Calculating Air density as a function of height?

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Air density can be calculated as a function of height using the relationship between pressure and density. The equation p(h) = p₀e^{-gh/RT} describes how air pressure decreases with height, where p₀ is the sea level pressure, T is the temperature, and R is the gas constant. The pressure of the atmosphere reflects the weight of the air above, and as altitude increases, the weight—and thus pressure—decreases. It is suggested that density can be assumed proportional to pressure, allowing for the derivation of air density from pressure changes with height. Understanding these relationships is crucial for accurate calculations of air density at varying altitudes.
Noone1982
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Is it possible to calculate the air density as a function of height? We know that density is given as,

p\; =\; \frac{M}{V}

And that pressure is given as,

P\mbox{re}ssu\mbox{re}\; =\; pgh

But I am failing to see the connection to combine the two to get air density as a function of height. Any insight?
 
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It's a miracle that I remember this from my hydrology course (the most boring one): p(h) = p_{0}e^{-\frac{gh}{RT}}. This is the expression for air pressure at a height h. p_{0} is the air pressure at the sea level, T is the average temperature at the height h, and R is a gas constant for dry air.
 
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Noone1982 said:
Is it possible to calculate the air density as a function of height? We know that density is given as,

p\; =\; \frac{M}{V}

And that pressure is given as,

P\mbox{re}ssu\mbox{re}\; =\; pgh

But I am failing to see the connection to combine the two to get air density as a function of height. Any insight?
The pressure of the atmosphere is the weight of the air above per unit area. If you move up slightly, the weight decreases by an amount that depends on the density and change in height. You can assume the density is proportional to the pressure. Your equation

P\mbox{re}ssu\mbox{re}\; =\; \rho gh

is the change in pressure for a small change in height for which the density may be assumed constant.
 
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The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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