AQA A-level Physics (7408) · 3.11.2.2

Non-flow processes (A-level only) Flashcards – AQA A-level Physics (7408)

Revise AQA A-level Physics (7408) specification point 3.11.2.2, Non-flow processes (A-level only), with free active-recall flashcards. Flip through the set or review every question and answer below.

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Cards in this set (17)

For a closed system, what is the first-law equation when QQ is energy transferred to the system by heating and WW is work done by the system?

Q=ΔU+WQ = \Delta U + W, where ΔU\Delta U is the change in internal energy.

Under the convention that WW is work done by a system, what sign does WW have for work done on the system?

Negative.

In non-flow processes, how does the conservation of energy compare with the amounts transferred as heating and work?

Energy is conserved, while the amounts transferred as heating and work depend on the process.

What remains constant during an isothermal change?

Temperature.

What equation relates the pressure, volume, amount and absolute temperature of an ideal gas?

pV=nRTpV=nRT, where pp is pressure, VV is volume, nn is amount of gas, RR is the molar gas constant and TT is absolute temperature.

How are pressure and volume related during an isothermal change of a fixed amount of ideal gas?

pV=constantpV=\text{constant}: pressure falls as volume rises, and vice versa.

What determines the internal energy of an ideal gas?

Only its temperature.

What is the change in internal energy of an ideal gas during an isothermal change?

ΔU=0\Delta U=0

During an isothermal change of an ideal gas, how does energy supplied by heating relate to work done by the gas?

They are equal: Q=WQ=W, where WW is the work done by the gas.

What defines an adiabatic change?

There is no energy transfer by heating between the system and its surroundings: Q=0Q=0.

What form does the first law take for an adiabatic change if WW is the work done by the gas?

ΔU=−W\Delta U=-W

How does the temperature of an ideal gas change during adiabatic expansion and compression?

It cools during expansion and warms during compression.

What pressure–volume relationship holds for a reversible adiabatic change of an ideal gas with constant heat capacities?

pVγ=constantpV^{\gamma}=\text{constant}

What is γ\gamma in the reversible adiabatic relationship for an ideal gas?

γ=CpCV\gamma=\frac{C_p}{C_V}, the ratio of the heat capacities at constant pressure and constant volume.

What pressure–temperature relationship follows from the ideal gas law for a fixed amount of gas at constant volume?

p/T=constantp/T = \text{constant}, where TT is measured on the absolute temperature scale.

How much pressure–volume work does a gas do during a constant-volume change?

Zero: W=0W = 0, because the volume does not change.

What does the first law give for heat transfer in a constant-volume change of an ideal gas?

Q=ΔUQ = \Delta U: energy transferred by heating changes the gas’s internal energy.

Non-flow processes (A-level only) Flashcards | AQA A-level Physics (7408) | KnowledgeSet