The objective in air compression is to reach the delivery pressure with the least possible expenditure of work. The type of thermodynamic process significantly affects the area under the P-V diagram, which represents the work done.
1. Comparing Processes on a P-V Diagram:
When air is compressed from a low pressure ($P_1$) to a higher delivery pressure ($P_2$):
• Isothermal Compression ($PV = C$): Temperature remains constant. This follows the lowest path on the P-V diagram, resulting in the smallest area and thus the
minimum work done.
• Adiabatic Compression ($PV^\gamma = C$): No heat is removed during the process. The temperature rises sharply, following the steepest path and requiring the maximum work.
• Polytropic Compression ($PV^n = C$): Represents real-world scenarios where some heat is removed ($1 \lt n \lt \gamma$). The work required is between isothermal and adiabatic.
2. The Concept of Isothermal Efficiency:
Since isothermal compression is the ideal goal for energy saving, we use "Isothermal Efficiency" to evaluate real compressors by comparing their actual work to the theoretical isothermal work.
3. Practical Implementation:
In practice, achieving perfect isothermal compression is impossible because it would require an infinitely slow stroke. However, engineers use
intercooling in multi-stage compressors to bring the process as close to isothermal as possible to save energy.