_2 \) | \( s^_2 \) | | 3 | 665 | 150 | .0777 | \( u_3 \) | \( s^_3 \) | | 4 | 100 | 546 | .854 | \( u_4 \) | \( s^_4 \) | Get \( u \) and \( s^ \) from ideal gas tables for air (values below are approximate): - At 298 K: \( u_1 = 214.07 \) kJ/kg, \( s^_1 = 6.869 \) kJ/kg·K - At 869 K: \( u_2 = 632.5 \) kJ/kg, \( s^_2 = 7.950 \) kJ/kg·K - At 150 K: \( u_3 = 112.7 \) kJ/kg, \( s^_3 = 8.732 \) kJ/kg·K - At 546 K: \( u_4 = 390.7 \) kJ/kg, \( s^_4 = 7.423 \) kJ/kg·K --- ## **Step 4: Heat and Efficiency Calculations** ### **Heat Added (\( q_{in} \), 2→3): Constant Pressure** \[ q_{in} = h_3 - h_2 \] From tables: - \( h_3 \) at 150 K: 1149.7 kJ/kg - \( h_2 \) at 869 K: 873.6 kJ/kg \[ q_{in} = 1149.7 - 873.6 = 276.1\,kJ/kg \] --- ### **Heat Rejected (\( q_{out} \), 4→1): Constant Volume** \[ q_{out} = u_4 - u_1 = 390.7 - 214.07 = 176.6\,kJ/kg \] --- ### **Thermal Efficiency** \[ \eta = 1 - \frac{q_{out}}{q_{in}} = 1 - \frac{176.6}{276.1} = .36 \text{ or } 36\% \] --- ## **Summary Table** | | P(kPa) | T(K) | \( v \) (\( m^3/kg \)) | \( u \) (kJ/kg) | \( s^ \) (kJ/kg·K) | |------|--------|------|------------------------|------------------|---------------------| | 1 | 100 | 298 | .854 | 214.07 | 6.869 | | 2 | 665 | 869 | .04495 | 632.5 | 7.950 | | 3 | 665 | 150 | .0777 | 112.7 | 8.732 | | 4 | 100 | 546 | .854 | 390.7 | 7.423 | | \( q_{in} \) | | | | 276.1 | | | \( q_{out} \) | | | | 176.6 | | | \( \eta \) | | | | .36 (36%) | | --- ## **Final Answers** - **Thermal efficiency,** \( \eta = 36\% \) - **Heat added:** \( q_{in} = 276.1 \) kJ/kg - **Heat rejected:** \( q_{out} = 176.6 \) kJ/kg If you want the T-s diagram, I can describe the process, but as per your request, no drawing is provided. --- **If you need any further clarification or calculations, let me know!**

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