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This is chapter 15, problem number 12.
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We have a diver who is observed in a bubble of air rising from the bottom of the lake, where we have the pressure.
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Let me use the index b to refer to the bottom.
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It's 3 .5 atm atmosphere, right? and the temperature at the bottom is given to us as 4 celsius.
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And the pressure on the surface is one atmosphere.
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And the temperature on the surface is 23 celsius.
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Now we're asked the ratio of the volume on the surface with respect to the bottom in part a.
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So we are asked the surface over the bottom, this ratio.
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So in order to address this question, since we have the pressure and the temperature in the bottom and the pressure and temperature on the surface, and in the meantime, inside the bubble, there is always the same amount of air as it's ascending from the bottom towards the surface of the lake.
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If you write the ideal gas law for these two cases on the bottom at the surface, then we would do pb vb equals nrtb, right? this is for the bottom.
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So let's try to see what remains constant here.
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Like we said, the amount of air is constant inside the bubble, right? so the number of moles is constant, and as you know, the ideal gas constant is constant.
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So if we divide both sides by the temperature at the bottom, we get on the left -hand side of the equation equals to n times r.
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Then if we write the ideal gas law for when the bubble is on the surface of the lake, then it would be p surface, v surface over the temperature at the surface, right? they have to be equal to each other...