claim: “Temperature, like viscosity and density, and of course phone numbers, is not something that can be meaningfully averaged. ‘
evidences.evidence_id: Density:10
evidences.article: Density
evidences.evidence: The density of a material varies with temperature and pressure.
evidences.votes: NOT_ENOUGH_INFO SUPPORTS NOT_ENOUGH_INFO
evidences.evidence_id: Density:79
evidences.article: Density
evidences.evidence: The density of an ideal gas is ρ = M P R T , {\displaystyle \rho ={\frac {MP}{RT}},} where M is the molar mass, P is the pressure, R is the universal gas constant, and T is the absolute temperature.
evidences.votes: NOT_ENOUGH_INFO REFUTES NOT_ENOUGH_INFO
evidences.evidence_id: Population density:0
evidences.article: Population density
evidences.evidence: Population density (in agriculture: standing stock and standing crop) is a measurement of population per unit area, or exceptionally unit volume; it is a quantity of type number density.
evidences.votes: NOT_ENOUGH_INFO REFUTES NOT_ENOUGH_INFO
evidences.evidence_id: Thermodynamic temperature:330
evidences.article: Thermodynamic temperature
evidences.evidence: Averaged across any bulk quantity of a gas, the internal thermal motions of molecules have zero net effect upon the temperature, pressure, or volume of a gas.
evidences.votes: NOT_ENOUGH_INFO SUPPORTS NOT_ENOUGH_INFO
evidences.evidence_id: Viscosity:142
evidences.article: Viscosity
evidences.evidence: An elementary calculation for a dilute gas at temperature T {\displaystyle T} and density ρ {\displaystyle \rho } gives μ = α ρ λ 2 k B T π m , {\displaystyle \mu =\alpha \rho \lambda {\sqrt {\frac {2k_{\text{B}}T}{\pi m}}},} where k B {\displaystyle k_{\text{B}}} is the Boltzmann constant, m {\displaystyle m} the molecular mass, and α {\displaystyle \alpha } a numerical constant on the order of 1 {\displaystyle 1} .
evidences.votes: NOT_ENOUGH_INFO REFUTES NOT_ENOUGH_INFO