The first law of thermodynamics concerns the internal energy of a gas and how it changes.
Definition: Internal energy (U) refers to the total thermal energy contained within a gas.
Components:
Composed of the kinetic energy of all the particles within the gas.
Represents the sum of the kinetic energies of the individual particles.
The internal energy of a gas can change in two primary ways:
Gain or Loss of Heat (Q)
If the gas is heated (e.g., above a Bunsen burner), it gains thermal energy:
Internal energy (U) increases.
Temperature increases; particles move faster.
If the gas loses heat, it cools down:
Internal energy (U) decreases.
Temperature decreases; particles slow down.
Work Done (W)
Work Done by the Gas: When the gas expands, it does work (e.g., pushing a piston).
This results in a decrease in internal energy.
Work Done on the Gas: If work is done on the gas (e.g., compressing it), its internal energy increases.
Fundamental Equation:
[ Q = \Delta U + W ]
Where:
Q = Heat added to the gas
\Delta U = Change in internal energy
W = Work done by the gas
Conservation of Energy: The energy provided to the gas must result in an increase in internal energy or work being done by/on the gas.
If heat is added to the gas, and it does no work (W=0):
[ Q = \Delta U ]
Internal energy increases as temperature rises.
In an adiabatic process:
When Q = 0 (no heat exchange), the equation simplifies to:
[ 0 = \Delta U + W ]
Indicates that work done by the gas results in a drop in internal energy.
Compression of Air in a Bicycle Pump:
Work is done on the air as it is compressed.
Resulting increase in internal energy causes the air to heat up.
Operation of a Fridge:
When the fridge turns on, internal energy of the air inside decreases, causing it to get colder.
The motor does work to move the refrigerant, thus lowering the internal energy.
The internal energy of a gas can increase either by adding heat or by doing work on it.
Understanding of terms such as internal energy (\Delta U), heat (Q), and work (W) is crucial for grasping the first law of thermodynamics.