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Ch 12: Fluid Mechanics
Chapter 12, Problem 12

A barrel contains a 0.120-m layer of oil floating on water that is 0.250 m deep. The density of the oil is 600 kg/m^3. (a) What is the gauge pressure at the oil–water interface? (b) What is the gauge pressure at the bottom of the barrel?

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1
Identify the densities and depths of the fluids. For oil, the density (\(\rho_{oil}\)) is 600 kg/m^3 and the depth (\(h_{oil}\)) is 0.120 m. For water, the density (\(\rho_{water}\)) is typically 1000 kg/m^3 and the depth (\(h_{water}\)) is 0.250 m.
Calculate the gauge pressure at the oil-water interface using the formula for pressure due to a fluid column, \(P = \rho \cdot g \cdot h\), where \(\rho\) is the density of the fluid, \(g\) is the acceleration due to gravity (approximately 9.81 m/s^2), and \(h\) is the height of the fluid column. Here, use the density and depth of the oil.
To find the gauge pressure at the bottom of the barrel, consider the pressure contributions from both the oil and the water. First, calculate the pressure at the bottom of the oil layer as done in step 2.
Add the pressure due to the water layer to the pressure at the bottom of the oil layer. Use the same pressure formula, but now with the density and depth of the water. The total pressure at the bottom of the barrel is the sum of the pressures due to both the oil and the water.
Remember that gauge pressure is the pressure relative to atmospheric pressure. Since atmospheric pressure acts on the surface of the oil, it does not affect the gauge pressure calculations in this scenario.

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Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Gauge Pressure

Gauge pressure is the pressure relative to atmospheric pressure. It is calculated by subtracting atmospheric pressure from the absolute pressure. In fluid mechanics, gauge pressure is important for understanding how pressure varies within a fluid column due to the weight of the fluid above a given point.
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Hydrostatic Pressure

Hydrostatic pressure is the pressure exerted by a fluid at rest due to the weight of the fluid above it. It is given by the formula P = ρgh, where P is the pressure, ρ is the fluid density, g is the acceleration due to gravity, and h is the height of the fluid column. This concept is crucial for calculating pressures at different depths in a fluid.
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Density and Buoyancy

Density is the mass per unit volume of a substance, and it plays a key role in buoyancy, which is the ability of an object to float in a fluid. The density of the oil and water determines how they interact at the interface, affecting the pressure calculations at different levels within the barrel. Understanding these properties is essential for solving problems involving layered fluids.
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Related Practice
Textbook Question
BIO. There is a maximum depth at which a diver can breathe through a snorkel tube (Fig. E12.17) because as the depth increases, so does the pressure difference, which tends to collapse the diver's lungs. Since the snorkel connects the air in the lungs to the atmosphere at the surface, the pressure inside the lungs is atmospheric pressure. What is the external– internal pressure difference when the diver's lungs are at a depth of 6.1 m (about 20 ft)? Assume that the diver is in fresh-water. (A scuba diver breathing from compressed air tanks can operate at greater depths than can a snorkeler, since the pressure of the air inside the scuba diver's lungs increases to match the external pressure of the water.)

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Oceans on Mars. Scientists have found evidence that Mars may once have had an ocean 0.500 km deep. The acceleration due to gravity on Mars is 3.71 m/s^2. (a) What would be the gauge pressure at the bottom of such an ocean, assuming it was freshwater? (b) To what depth would you need to go in the earth's ocean to experience the same gauge pressure?
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Textbook Question
A closed container is partially filled with water. Initially, the air above the water is at atmospheric pressure (1.01×10^5 Pa) and the gauge pressure at the bottom of the water is 2500 Pa. Then additional air is pumped in, increasing the pressure of the air above the water by 1500 Pa. (a) What is the gauge pressure at the bottom of the water?
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Textbook Question
BIO. The lower end of a long plastic straw is immersed below the surface of the water in a plastic cup. An average person sucking on the upper end of the straw can pull water into the straw to a vertical height of 1.1 m above the surface of the water in the cup. (a) What is the lowest gauge pressure that the average person can achieve inside his lungs? (b) Explain why your answer in part (a) is negative.
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