A-LEVEL PHYSICS: 11.2.3: Thermodynamic Processes (SaveMyExams) Flashcards
(20 cards)
the 4 main thermodynamic processes are:
-isovolumetric (W=0)
-isobaric (∆p=0)
-isothermal (∆T=0)
-adiabatic (∆Q=0)
isobaric process:
a process in which no change in pressure occurs
(constant pressure)
constant pressure process:
isobaric process
when do isobaric processes occur?
when gases expand or contract at constant pressure during a change in temperature (Δp=0)
when there is a change in volume at a constant pressure, work done = …
W=p∆V
first law of thermodynamics:
∆U=Q-W
isovolumetric process:
a process where no change in volume occurs and the system does no work
(constant volume ∆V=0 ∴ W=0)
process where no change in volume occurs and the system does no work:
isovolumetric
a process in which no change in pressure occurs (constant pressure):
isobaric
if there is no change in volume, then there is no ___ ___ on or by the ___, so…
work done, gas, W=0
first law of thermodynamics in isobaric process:
∆U= Q ± (p∆V)
(W=p∆V)
(± whether work has been done on or by the gas as a result of ∆V) (expansion = +∆V) (compression = -∆V)
first law of thermodynamics in isovolumetric process:
∆U = Q
(bc W=0 in isovolumetric processes)
isothermal process:
a process in which no change in temperature occurs (constant temperature)
a process in which no change in temperature occurs (constant temperature):
isothermal
first law of thermodynamics in isothermal process:
Q=W
(if the temperature does not change, then the internal energy of the gas will not change ∴ ∆U=0)
adiabatic process:
a process where no heat is transferred into or out of the system (Q=0)
a process where no heat is transferred into or out of the system (Q=0)
adiabatic
first law of thermodynamics in adiabatic process:
∆U = -W
(bc Q=0)
state and explain first law of thermodynamics in adiabatic process: (3)
∆U = -W
-because Q=0 (no heat is transferred into or out of the system)
-this means that all the work done is at the expense of the system’s internal energy
- ∴ an adiabatic process will usually be accompanied by a change in temperature (due to ∆U)
adiabatic processes in ideal gases can be modelled by the equation:
pV ^γ = constant