The first law of thermodynamics is a principle concerning the conservation of energy. It is typically expressed as:
\(\Delta U = q + w\)
where:
- \(\Delta U\): Change in the internal energy of the system
- \(q\): Heat added to the system
- \(w\): Work done on the system
Let us analyze the given options:
- Cyclic process: \(q = -w\)
- In a cyclic process, the system returns to its initial state. Hence, the change in internal energy, \(\Delta U\), is zero.
- Thus, \(0 = q + w \Rightarrow q = -w\).
- This equation correctly represents the first law for a cyclic process.
- Adiabatic process: \(\Delta U = -w\)
- In an adiabatic process, no heat is exchanged with the surroundings, hence \(q = 0\).
- Therefore, the first law becomes \(\Delta U = 0 + w \Rightarrow \Delta U = w\).
- The given statement \(\Delta U = -w\) is incorrect for an adiabatic process.
- Isochoric process: \(\Delta U = q\)
- In an isochoric process, the volume remains constant, meaning no work is performed (\(w = 0\)).
- Therefore, the first law becomes \(\Delta U = q + 0 \Rightarrow \Delta U = q\).
- This equation correctly represents the first law for an isochoric process.
- Isothermal process: \(q = -w\)
- In an isothermal process, the temperature remains constant, leading to no change in internal energy (\(\Delta U = 0\)).
- Therefore, the first law becomes \(0 = q + w \Rightarrow q = -w\).
- This equation correctly represents the first law for an isothermal process.
Thus, the equation for the adiabatic process \(\Delta U = -w\) does not correctly represent the first law of thermodynamics for the given process, making it the correct answer.