Nitrogen turbine. Nitrogen expands from 30 bar, 600°C to 12 bar in a turbine operating at steady-state. Assume nitrogen to be an ideal gas (C₂=29 J/mol-K). a. Calculate the amount of work and the final temperature if expansion is reversible. b. Repeat the calculation if the efficiency of the turbine is 82% and report the lost work.

Introduction to Chemical Engineering Thermodynamics
8th Edition
ISBN:9781259696527
Author:J.M. Smith Termodinamica en ingenieria quimica, Hendrick C Van Ness, Michael Abbott, Mark Swihart
Publisher:J.M. Smith Termodinamica en ingenieria quimica, Hendrick C Van Ness, Michael Abbott, Mark Swihart
Chapter1: Introduction
Section: Chapter Questions
Problem 1.1P
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### Nitrogen Turbine Analysis

In this example, we examine the behavior of nitrogen gas expanding in a turbine under specified conditions. The expansion of nitrogen occurs from an initial pressure and temperature, leading to a specific final pressure. The conditions are as follows:

- **Initial Pressure (P1)**: 30 bar
- **Initial Temperature (T1)**: 600°C
- **Final Pressure (P2)**: 12 bar

We assume that nitrogen behaves as an ideal gas with a constant specific heat capacity at constant pressure (\(C_p\)) provided as:

- \(C_p = 29 \, \text{J/(mol·K)}\)

The problem is divided into two parts:
  
#### Part (a): Reversible Expansion
1. **Objective**: Calculate the work done and the final temperature when the expansion is reversible.
2. **Approach**: Utilize the principles of thermodynamics for a reversible process.

#### Part (b): Real Expansion with Efficiency Consideration
1. **Objective**: Recalculate the work done considering the turbine operates with 82% efficiency, and report the lost work.
2. **Approach**: Apply the efficiency factor to the work calculated in (a), and determine the corresponding loss.

#### Understanding Principles and Formulas
- **Reversible Process**: A process that can be reversed without leaving any change in both the system and the surroundings.
- **Efficiency of Turbine (\(\eta\))**: The ratio of actual work output to the ideal (reversible) work output.

\[ \eta = \frac{\text{Actual Work}}{\text{Reversible Work}} \]

\[ \text{Loss of Work} = \text{Reversible Work} - \text{Actual Work} \]

### Steps for Calculation
1. **For Part (a)**:
   - Use the ideal gas law and isentropic relations for a reversible adiabatic process to find work output and final temperature.
   - **Isentropic Process Formulae**:
     \[ \left( \frac{T_2}{T_1} \right) = \left( \frac{P_2}{P_1} \right)^{\frac{\gamma - 1}{\gamma}} \]
     \[ W = C_p(T_1 - T_2) \]
   - Where \(\gamma\) is the heat capacity ratio \(\
Transcribed Image Text:### Nitrogen Turbine Analysis In this example, we examine the behavior of nitrogen gas expanding in a turbine under specified conditions. The expansion of nitrogen occurs from an initial pressure and temperature, leading to a specific final pressure. The conditions are as follows: - **Initial Pressure (P1)**: 30 bar - **Initial Temperature (T1)**: 600°C - **Final Pressure (P2)**: 12 bar We assume that nitrogen behaves as an ideal gas with a constant specific heat capacity at constant pressure (\(C_p\)) provided as: - \(C_p = 29 \, \text{J/(mol·K)}\) The problem is divided into two parts: #### Part (a): Reversible Expansion 1. **Objective**: Calculate the work done and the final temperature when the expansion is reversible. 2. **Approach**: Utilize the principles of thermodynamics for a reversible process. #### Part (b): Real Expansion with Efficiency Consideration 1. **Objective**: Recalculate the work done considering the turbine operates with 82% efficiency, and report the lost work. 2. **Approach**: Apply the efficiency factor to the work calculated in (a), and determine the corresponding loss. #### Understanding Principles and Formulas - **Reversible Process**: A process that can be reversed without leaving any change in both the system and the surroundings. - **Efficiency of Turbine (\(\eta\))**: The ratio of actual work output to the ideal (reversible) work output. \[ \eta = \frac{\text{Actual Work}}{\text{Reversible Work}} \] \[ \text{Loss of Work} = \text{Reversible Work} - \text{Actual Work} \] ### Steps for Calculation 1. **For Part (a)**: - Use the ideal gas law and isentropic relations for a reversible adiabatic process to find work output and final temperature. - **Isentropic Process Formulae**: \[ \left( \frac{T_2}{T_1} \right) = \left( \frac{P_2}{P_1} \right)^{\frac{\gamma - 1}{\gamma}} \] \[ W = C_p(T_1 - T_2) \] - Where \(\gamma\) is the heat capacity ratio \(\
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