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Ch 12: Fluid Mechanics

Chapter 12, Problem 12

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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Everyone today, we are going to determine the gauge pressure at the bottom of the ocean of the newly discovered planet and determine the depth of the earth's ocean, where a gauge pressure will record similar values. So we know or it is given in our problem statement that the newly discovered planet has a 1.2 kilometer deep ocean. So I'm just gonna write it down as a church are H is going to be 1.2 kilometer or essentially 1.2 times 10 to the power of three m. And it is also given that the gravitational acceleration is going to be 5.20 m per second squared. Okay, so recall that to calculate for this pressure or pressure under a surface level, we're gonna need this formula right here, which is pressure equals the atmospheric pressure plus H. Rho G. And we can actually calculate the gauge pressure which is essentially just going to be the pressure difference delta P. Which is equals to p minus P A T. M. This p right here, we can actually substituted from this formula. So P is going to be P A T. M plus H rho g minus B A T M. So we can cancel out the P A. T. M. And the gauge pressure is just going to be a church row and G. Awesome. Okay, so let's start solving the first part which is determining the gauge pressure at the bottom of the newly discovered planets ocean. So the gauge pressure as I said previously is the pressure difference. So delta P equals H rho G And the density of the freshwater row of freshwater. Because we assume that the ocean is filled with fresh water is 1000 kilograms per meter cube. So the age is going to be 1.2 times 10 to the power of three m. The row is going to be this which is 1000 kg per meter cube. And the G is going to be the new gravitational acceleration. Don't forget which is the 5.2 m per second squared. Okay, and this will actually give us a gauge pressure of 6.24 times 10 to the power of six pascal's. Remember that all of this unit combined will be considered a pascal. Okay, so that will be our first part and the second part is if we have this gauge pressure here. So Delta P. If delta P 6.24 times 10 to the power of six pascal, what is going to be the depth of the Earth's ocean that will record similar values? So delta piece H. Road G. So what will be the H value that will give us this delta P. So H will then be 6.24 times 10 to the power of six pascal's. We know that the row of seawater is 10 30 kg per meter cube. So I'm just gonna write it down. So H is going to be 6.24 times 10 to the power of six pascal divided by rho divided by G. So H is going to be 6.24 times 10 to the power of six pascal's divided by 30 kg per meter cube. Multiplied by this is going to be the gravitational acceleration of earth, so 9.8 m per second squared. And this will give us a value of 618 m just like so okay, so we know that the gauge pressure is going to be 6. times down to the part of six pascal's and we know that the age is going to be 6 18 m, which is going to correspond to option A just like so. Okay, and that would be all for this particular problem. Let me know if you guys have any questions or please continue and watch other videos on this similar lessons because there are a lot of other videos that will explain and give you guys a better understanding on this. Thank you.
Related Practice
Textbook Question
You are designing a diving bell to withstand the pressure of seawater at a depth of 250 m. (a) What is the gauge pressure at this depth? (You can ignore changes in the density of the water with depth.) (b) At this depth, what is the net force due to the water outside and the air inside the bell on a circular glass window 30.0 cm in diameter if the pressure inside the diving bell equals the pressure at the surface of the water? (Ignore the small variation of pressure over the surface of the window.)
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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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Textbook Question
BIO. Ear Damage from Diving. If the force on the tympanic membrane (eardrum) increases by about 1.5 N above the force from atmospheric pressure, the membrane can be damaged. When you go scuba diving in the ocean, below what depth could damage to your eardrum start to occur? The eardrum is typically 8.2 mm in diameter. (Consult Table 12.1.)
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Textbook Question
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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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
Exploring Venus. The surface pressure on Venus is 92 atm, and the acceleration due to gravity there is 0.894g. In a future exploratory mission, an upright cylindrical tank of benzene is sealed at the top but still pressurized at 92 atm just above the benzene. The tank has a diameter of 1.72 m, and the benzene column is 11.50 m tall. Ignore any effects due to the very high temperature on Venus. (b) What force does the Venusian atmosphere exert on the outside surface of the bottom of the tank?
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