Thermodynamics — Class 11 Physics
Physics Part II · Chapter 4
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- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
- Space weighted by unit marks
- Charts from the book's own data
- Traps corrected
Chapter summary
Key ideas & terms
- Internal energy
- The total energy of a system stored in its molecules due to molecular motion and configuration; a state variable.
- Zeroth law
- The law stating that two systems each in thermal equilibrium with a third are in thermal equilibrium with each other.
- First law of thermodynamics
- The conservation of energy applied to heat,
. - Adiabatic process
- A process in which no heat is exchanged with the surroundings (
). - Second law of thermodynamics
- The principle that heat cannot flow spontaneously from a colder to a hotter body and no engine can fully convert heat to work.
- Carnot engine
- An ideal reversible heat engine working between two temperatures with the maximum possible efficiency.
Extra questions & answers
State the zeroth law of thermodynamics.
If two systems are each in thermal equilibrium with a third system, they are in thermal equilibrium with one another, which lets temperature be defined.
State the first law of thermodynamics.
The heat supplied to a system equals the increase in internal energy plus the work done by the system,
What is internal energy and why is it a state variable?
It is the total molecular energy of a system; it depends only on the state, not on how the state was reached.
Relate the two molar specific heats of an ideal gas.
For an ideal gas
Distinguish isothermal and adiabatic processes.
In an isothermal process temperature is constant and heat is exchanged; in an adiabatic process no heat is exchanged and temperature changes.
State the Clausius statement of the second law.
Heat cannot flow of itself from a colder body to a hotter body without external work being done.
State the Kelvin-Planck statement of the second law.
No process is possible whose sole result is the complete conversion of heat from a reservoir into work.
Distinguish reversible and irreversible processes.
A reversible process can be retraced exactly through equilibrium states with no dissipation; real processes are irreversible due to friction and finite temperature differences.
Write the efficiency of a Carnot engine.
Why is the Carnot engine the most efficient?
Because it is reversible; no engine working between the same two temperatures can have a greater efficiency (Carnot's theorem).


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