The microstate of a system is completely determined by its macrostate.

The macrostate of a system is completely determined by its microstate.

The microstate and macrostate of a system are independent of each other.

The microstate and macrostate of a system are related by a probability distribution.

Entropy is directly proportional to disorder.

Entropy is inversely proportional to disorder.

Entropy is independent of disorder.

Entropy is a measure of the number of possible microstates of a system.

A probability distribution that describes the distribution of energy among the particles in a system.

A probability distribution that describes the distribution of particles among the energy levels in a system.

A probability distribution that describes the distribution of particles in a system.

A probability distribution that describes the distribution of energy in a system.

A probability distribution that describes the distribution of velocities among the particles in a gas.

A probability distribution that describes the distribution of energies among the particles in a gas.

A probability distribution that describes the distribution of particles in a gas.

A probability distribution that describes the distribution of velocities among the particles in a liquid.

A probability distribution that describes the distribution of particles among the energy levels in a system of fermions.

A probability distribution that describes the distribution of energies among the particles in a system of fermions.

A probability distribution that describes the distribution of particles in a system of fermions.

A probability distribution that describes the distribution of velocities among the particles in a system of fermions.

A probability distribution that describes the distribution of particles among the energy levels in a system of bosons.

A probability distribution that describes the distribution of energies among the particles in a system of bosons.

A probability distribution that describes the distribution of particles in a system of bosons.

A probability distribution that describes the distribution of velocities among the particles in a system of bosons.

PV = nRT

PV = NkT

PV = nT

PV = Nk

$\left(P + \frac{a}{V^2}\right)(V - b) = RT$

$\left(P + \frac{a}{V}\right)(V - b) = RT$

$\left(P + \frac{a}{V^3}\right)(V - b) = RT$

$\left(P + \frac{a}{V^4}\right)(V - b) = RT$

The temperature at which a gas can no longer be liquefied.

The temperature at which a liquid can no longer be vaporized.

The temperature at which a solid can no longer be melted.

The temperature at which a gas and a liquid can coexist in equilibrium.

The pressure at which a gas can no longer be liquefied.

The pressure at which a liquid can no longer be vaporized.

The pressure at which a solid can no longer be melted.

The pressure at which a gas and a liquid can coexist in equilibrium.

The volume at which a gas can no longer be liquefied.

The volume at which a liquid can no longer be vaporized.

The volume at which a solid can no longer be melted.

The volume at which a gas and a liquid can coexist in equilibrium.

The temperature and pressure at which a solid, liquid, and gas can coexist in equilibrium.

The temperature and pressure at which a solid and a liquid can coexist in equilibrium.

The temperature and pressure at which a liquid and a gas can coexist in equilibrium.

The temperature and pressure at which a solid and a gas can coexist in equilibrium.

$\frac{dP}{dT} = \frac{\Delta H}{T\Delta V}$

$\frac{dP}{dT} = \frac{\Delta S}{T\Delta V}$

$\frac{dP}{dT} = \frac{\Delta G}{T\Delta V}$

$\frac{dP}{dT} = \frac{\Delta U}{T\Delta V}$

The cooling of a gas when it is allowed to expand freely.

The heating of a gas when it is allowed to expand freely.

The cooling of a gas when it is compressed.

The heating of a gas when it is compressed.

A process in which there is no heat transfer between the system and its surroundings.

A process in which there is heat transfer between the system and its surroundings.

A process in which the temperature of the system remains constant.

A process in which the pressure of the system remains constant.