Deriving the Relationship Between Pressure, Boiling Point, and Height

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SUMMARY

The discussion focuses on deriving the relationship between pressure, boiling point, and height using the equation P(z)=P(0)e^{(-mgz/k_bT)}. The rate of change of the boiling point, T_b, with height, z, is expressed as dT_b/dz=-P(z)mgT_b/(K_bT)(T_b(ρ_L-ρ_G)/(ρ_Lρ_GL_{LG})). Key equations include L_{LG}=T_bΔS and dP/dT=L_{LG}/(T_bΔV). The user attempts to differentiate the pressure expression with respect to temperature and seeks assistance in further simplifying the derived expression for T_b.

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  • Understanding of thermodynamics, specifically the relationship between pressure and temperature.
  • Familiarity with the ideal gas law and its implications on boiling point.
  • Knowledge of latent heat concepts, particularly L_{LG} and its calculation.
  • Proficiency in calculus, particularly differentiation techniques applied to physical equations.
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I'm given an expression for the pressure of air with height z, as

P(z)=P(0)e^{(-mgz/k_bT)}

Where m is the molecular weight of air. It's know that the pressure of water varies with height above sea-level due to the variation of the pressure of the air. The exercise is about to show that the rate of change of the boiling point, Tb, with height, z, is given by the following expression,

\frac{dT_b}{dz}=-\frac{P(z)mg}{K_bT}\frac{dT_b}{dP}=-\frac{P(z)mgT_b}{K_bT}\frac{T_b(\rho_L-\rho_G)}{\rho_L\rho_GL_{LG}}

Where \rho_L is the mass density of water, \rho_G is the mass vapour density and L_{LG} is the latent heat per unit mass.

Relevant equation,

L_{LG}=T_b\Delta S (1)


\frac{dP}{dT}=\frac{L_{LG}}{T_b\Delta V} (2)

My attempt:

I differentiate the given expression for the pressure with respect to the temperature, according to equation (2) to get the following,

\frac{dP}{dT}=\frac{d}{dT}P(z)=\frac{mgz}{k_bT^2}P(z)=\frac{L_{LG}}{T_b\Delta V}

Solving for the boiling point, Tb, gives,


T_b=\frac{L_{LG}k_bT^2}{\Delta V mgzP(z)}

To find the relation which is asked in the exercise, I differentiate Tb with respect to z,

\frac{dT_b}{dz}=\frac{L_{LG}k_bT^2}{\Delta V mg}(-\frac{1}{z^2P(z)}+\frac{mg}{k_bTzP(z)})=\frac{L_{LG}T(mgz-k_BT)}{\Delta V mgz^2P(z)}

Which is basically as far as I'm coming with this expression. I would appreciate help/hints about how to get further with this expression.
 
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