Title | Formelsamling |
---|---|
Course | Termodynamik |
Institution | Kungliga Tekniska Högskolan |
Pages | 3 |
File Size | 101 KB |
File Type | |
Total Downloads | 62 |
Total Views | 127 |
Formelsamling till kursen termodynamik...
L L0 T
linear thermal expansion
V V0 T
volume thermal expansion
Q mc T
heat required to change temperature of a certain mass
Q nC T
heat required to change temperature of a certain number of moles
Q mL
H
𝐻=
heat transfer in a phase change
dQ T T kA H C dt L 𝐴(𝑇𝐻−𝑇𝐶 ) 𝑅
heat current in conduction
(heat current in conduction)
𝐿
𝑅 = 𝑘 (relationship between thermal resistance and thermal conductivity)
heat current in radiation
H Ae T 4
4 4 Hnet Ae T Ts
(net heat current in radiation)
mtotal nM
total mass, number of moles, and molar mass
pV nRT
ideal-gas equation
(𝑝 +
𝑎 𝑛2 ) (𝑉 𝑉2
− 𝑛 𝑏 ) = 𝑛 𝑅 𝑇 (van der Waals’ equation)
𝑅 = 𝑘 𝑁𝐴 (gas constant, Boltzmann constant, Avogadro’s number)
M NA m 𝐸𝑘𝑖𝑛 =
𝑚 𝑣2 2
molar mass, Avogadro's number, and mass of a molecule 𝑝2
= 2𝑚 (kinetic energy)
𝑝 = 𝑚 𝑣 (momentum)
𝐸𝑝𝑜𝑡 = 𝑚 𝑔 ℎ (potential energy near the earth’s surface) 𝑊 = 𝐹 𝑠 (work)
average translational kinetic energy of an ideal gas
3
Ktr nRT 2
1 2
m 2 av 3 kT
average translational kinetic energy of a gas molecule
2
rms
2
t mean
av
3kT 3RT m M
V 4 2r 2N
root-mean-square speed of a gas molecule
mean free path of a gas molecule
CV 3 R
ideal gas of point particles
CV 5 R
diatomic gas, including rotation
CV 3R
ideal monatomic solid
2
2
3/ 2
2 m f 4 2e m / 2 kT 2 kT
V2
work done in a volume change
W p dV V1
W p V2 V1
U Q W
Maxwell Boltzmann distribution
work done in a volume change at constant pressure
first law of thermodynamics
dU dQ dW
first law of thermodynamics, infinitesimal process
𝑑𝑈 = 𝑛 𝐶𝑉 𝑑𝑇 (change of inner energy and temperature for ideal gas, all processes) Cp CV R
molar heat capacities of an ideal gas
Cp CV
ratio of heat capacities
W nCV T1 T2
W
adiabatic process, ideal gas
1 CV pV pV pV p V 1 1 2 2 1 1 1 2 2 R
adiabatic process, ideal gas
𝑝 𝑉 = 𝑐𝑜𝑛𝑠𝑡𝑎𝑛𝑡 (reversible, adiabatic process) 𝑇 𝑉 −1 = 𝑐𝑜𝑛𝑠𝑡𝑎𝑛𝑡 (reversible, adiabatic process)
e
W Q Q 1 C 1 C QH QH QH
K
QC W
e Carnot 1
KCarnot
S
2
1
QC Q H QC
TC TH TC TH TH
TC TH TC dQ T
S k ln w
thermal efficiency of an engine
coefficient of performance of a refrigerator efficiency of a Carnot engine
coefficient of performance of a Carnot refrigerator
entropy change in a reversible process
microscopic expression for entropy...