Thermodynamics
Worked examples
Worked example: enthalpy vs. internal energy in a vented bioreactor
In notes →Question. An aerobic fermentation runs in a bioreactor vented to hold a constant headspace pressure of 101.3 kPa (1 atm). Over one hour, the culture's respiration is exothermic enough that the cooling jacket has to remove 850 kJ of heat to hold temperature — so kJ. Off-gas analysis shows CO production exceeds O consumption enough that the gas phase expands by 50 L ( m³) over that hour. Find for the hour, and compare it with .
Solution.
- At constant pressure, kJ.
- Compute the pressure–volume work term: kJ.
- Rearrange to solve for : kJ.
Answer: kJ, compared with kJ — a difference of about 5 kJ, or roughly 0.6% of the total.
That 5 kJ is real energy: it is what left the system as gas-phase expansion work against the vent, not as heat the jacket could remove. It is small here because the gas volume change is small relative to the heat released, but it is exactly the term you would need to close an energy balance around the headspace or size an off-gas system — and in a sealed, gas-generating process where is larger, it stops being a rounding error.
Worked example: does a growing cell violate the second law?
In notes →Question. Over one hour, a growing microbial culture assembles disordered nutrients (glucose, amino acids) into ordered biomass, decreasing the system's entropy by kJ/K. In that same hour, the culture's respiration releases 850 kJ of heat to the surroundings (the reactor's cooling water), held at a constant K (37 °C). Find and , and check whether the second law holds.
Solution.
- For a large reservoir at constant temperature, heat released by the system raises the surroundings' entropy by .
- kJ/K.
- kJ/K.
Answer: kJ/K — positive, so the second law holds. The cell's own entropy fell, but the heat it released into the surroundings raised their entropy by more, so the total for system plus surroundings still increased.