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Suppose a distant world with surface gravity of \(7.44 \mathrm{~m} / \mathrm{s}^{2}\) has an atmospheric pressure of \(8.04 \times 10^{4} \mathrm{~Pa}\) at the surface. (a) What force is exerted by the atmosphere on a disk-shaped region \(2.00 \mathrm{~m}\) in radius at the surface of a methane ocean? (b) What is the weight of a \(10.0-\mathrm{m}\) deep cylindrical column of methane with radius \(2.00 \mathrm{~m}\) ? (c) Calculate the pressure at a depth of \(10.0 \mathrm{~m}\) in the methane ocean. Note: The density of liquid methane is \(415 \mathrm{~kg} / \mathrm{m}^{3}\).

Short Answer

Expert verified
The atmospheric force exerted on the disk-shaped region is about \(1.01 \times 10^{6}\) N. The weight of a 10.0-m deep cylindrical column of methane is approximately \(3.87 \times 10^{5}\) N and the pressure at a depth of 10.0 m in the methane ocean is roughly \(1.35 \times 10^{5}\) Pa.

Step by step solution

01

Calculate the Force exerted by the Atmosphere on a Disk-shaped Region

Atmospheric pressure \(P_{a}\) is given by \(8.04 \times 10^{4}\) Pa and radius \(r\) of the disk-shaped region is \(2.00 m\). The area \(A\) of the region is given by \(\pi r^{2}\). Force \(F\) exerted by the atmosphere can be calculated using the formula \(F = P_{a} \times A\). We calculate it to be \(F = 8.04 \times 10^{4} \times \pi \times 2^{2} = 1.01 \times 10^{6}\) N.
02

Calculate the Weight of the Cylindrical Column of Methane

The weight \(W\) of an object is given by \(W = m \times g\). The mass \(m\) is equal to the density \(蟻\) times the volume \(V\). Here, \(蟻 = 415 kg/m^{3}\), the height \(h\) is \(10.0 m\), and \(g = 7.44 m/s^{2}\). The volume of the cylinder is \(V = \pi r^{2} h\). Thus, \(W = \rho \times V \times g = 415 \times \pi \times 2^{2} \times 10.0 \times 7.44 = 3.87 \times 10^{5}\) N.
03

Calculate the Pressure at A Depth of 10.0 m in the Methane Ocean

The pressure \(P\) at a depth \(h\) in a fluid of density \(蟻\) under gravity \(g\) is given by \(P = P_{a} + \rho \times g \times h\). Here, \(P_{a} = 8.04 \times 10^{4}\) Pa, \(蟻 = 415 kg/m^{3}\), \(g = 7.44 m/s^{2}\) and \(h = 10.0 m\). Therefore, \(P = 8.04 \times 10^{4} + 415 \times 7.44 \times 10.0 = 1.35 \times 10^{5}\) Pa.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Surface Gravity
Surface gravity is a measure of the gravitational pull that a planet or celestial body exerts on objects at its surface. It determines how much an object will weigh compared to its weight on Earth. So if you know how much something weighs on Earth, you can calculate its weight on another planet by comparing the respective surface gravities.

On Earth, surface gravity is approximately 9.81 meters per second squared (9.81 \mathrm{~m/s^2}). In this exercise, the distant world has a surface gravity of 7.44 \mathrm{~m/s^2}, which means that an object would weigh less on this planet compared to Earth.

To understand how this affects calculations, especially in physics problems, you need to know that gravitational force is involved in weight calculations. Weight is expressed as the product of mass and surface gravity: \( W = mg \), where \( W \) is the weight, \( m \) is the mass of the object, and \( g \) is the surface gravity.
  • If g is less, as is the case on this distant world, objects weigh less.
  • This directly influences how you calculate pressure and force in physics.
Atmospheric Pressure
Atmospheric pressure is the force exerted by the molecules of the atmosphere on a surface. It's why you can feel wind on your face or why objects can float or sink in a fluid. Atmospheric pressure is typically measured in Pascals (Pa) and varies based on altitude and weather conditions.

