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In thermodynamics, the fugacity of a real gas is an effective partial pressure which replaces the ideal partial pressure in an accurate computation of chemical equilibrium. It is equal to the pressure of an ideal gas which has the same temperature and molar Gibbs free energy (chemical potential) as the real gas.
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pressure gas displaystyle chemical ideal ln equal frac rt potential temperature real mathrm equilibrium molar pressures state law vapor gases
| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| a Van der Waals gas that are closer to reality than an ideal gas | instance of | as the real gas.Fugacities are determined experimentally or estimated from various models | 0.80 | text |
| Fugacity | measured by | The | 0.60 | section |
| Fugacity | measured by | In | 0.60 | section |
| Fugacity | measured by | RT | 0.60 | section |
| Fugacity | measured by | This | 0.60 | section |
| Fugacity | measured by | Then | 0.60 | section |
| Fugacity | measured by | Z-1 | 0.60 | section |
| Fugacity | measured by | If | 0.60 | section |
| Fugacity | measured by | Pc | 0.60 | section |
| Fugacity | measured by | Tc | 0.60 | section |
| Fugacity | measured by | Pr | 0.60 | section |
| Fugacity | measured by | P/Pc | 0.60 | section |
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