| 11. | Therefore, one can define a quantity, called "'fugacity "', so that the chemical potential for a real gas becomes
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| 12. | At high pressures, the volume of a real gas is often considerably greater than that of an ideal gas.
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| 13. | These equations are exact only for an ideal gas, which neglects various intermolecular effects ( see real gas ).
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| 14. | A solvent at its theta temperature is, in this way, analogous to a real gas at its Boyle temperature.
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| 15. | At low temperatures, the pressure of a real gas is often considerably less than that of an ideal gas.
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| 16. | With that in mind, the following table explains when the Joule Thomson effect cools or warms a real gas:
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| 17. | The introduction of real gas effects means that more variables are required to describe the full state of a gas.
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| 18. | It is desirable that the expression for a real gas's chemical potential to be similar to the one for an ideal gas.
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| 19. | For a real gas, the isentropic chain is unusable and a " Mollier diagram " would be used instead for manual calculation.
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| 20. | The contribution of nonideality to the chemical potential of a real gas is equal to " RT " ln " ? ".
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