Chapter 5 Thermodynamics Flashcards
Defining Internal Energy
The sum of the random distribution of kinetic and potential energies within a system of molecules
- The symbol for internal energy is U, with units of Joules (J)
The internal energy of a system is determined by
- Temperature
- The random motion of molecules
- The phase of matter: gases have the highest internal energy, solids have the lowest
The internal energy of a system can increase by:
- Doing work on it
- Adding heat to it
The internal energy of a system can decrease by:
- Losing heat to its surroundings
Energy can generally be classified into two forms:
- kinetic or potential energy
- The molecules of all substances contain both kinetic and potential energies
- The amount of kinetic and potential energy a substance contains depends on the phases of matter (solid, liquid or gas), this is known as the internal energy
The internal energy of an object is intrinsically related to its
- temperature
When a container containing gas molecules is heated up, the molecules begin to move around
- faster, increasing their kinetic energy
- If the object is a solid, where the molecules are tightly packed, when heated the molecules begin to vibrate more
- Molecules in liquids and solids have both kinetic and potential energy because they are close together and bound by intermolecular forces
ideal gas molecules are assumed to have no
intermolecular forces
- This means there have no potential energy, only kinetic energy
- The (change in) internal energy of an ideal gas is equal to:
ΔU=3/2KΔT
- Therefore, the change in internal energy is proportional to the change in temperature:
ΔU ∝ ΔT
- Where:
- ΔU = change in internal energy (J)
- ΔT = change in temperature (K)
As the container is heated up, the gas molecules move faster with higher kinetic energy and therefore higher internal energy
EXAM TIP
If an exam question about an ideal gas asks for the total internal energy, remember that this is equal to the total kinetic energy since an ideal gas has zero potential energy
Work Done by a Gas
- When a gas expands, it does work on its surroundings by exerting pressure on the walls of the container it’s in
- This is important, for example, in a steam engine where expanding steam pushes a piston to turn the engine
The work done when a volume of gas changes at constant pressure is defined as: equation
W = pΔV
- Where:
- W = work done (J)
- p = external pressure (Pa)
- V = volume of gas (m3)
the gas does work on the piston
- For a gas inside a cylinder enclosed by a moveable piston, the force exerted by the gas pushes the piston outwards
Derivation of W = pΔV
- The volume of gas is at constant pressure. This means the force F exerted by the gas on the piston is equal to :
F = p × A
- Where:
- p = pressure of the gas (Pa)
- A = cross-sectional area of the cylinder (m2)
- The definition of work done is:
W = F × s
- Where:
- F = force (N)
- s = displacement in the direction of force (m)
- The displacement of the gas d multiplied by the cross-sectional area A is the increase in volume ΔV of the gas:
W = p × A × s
- This gives the equation for the work done when the volume of a gas changes at constant pressure:
W = pΔV
- Where:
- ΔV = increase in the volume of the gas in the piston when expanding (m3)