Abstract
Dry air is a mixture of gases (chiefly oxygen and nitrogen) having different boiling points. There is no single vapor-pressure curve, as in the case of a pure substance. Instead, the liquid-vapor equilibrium is represented by a bubble-point curve and a dew-point curve. The bubble-point pressure of a liquid mixture is that pressure at which, for a given temperature, vapor just begins to appear. When this pressure is plotted against temperature for a liquid mixture of constant composition, the curve obtained is called the bubble-point curve. The dew-point pressure of a gaseous mixture is that pressure at which, for a given temperature, liquid just begins to appear. When this pressure is plotted against temperature for a gaseous mixture of constant composition, the curve obtained is called the dew-point curve.
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References
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© 1966 Springer Science+Business Media New York
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Walker, G., Christian, W.J., Budenholzer, R.A. (1966). The Vapor Pressure of Dry Air at Low Temperatures. In: Timmerhaus, K.D. (eds) Advances in Cryogenic Engineering. Advances in Cryogenic Engineering, vol 11. Springer, Boston, MA. https://doi.org/10.1007/978-1-4757-0522-5_41
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DOI: https://doi.org/10.1007/978-1-4757-0522-5_41
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