Chapter 9: Problem 100
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Chapter 9: Problem 100
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Atmospheric pressure is equal to the weight of a vertical column of air, extending all the way up through the atmosphere, divided by the cross- sectional area of the column. (a) Explain why that must be true. [Hint: Apply Newton's second law to the column of air.] (b) If the air all the way up had a uniform density of \(1.29 \mathrm{kg} / \mathrm{m}^{3}\) (the density at sea level at \(0^{\circ} \mathrm{C}\) ), how high would the column of air be? (c) In reality, the density of air decreases with increasing altitude. Does that mean that the height found in (b) is a lower limit or an upper limit on the height of the atmosphere?
Two identical spheres are dropped into two different columns: one column contains a liquid of viscosity \(0.5 \mathrm{Pa} \cdot \mathrm{s},\) while the other contains a liquid of the same density but unknown viscosity. The sedimentation velocity in the second tube is \(20 \%\) higher than the sedimentation velocity in the first tube. What is the viscosity of the second liquid?
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