Assumptions:
The default resistivities (η = 1/(89.6e-7*U.Pa*U.s)
and θ = U.m*U.K/(183e-3*U.W)
) are based on data of H2 gas at 1 atm and
300 K from Incropera and DeWitt [Incropera2002, pp. 919–920].
Table 1 lists the properties at other temperatures.
T/U.K |
cp*U.kg*U.K |
η
|
θ*U.W |
---|---|---|---|
100 | 11.23e3 | 1/42.1e-7 | 1/67.0e-3 |
150 | 12.60e3 | 1/56.0e-7 | 1/101e-3 |
200 | 13.54e3 | 1/68.1e-7 | 1/131e-3 |
250 | 14.06e3 | 1/78.9e-7 | 1/157e-3 |
300 | 14.31e3 | 1/89.6e-7 | 1/183e-3 |
350 | 14.43e3 | 1/98.8e-7 | 1/204e-3 |
400 | 14.48e3 | 1/108.2e-7 | 1/226e-3 |
450 | 14.50e3 | 1/117.2e-7 | 1/247e-3 |
500 | 14.52e3 | 1/126.4e-7 | 1/266e-3 |
550 | 14.53e3 | 1/134.3e-7 | 1/285e-3 |
600 | 14.55e3 | 1/142.4e-7 | 1/305e-3 |
700 | 14.61e3 | 1/157.8e-7 | 1/342e-3 |
800 | 14.70e3 | 1/172.4e-7 | 1/378e-3 |
900 | 14.83e3 | 1/186.5e-7 | 1/412e-3 |
1000 | 14.99e3 | 1/201.3e-7 | 1/448e-3 |
1100 | 15.17e3 | 1/213.0e-7 | 1/488e-3 |
1200 | 15.37e3 | 1/226.2e-7 | 1/528e-3 |
1300 | 15.59e3 | 1/238.5e-7 | 1/568e-3 |
1400 | 15.81e3 | 1/250.7e-7 | 1/610e-3 |
1500 | 16.02e3 | 1/262.7e-7 | 1/655e-3 |
1600 | 16.28e3 | 1/273.7e-7 | 1/697e-3 |
1700 | 16.58e3 | 1/284.9e-7 | 1/742e-3 |
1800 | 16.96e3 | 1/296.1e-7 | 1/786e-3 |
1900 | 17.49e3 | 1/307.2e-7 | 1/835e-3 |
2000 | 18.25e3 | 1/318.2e-7 | 1/878e-3 |
The specific heat capacity is not fixed because it would affect the chemical potential and result in an incorrect cell potential.
For more information, please see the Species model.