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In a lecture demonstration, a professor pulls apart two hemispherical steel shells (diameter \(D\) ) with ease using their attached handles. She then places them together, pumps out the air to an absolute pressure of \(p\) , and hands them to a bodybuilder in the back row to pull apart. (a) If atmospheric pressure is \(p_{0}\) , how much force must the bodybuilder exert on each shell? (b) Evaluate your answer for the case \(p=0.025 \mathrm{atm}, D=10.0 \mathrm{cm} .\)

Short Answer

Expert verified
The bodybuilder must exert 388.54 N on each shell.

Step by step solution

01

Understanding the Problem

We need to find the force the bodybuilder must exert to pull the hemispheres apart when the inside pressure is reduced. We know atmospheric pressure outside is \( p_0 \) and pressure inside the hemisphere is \( p \). We'll use these to calculate the force.
02

Calculating Force Exerted by Pressure

The difference in pressure on the inside and outside creates a net force. The force \( F \) is given by the formula: \[ F = (p_0 - p)A \] where \( A \) is the area of the circular surface of one hemisphere. The area \( A \) can be calculated using \( A = \pi r^2 \), where \( r \) is the radius of the hemisphere.
03

Calculating the Radius and Area

Given the diameter \( D = 10.0 \text{ cm} = 0.1 \text{ m} \), the radius \( r = \frac{D}{2} = 0.05 \text{ m} \). The area \( A \) is then: \[ A = \pi (0.05)^2 = 0.00785 \text{ m}^2 \].
04

Substituting Values and Calculating Force

Substitute the area and pressures into the force equation: \[ F = (1.00 \text{ atm} - 0.025 \text{ atm}) \times 0.00785 \text{ m}^2 \]. Convert atm to Pa: \( 1.00 \text{ atm} = 101325 \text{ Pa} \). Thus, \( F = (101325 \text{ Pa} - 0.025 \times 101325 \text{ Pa}) \times 0.00785 \text{ m}^2 \). Simplify: \[ F = 99092.87 \text{ Pa} \times 0.00785 \text{ m}^2 = 777.07 \text{ N} \]. Each hemisphere will experience half of this force, so the bodybuilder must exert \( F = 388.54 \text{ N} \) on each hemisphere.

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Key Concepts

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

Pressure Difference
Pressure difference is a key concept in understanding why the hemispheres stick together when the air inside is pumped out. It refers to the difference between the atmospheric pressure outside the hemispheres and the pressure inside them. When the air is removed, the pressure inside decreases, creating a larger pressure outside than inside. This imbalance is what holds the hemispheres together.

Pressure, in general, is defined as force per unit area. Thus, when there is a pressure difference, a net force is exerted. To calculate this force, we use the formula for pressure difference:
  • Pressure Difference = Atmospheric Pressure - Inside Pressure
This net pressure difference across the hemispheres leads to a force that must be overcome to pull them apart.
Force Calculation
Force calculation involves finding out the exact amount of force the bodybuilder needs to exert to separate the hemispheres. The net force due to pressure difference is what resists the pulling apart of the hemispheres.

To find the force (\( F \)), we use the formula:
  • \[ F = (p_0 - p)A\]
  • Where:
    • \( p_0 \) is the atmospheric pressure,
    • \( p \) is the pressure inside the hemisphere,
    • \( A \) is the area of the circular surface of a hemisphere.
This equation highlights the role of both the pressure difference and the area in determining the force needed.

In practice, you need to understand how to manipulate these variables. For example, if either the area or the pressure difference increases, the force required also increases.
Hemisphere Geometry
Hemisphere geometry helps us determine the area of the surface that is held under pressure, which is crucial for force calculation. The geometrical shape here is a hemisphere, effectively half a sphere.

To calculate the area (\( A \)) of the circle (the base of the hemisphere), we need the radius (\( r \)). The radius is half the diameter (\( D \)):
  • \[ r = \frac{D}{2}\]
The area of the circle can be found using the formula:
  • \[ A = \pi r^2\]
Understanding these geometrical concepts helps in calculating the right area, which in turn is necessary for making correct force calculations. In our example, with a diameter of 10 cm, the radius becomes 5 cm (or 0.05 m), resulting in the calculated area in square meters.
Atmospheric Pressure
Atmospheric pressure is an important concept and is the force exerted by the weight of the air in the atmosphere surrounding us. It accounts for a large portion of the pressure difference seen in this demonstration problem. This pressure is what the outside air exerts on everything at the Earth's surface, including these hemispheres.

Usually measured in atmospheres (atm) or Pascals (Pa), standard atmospheric pressure is approximately 1 atm or 101325 Pa. In problems like this, atmospheric pressure serves as the baseline against which any changes are measured. For instance, if the air inside an object is less than outside (as by pumping some out), the outside, higher atmospheric pressure pushes against the object with greater force.

Being familiar with atmospheric pressure concepts helps in understanding why decreasing inside pressure leads to a requirement of exerting force to counteract the grip created by the higher outside atmospheric pressure.

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Most popular questions from this chapter

(a) Calculate the difference in blood pressure between the feet and top of the head for a person who is 1.65 \(\mathrm{m}\) tall. (b) Consider a cylindrical segment of a blood vessel 2.00 \(\mathrm{cm}\) long and 1.50 \(\mathrm{mm}\) in diameter. What additional outward force would such a vessel need to withstand in the person's feet compared to a similar vessel in her head?

A sealed tank containing seawater to a height of 11.0 \(\mathrm{m}\) also contains air above the water at a gauge pressure of 3.00 atm. Water flows out from the bottom through a small hole. How fast is this water moving?

A liquid flowing from a vertical pipe has a definite shape as it flows from the pipe. To get the equation for this shape, assume that the liquid is in free fall once it leaves the pipe. Just as it leaves the pipe, the liquid has speed \(v_{0}\) and the radius of the stream of liquid is \(r_{0 .}\) (a) Find an equation for the speed of the liquid as a function of the distance \(y\) it has fallen. Combining this with the equation of continuity, find an expression for the radius of the stream as a function of \(y\) . (b) If water flows out of a vertical pipe at a speed of 1.20 \(\mathrm{m} / \mathrm{s}\) , how far below the outlet will the radius be one-half the original radius of the stream?

SHM of a Floating Object. An object with height \(h\) , mass \(M,\) and a uniform cross-sectional area \(A\) floats upright in a liquid with density \(\rho\) . (a) Calculate the vertical distance from the surface of the liquid to the bottom of the floating object at equilibrium. (b) A downward force with magnitude \(F\) is applied to the top of the object. At the new equilibrium position, how much farther below the surface of the liquid is the bottom of the object than it was in part (a)? (Assume that some of the object remains above the surface of the liquid.) (c) Your result in part (b) shows that if the force is suddenly removed, the object will oscillate up and down in SHM. Calculate the period of this motion in terms of the density \(\rho\) of the liquid, the mass \(M,\) and cross-sectional area \(A\) of the object. You can ignore the damping due to fluid friction (see Section \(13.7 ) .\)

A golf course sprinkler system discharges water from a horizontal pipe at the rate of 7200 \(\mathrm{cm}^{3} / \mathrm{s}\) . At one point in the pipe, where the radius is 4.00 \(\mathrm{cm}\) , the water's absolute pressure is \(2.40 \times 10^{5} \mathrm{Pa}\) . At a second point in the pipe, the water passes through a constriction where the radius is \(2.00 \mathrm{cm} .\) What is the water's absolute pressure as it flows through this constriction?

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