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''' | ! colspan="7" align="center" style="background:#cccccc;"| Specific heat ratio of various gases | ||
|- | |||
| bgcolor="#E0E0E0" align="center" | Gas | |||
| bgcolor="#E0E0E0" align="center" | °C | |||
| bgcolor="#E0E0E0" align="center" | '''''k''''' | |||
| bgcolor="#E0E0E0" width="2" rowspan="17"| | |||
| bgcolor="#E0E0E0" align="center" | Gas | |||
| bgcolor="#E0E0E0" align="center" | °C | |||
| bgcolor="#E0E0E0" align="center" | '''''k''''' | |||
|- | |||
| rowspan="7" align="center" | H<sub>2</sub> | |||
| align="center" |−181 | |||
| 1.597 | |||
| rowspan="4" align="center" | Dry<BR>Air | |||
| align="center" |20 | |||
| 1.40 | |||
|- | |||
| align="center" |−76 | |||
| 1.453 | |||
| align="center" |100 | |||
| 1.401 | |||
|- | |||
| align="center" |20 | |||
| 1.41 | |||
| align="center" |200 | |||
| 1.398 | |||
|- | |||
| align="center" |100 | |||
| 1.404 | |||
| align="center" |400 | |||
| 1.393 | |||
|- | |||
| align="center" |400 | |||
| 1.387 | |||
| rowspan="4" align="center" | CO<sub>2</sub> | |||
| align="center" |0 | |||
| 1.310 | |||
|- | |||
| align="center" |1000 | |||
| 1.358 | |||
| align="center" |20 | |||
| 1.30 | |||
|- | |||
| align="center" |2000 | |||
| 1.318 | |||
| align="center" |100 | |||
| 1.281 | |||
|- | |||
| align="center" | He | |||
| align="center" |20 | |||
| 1.66 | |||
| align="center" |400 | |||
| 1.235 | |||
|- | |||
|rowspan="2" align="center"|N<sub>2</sub> | |||
| align="center" |−181 | |||
| 1.47 | |||
| align="center" |NH<sub>3</sub> | |||
| align="center" |15 | |||
| 1.310 | |||
|- | |||
| align="center" |15 | |||
| 1.404 | |||
| align="center" | CO | |||
| align="center" |20 | |||
| 1.40 | |||
|- | |||
| align="center"|Cl<sub>2</sub> | |||
| align="center" |20 | |||
| 1.34 | |||
| rowspan="6" align="center" | O<sub>2</sub> | |||
| align="center" |−181 | |||
| 1.45 | |||
|- | |||
| rowspan="2" align="center" | Ar | |||
| align="center" |−180 | |||
| 1.76 | |||
| align="center" |−76 | |||
| 1.415 | |||
|- | |||
| align="center" |20 | |||
| 1.67 | |||
| align="center" |20 | |||
| 1.40 | |||
|- | |||
| rowspan="3" align="center" | CH<sub>4</sub> | |||
| align="center" |−115 | |||
| 1.41 | |||
| align="center" |100 | |||
| 1.399 | |||
|- | |||
| align="center" |−74 | |||
| 1.35 | |||
| align="center" |200 | |||
| 1.397 | |||
|- | |||
| align="center" |20 | |||
| 1.32 | |||
| align="center" |400 | |||
| 1.394 | |||
|} | |||
The '''[[specific heat ratio]]''' of a gas is the ratio of the specific heat at constant pressure, <math>C_p</math>, to the specific heat at constant volume, <math>C_v</math>. It is sometimes referred to as the '''adiabatic index''' or the '''heat capacity ratio''' or the '''isentropic expansion factor''' or the '''adiabatic exponent''' or the '''isentropic exponent'''. | |||
Either <math>\kappa</math> (kappa), <math>k</math> (Roman letter k) or <math>\gamma</math> (gamma) may be used to denote the specific heat ratio: | |||
:<math>\kappa = k = \gamma = \frac{C_p}{C_v}</math> | |||
where: | |||
:<math>C</math> = the specific heat of a gas | |||
:<math>p</math> = refers to constant pressure conditions | |||
:<math>v</math> = refers to constant volume conditions | |||
<BR><BR> |
Revision as of 03:31, 3 June 2011
Specific heat ratio of various gases | ||||||
---|---|---|---|---|---|---|
Gas | °C | k | Gas | °C | k | |
H2 | −181 | 1.597 | Dry Air |
20 | 1.40 | |
−76 | 1.453 | 100 | 1.401 | |||
20 | 1.41 | 200 | 1.398 | |||
100 | 1.404 | 400 | 1.393 | |||
400 | 1.387 | CO2 | 0 | 1.310 | ||
1000 | 1.358 | 20 | 1.30 | |||
2000 | 1.318 | 100 | 1.281 | |||
He | 20 | 1.66 | 400 | 1.235 | ||
N2 | −181 | 1.47 | NH3 | 15 | 1.310 | |
15 | 1.404 | CO | 20 | 1.40 | ||
Cl2 | 20 | 1.34 | O2 | −181 | 1.45 | |
Ar | −180 | 1.76 | −76 | 1.415 | ||
20 | 1.67 | 20 | 1.40 | |||
CH4 | −115 | 1.41 | 100 | 1.399 | ||
−74 | 1.35 | 200 | 1.397 | |||
20 | 1.32 | 400 | 1.394 |
The specific heat ratio of a gas is the ratio of the specific heat at constant pressure, , to the specific heat at constant volume, . It is sometimes referred to as the adiabatic index or the heat capacity ratio or the isentropic expansion factor or the adiabatic exponent or the isentropic exponent.
Either (kappa), (Roman letter k) or (gamma) may be used to denote the specific heat ratio:
where:
- = the specific heat of a gas
- = refers to constant pressure conditions
- = refers to constant volume conditions