Related Resources: thermodynamics
Specific Heat Common Gases at Various Temperatures
Thermodynamics Related Resources
Specific heat is the amount of heat needed to raise the temperature of one gram of mass by 1 kelvin. Heat capacity is an extensive property of matter, meaning it is proportional to the size of the system.
Ideal-gas specific heats of various common gases at various temperatures
Temperature, K |
cp kJ/kg · K |
cv kJ/kg · K |
k |
cp kJ/kg · K |
c kJ/kg · K |
k |
cp kJ/kg · K |
cv kJ/kg · K |
k |
||||
Air |
Carbon dioxide, CO2 |
Carbon monoxide, CO |
|||||||||||
250 |
1.003 |
0.716 |
1.401 |
0.791 |
0.602 |
1.314 |
1.039 |
0.743 |
1.400 |
||||
300 |
1.005 |
0.718 |
1.400 |
0.846 |
0.657 |
1.288 |
1.040 |
0.744 |
1.399 |
||||
350 |
1.008 |
0.721 |
1.398 |
0.895 |
0.706 |
1.268 |
1.043 |
0.746 |
1.398 |
||||
400 |
1.013 |
0.726 |
1.395 |
0.939 |
0.750 |
1.252 |
1.047 |
0.751 |
1.395 |
||||
450 |
1.020 |
0.733 |
1.391 |
0.978 |
0.790 |
1.239 |
1.054 |
0.757 |
1.392 |
||||
500 |
1.029 |
0.742 |
1.387 |
1.014 |
0.825 |
1.229 |
1.063 |
0.767 |
1.387 |
||||
550 |
1.040 |
0.753 |
1.381 |
1.046 |
0.857 |
1.220 |
1.075 |
0.778 |
1.382 |
||||
600 |
1.051 |
0.764 |
1.376 |
1.075 |
0.886 |
1.213 |
1.087 |
0.790 |
1.376 |
||||
650 |
1.063 |
0.776 |
1.370 |
1.102 |
0.913 |
1.207 |
1.100 |
0.803 |
1.370 |
||||
700 |
1.075 |
0.788 |
1.364 |
1.126 |
0.937 |
1.202 |
1.113 |
0.816 |
1.364 |
||||
750 |
1.087 |
0.800 |
1.359 |
1.148 |
0.959 |
1.197 |
1.126 |
0.829 |
1.358 |
||||
800 |
1.099 |
0.812 |
1.354 |
1.169 |
0.980 |
1.193 |
1.139 |
0.842 |
1.353 |
||||
900 |
1.121 |
0.834 |
1.344 |
1.204 |
1.015 |
1.186 |
1.163 |
0.866 |
1.343 |
||||
1000 |
1.142 |
0.855 |
1.336 |
1.234 |
1.045 |
1.181 |
1.185 |
0.888 |
1.335 |
||||
Temperature,
K |
Hydrogen, H2 |
Nitrogen, N2 |
Oxygen, O2 |
||||||||||
250 |
14.051 |
9.927 |
1.416 |
1.039 |
0.742 |
1.400 |
0.913 |
0.653 |
1.398 |
||||
300 |
14.307 |
10.183 |
1.405 |
1.039 |
0.743 |
1.400 |
0.918 |
0.658 |
1.395 |
||||
350 |
14.427 |
10.302 |
1.400 |
1.041 |
0.744 |
1.399 |
0.928 |
0.668 |
1.389 |
||||
400 |
14.476 |
10.352 |
1.398 |
1.044 |
0.747 |
1.397 |
0.941 |
0.681 |
1.382 |
||||
450 |
14.501 |
10.377 |
1.398 |
1.049 |
0.752 |
1.395 |
0.956 |
0.696 |
1.373 |
||||
500 |
14.513 |
10.389 |
1.397 |
1.056 |
0.759 |
1.391 |
0.972 |
0.712 |
1.365 |
||||
550 |
14.530 |
10.405 |
1.396 |
1.065 |
0.768 |
1.387 |
0.988 |
0.728 |
1.358 |
||||
600 |
14.546 |
10.422 |
1.396 |
1.075 |
0.778 |
1.382 |
1.003 |
0.743 |
1.350 |
||||
650 |
14.571 |
10.447 |
1.395 |
1.086 |
0.789 |
1.376 |
1.017 |
0.758 |
1.343 |
||||
700 |
14.604 |
10.480 |
1.394 |
1.098 |
0.801 |
1.371 |
1.031 |
0.771 |
1.337 |
||||
750 |
14.645 |
10.521 |
1.392 |
1.110 |
0.813 |
1.365 |
1.043 |
0.783 |
1.332 |
||||
800 |
14.695 |
10.570 |
1.390 |
1.121 |
0.825 |
1.360 |
1.054 |
0.794 |
1.327 |
||||
900 |
14.822 |
10.698 |
1.385 |
1.145 |
0.849 |
1.349 |
1.074 |
0.814 |
1.319 |
||||
1000 |
14.983 |
10.859 |
1.380 |
1.167 |
0.870 |
1.341 |
1.090 |
0.830 |
1.313 |
Source: Kenneth Wark, Thermodynamics, 4th ed. (New York: McGraw-Hill, 1983), p. 783, Table A–4M.