Reference data and engineering information about thermodynamic terms for miscellaneous applications.
Engineering reference data for Thermodynamic Terms in miscellaneous.
y=x⋅k
Multiply by conversion factor.
y=y1+x2−x1(x−x1)(y2−y1)
Estimate between two known points.
p=wholepart×100%
Part as fraction of whole.
| Symbol |
Description |
Unit |
| x |
Input value |
— |
| y |
Output value |
— |
| k |
Conversion factor |
— |
- Chemical Energy: Related to molecular relationships in compounds. Releases heat in exothermic reactions; absorbs heat in endothermic reactions.
- Electric Energy: Associated with electron flow through a conductor.
- Kinetic Energy: Energy of motion, proportional to mass and the square of velocity.
- Nuclear Energy: Energy from atomic relationships, released in fission or fusion.
- Potential Energy: Energy of position or location within a force field.
- Internal Energy: Activity within molecular structure, typically measured by temperature.
- Enthalpy: Energy unit combining internal energy with pressure-volume or flow work.
- Entropy: Measure of disorder or randomization; always produced in natural processes.
- Temperature: Quantifies the warm/cold level of internal energy in a substance.
- Heat: Energy in transit due to temperature difference.
- Work: Energy transfer equivalent to moving a mass against a force.
- Property: A measurable characteristic (e.g., temperature, density, pressure).
- Isobaric heat capacity: C_p = \left(\\frac{\\partial H}{\\partial T}\\right)_p
- Isochoric heat capacity: C_V = \left(\\frac{\\partial U}{\\partial T}\\right)_V
- Relation: Cp−CV=fracTα2VκT
- Isobaric expansivity: αV=frac1Vleft(fracpartialVpartialTright)p
- Isothermal compressibility: κT=−frac1Vleft(fracpartialVpartialpright)T
- Isentropic compressibility: κS=−frac1Vleft(fracpartialVpartialpright)S
- Relation: κT−κS=fracTαV2VCp
- Joule-Thomson coefficient: μJT=left(fracpartialTpartialpright)H=−frac1Cpleft[V−left(fracpartialVpartialTright)pright]
- Φ function: ΦJT=left(fracpartialHpartialpright)T=V−Tleft(fracpartialVpartialTright)p
left(fracpartialSpartialpright)T=−left(fracpartialVpartialTright)p
left(fracpartialSpartialVright)T=left(fracpartialppartialTright)V
For a perfect gas (denoted by superscript ig):
pV=left(suminiright)RT
μiig=μiθ+RTlnleft(fracxippθright)