Resources on physics related to aerodynamics
The List of elementary physics formulae on wikipedia is useful.
List of variables
Variable
|
Meaning
|
Unit (SI)
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γ (gamma)
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Surface tension or Heat capacity ratio (adiabatic process in thermodynamics)
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N.m-1 (Newton per meter)
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μ (mu) or η (eta)
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Viscosity
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Pa·s (Pascal second) or P (Poise, 1 Poise is 0.1 Pa.s)
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C, Cp, CV
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Heat capacity, general, at constant pressure, at constant volume.
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J.K-1 (Joule per Kelvin)
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G
|
Gibbs free energy
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J (Joule)
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H
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Enthalpy: total energy of a thermodynamic system.
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J (Joule)
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ΔHvap or L
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Vaporization heat or Latent heat of vaporization: energy required to vaporize a mole of liquid at a given temperature.
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J.mol-1 (Joule per mole)
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M
|
Mach number
|
no unit
|
Q
|
Amount of Heat
|
J (Joule)
|
T
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Temperature. T0 or Tt is the stagnation temperature.
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K (Kelvin)
|
S
|
Entropy
|
J.K-1 (Joule per Kelvin)
|
U
|
Internal energy of a system (see first law of Thermodynamics below)
|
J (Joule)
|
V
|
Volume
|
m3 (cubic meter)
|
W
|
Work: mechanical constraints on the system.
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J (Joule)
|
a
|
Speed of sound in medium (used to calculate Mach number)
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m.s-1
|
c
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Velocity of a flow in thermodynamics, also noted V; generally noted u in fluid dynamics.
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m.s-1
|
n
|
Quantity of matter
|
mol (mole)
|
p
|
Pressure. pt is the stagnation pressure.
|
Pa (Pascal)
|
List of constants
List of equations
Equation
|
Name
|
Meaning
|
|
Ideal gas equation
|
Relation between properties of an ideal gas (state equation). k is kB.
|
|
Clausius-Clapeyron relation
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Relation between the pressure, latent heat of vaporization and temperature of a vapour at two temperatures (approximation, at low temperatures).
|
|
Heat at state change for an ideal gas.
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The heat required to change the state of a some matter, L being the latent heat. Delta H equals Q only when pressure is constant (isobaric).
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First law of thermodynamics
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Variations of internal energy of a system between two states is the sum of the received heat and work (minus the given work).
|
|
Enthalpy
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Total amount of energy of a system, defined as the sum of the internal energy U of the system and pressure * volume at the boundary of the system and its environment.
|
|
Work of gas expansion.
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Work done by expanding an ideal gas.
|
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Entropy
|
Internal energy related to entropy variation for a closed system in thermal equilibrium (fundamental thermodynamic relation).
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ΔSuniverse = ΔSsurroundings + ΔSsystem
|
Entropy variation as a whole.
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Entropy variation of a system is generally compensated by the inverse variation of the surroundings, not including losses.
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Second law of thermodynamics
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A change in the entropy of a system is the infinitesimal transfer of heat to a closed system driving a reversible process, divided by the equilibrium temperature of the system.
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Gibbs free energy / Free enthalpy
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Useful work obtainable from a system at isobaric and isothermal conditions. Since H is U + pV, it can be replaced in the equation, making G = H - TS.
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Gibbs free energy variation.
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If ΔG < 0, the system's transformation can be spontaneous, if ΔG = 0 the transformation is inversible and the system is in an equilibrium state, if ΔG > 0 it can't be spontaneous.
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