SUMMARY
During an adiabatic process, if 37 J of work is done on the system, the work done by the system is -37 J. This indicates that the change in internal energy (ΔU) is equal to 37 J, as per the equation ΔU = -W, where W is the work done on the system. The discussion clarifies that negative work does not imply impossibility; rather, it reflects the energy transfer direction. Therefore, the scenario presented is feasible and aligns with the principles of thermodynamics.
PREREQUISITES
- Understanding of adiabatic processes in thermodynamics
- Familiarity with the first law of thermodynamics
- Knowledge of internal energy concepts
- Proficiency in interpreting work-energy equations
NEXT STEPS
- Study the first law of thermodynamics in detail
- Learn about the implications of work done on and by a system
- Explore examples of adiabatic processes in real-world applications
- Investigate the relationship between heat transfer and work in thermodynamic systems
USEFUL FOR
Students of thermodynamics, physics enthusiasts, and professionals in engineering fields who require a solid understanding of energy transfer during adiabatic processes.