In this distant world, the atmospheric pressure at the surface is given as 8.04 \times 10^{4} \mathrm{~Pa}. To comprehend what this means in practical terms, consider that the atmospheric pressure at sea level on Earth is approximately 101,325 \mathrm{~Pa}. Thus, the atmospheric pressure on this distant world is slightly less than that of Earth.
  • To find the force exerted by this pressure over a specific area, use the formula: \( F = P \times A \).
  • The area A for a circular region is calculated with \( \pi r^2 \), where r is the radius of the circle.
  • This knowledge allows you to compute how much force the atmosphere applies on objects, like the disk-shaped region in the exercise.
Density of Liquid Methane
Density is a property that tells us how much mass is contained in a given volume of a substance. It is crucial for understanding buoyancy and pressure within fluids. The density of a substance is given in kilograms per cubic meter (\mathrm{ kg/m^3}) and for liquid methane, it is provided as 415 \mathrm{ kg/m^3}.

Density is significant in fluid mechanics because it affects the pressure exerted at various depths. In our exercise, the pressure at a certain depth within the methane ocean depends on the density of liquid methane. This is encapsulated in the formula:
\( P = P_a + \rho gh \),
  • where \( P_a \) is the atmospheric pressure at the surface, \( \rho \) is the density,
  • \( g \) is the surface gravity, and \( h \) is the depth of the fluid.
This equation illustrates that as you go deeper in a fluid, the pressure increases linearly with depth due to the weight of the fluid above. Understanding how density interacts with surface gravity and depth is vital for accurate pressure calculations in any body of liquid.

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Most popular questions from this chapter

The aorta in humans has a diameter of about \(2.0 \mathrm{~cm}\), and at certain times the blood speed through it is about \(55 \mathrm{~cm} / \mathrm{s}\). Is the blood flow turbulent? The density of whole blood is \(1050 \mathrm{~kg} / \mathrm{m}^{3}\), and its coefficient of viscosity is \(2.7 \times 10^{-3} \mathrm{~N} \cdot \mathrm{s} / \mathrm{m}^{2}\).

The true weight of an object can be measured in a vacuum, where buoyant forces are absent. A measurement in air, however, is disturbed by buoyant forces. An object of volume \(V\) is weighed in air on an equal-arm balance with the use of counterweights of density \(\rho\). Representing the density of air as \(\rho_{\text {air }}\) and the balance reading as \(F_{g}^{\prime}\), show that the true weight \(F_{g}\) is $$ F_{g}=F_{g}^{\prime}+\left(V-\frac{F_{g}^{\prime}}{\rho g}\right) \rho_{\text {air }} g $$

A \(200-\mathrm{kg}\) load is hung on a wire of length \(4.00 \mathrm{~m}\), cross-sectional area \(0.200 \times 10^{-4} \mathrm{~m}^{2}\), and Young's modulus \(8.00 \times 10^{10} \mathrm{~N} / \mathrm{m}^{2}\). What is its increase in length?

Four acrobats of mass \(75.0 \mathrm{~kg}, 68.0 \mathrm{~kg}, 62.0 \mathrm{~kg}\), and \(55.0 \mathrm{~kg}\) form a human tower, with each acrobat standing on the shoulders of another acrobat. The \(75.0-\mathrm{kg}\) acrobat is at the bottom of the tower. (a) What is the normal force acting on the \(75-\mathrm{kg}\) acrobat? (b) If the area of each of the 75.0-kg acrobat's shoes is \(425 \mathrm{~cm}^{2}\), what average pressure (not including atmospheric pressure) does the column of acrobats exert on the floor? (c) Will the pressure be the same if a different acrobat is on the bottom?

A high-speed lifting mechanism supports an \(800-\mathrm{kg}\) object with a steel cable that is \(25.0 \mathrm{~m}\) long and \(4.00 \mathrm{~cm}^{2}\) in cross-sectional area. (a) Determine the elongation of the cable. (b) By what additional amount does the cable increase in length if the object is accelerated upward at a rate of \(3.0 \mathrm{~m} / \mathrm{s}^{2} ?\) (c) What is the greatest mass that can be accelerated upward at \(3.0 \mathrm{~m} / \mathrm{s}^{2}\) if the stress in the cable is not to exceed the elastic limit of the cable, which is \(2.2 \times 10^{8} \mathrm{~Pa}\) ?

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