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UNIT TWO Fluids and Heat

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1 UNIT TWO Fluids and Heat
Understanding the behavior of fluids and thermodynamics is crucial to understanding engines and energy utilization.

2 Chapter 9 The Behavior of Fluids
Lecture PowerPoint Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.

3 floating objects and moving fluids
Pressure explains... floating objects and moving fluids

4 Pressure and Pascal’s Principle
Why does a small woman wearing high-heel shoes sink into soft ground more than a large man wearing large shoes?

5 Pressure The man weighs more, so he exerts a larger force on the ground. The woman weighs less, but the force she exerts on the ground is spread over a much smaller area. Pressure takes into account both force and the area over which the force is applied. Pressure is the ratio of the force to the area over which it is applied: Units: 1 N/m2 = 1 Pa (pascal) Pressure is the quantity that determines whether the soil will yield.

6 Pascal’s Principle What happens inside a fluid when pressure is exerted on it? Does pressure have a direction? Does it transmit a force to the walls or bottom of a container?

7 Pascal’s Principle Fluid pushes outward uniformly in all directions when compressed. Any increase in pressure is transmitted uniformly throughout the fluid. Pressure exerted on a piston extends uniformly throughout the fluid, causing it to push outward with equal force per unit area on the walls and the bottom of the cylinder. This is the basis of Pascal’s Principle: Any change in the pressure of a fluid is transmitted uniformly in all directions throughout the fluid.

8 How does a hydraulic jack work?
A force applied to a piston with a small area can produce a large increase in pressure in the fluid because of the small area of the piston. This increase in pressure is transmitted through the fluid to the piston with the larger area. The force exerted on the larger piston is proportional to the area of the piston: F = PA. Applying the same pressure to the larger area of the second piston results in a larger force on the second piston.

9 A force of 10 N is applied to a circular piston with an area of 2 cm2 in a hydraulic jack. The output piston for the jack has an area of 100 cm2. What is the pressure in the fluid? F1 = 10 N A1 = 2 cm2 = m2 P = F1 / A1 = 10 N / m2 = 50,000 N/m2 = 50 kPa 0.002 Pa 5 Pa 10 Pa 50 kPa

10 What is the force exerted on the output piston by the fluid?
P = 50 kPa A2 = 100 cm2 = 0.01 m2 F1 = PA1 = (50,000 N/m2)(0.01 m2) = 500 N Side note: The mechanical advantage for this machine is 500 N / 10 N = 50. 50 N 500 N 5,000 N 50,000 N

11 Atmospheric Pressure and the Behavior of Gases
Living on the surface of the earth, we are at the bottom of a sea of air. This sea of air is thinner at higher altitudes. It is also thinner during certain weather conditions. We describe this property by atmospheric pressure: the pressure of the layer of air that surrounds the earth. At sea level, the atmospheric pressure is 100 kPa, or 14.7 pounds per square inch, but it decreases with altitude.

12 Mercury worked well because it is much denser than water.
Torricelli invented the barometer, a device for measuring atmospheric pressure, in an attempt to explain why water pumps could pump water to a height of only 32 feet. He filled a tube with mercury and inverted it into an open container of mercury. Mercury worked well because it is much denser than water. Density is the mass of an object divided by its volume. Air pressure acting on the mercury in the dish supported a column of mercury, of height proportional to the atmospheric pressure.

13 Otto von Guericke performed a famous experiment to demonstrate the effects of air pressure.
He designed two bronze hemispheres that could be smoothly joined together at their rims. He pumped the air out of the sphere formed from the two hemispheres. Two eight-horse teams were unable to pull the hemispheres apart.

14 In other experiments on variations in atmospheric pressure, Pascal sent his brother-in-law to the top of a mountain with a barometer and a partially inflated balloon. The balloon expanded as the climbers gained elevation. This was evidence of a decrease in the external atmospheric pressure.

15 Boyle’s Law Variations in the volume and density of a gas that accompanies changes in pressure were studied by Boyle and Mariotte. The density of a column of air decreases as altitude increases because air expands as pressure decreases.

16 Boyle’s Law Boyle discovered that the volume of a gas is inversely proportional to the pressure. Boyle’s Law: PV = constant If the pressure increases, the volume decreases. The density of a column of air decreases as altitude increases because air expands as pressure decreases. P1V1 = P2V2

17 A fixed quantity of gas is held in a cylinder capped at one end by a movable piston. The pressure of the gas is initially 1 atmosphere (101 kPa) and the volume is initially 0.3 m3. What is the final volume of the gas if the pressure is increased to 3 atmospheres at constant temperature? P1 = 1 atm P2 = 3 atm V1 = 0.3 m3 V2 = ? V2 = P1V1 / P2 = (1 atm)(0.3 m3) / 3 atm = 0.1 m3 0.1 m3 0.3 m3 1 m3 3 m3

18 Archimedes’ Principle
The average density of an object compared to a fluid determines whether the object will sink or float in that liquid. The upward force that pushes objects back toward the surface in liquids is called the buoyant force. Archimedes’ Principle: The buoyant force acting on an object fully or partially submerged in a fluid is equal to the weight of the fluid displaced by the object.

19 The source of the buoyant force is the increase in pressure that occurs with increasing depth in a fluid. Atmospheric pressure is greater near the surface of the earth than at higher altitudes. The pressure near the bottom of a pool is larger than near the surface. The weight of the fluid above contributes to the pressure that we experience. Water emerging from a hole near the bottom of a can filled with water has a larger horizontal velocity than water emerging from a hole near the top.

20 For example, consider a block submerged in water, suspended from a string.
The pressure of the water pushes on the block from all sides. Because the pressure increases with depth, the pressure at the bottom of the block is greater than at the top. There is a larger force (F = PA) pushing up at the bottom than there is pushing down at the top. The difference between these two forces is the buoyant force. The buoyant force is proportional to both the height and the cross-sectional area of the block, and thus to its volume. The volume of the fluid displaced is directly related to the weight of the fluid displaced.

21 What forces act on a floating object?
For the block shown, the weight W is balanced by the string’s tension T and the buoyant force. If there are no strings attached or other forces pushing or pulling on the object, only the weight of the object and the buoyant force determine what happens. The weight is proportional to the density and volume of the object, and the buoyant force depends on the density of the fluid and the volume of the fluid displaced by the object. What happens if the density of the object is: greater than that of the fluid? less than that of the fluid? the same as that of the fluid?

22 Fluids in Motion The flow of a fluid is affected by many factors, including the viscosity of the fluid, a measure of the frictional effects within the fluid. The larger the viscosity, the larger the frictional forces between different layers of the fluid. Molasses has a larger viscosity than water. Size also has an effect; for example, a stream’s current is faster where the stream is narrow. Rate of flow, for example of water through a stream or pipe, is volume divided by time. Gallons per minute; liters per second; cubic meters per second.

23 Fluids in Motion The volume of a portion of water of length L flowing past some point in a pipe is the product of the length times the cross-sectional area A, or LA. The rate at which water moves through the pipe is this volume divided by time: LA / t. Since L / t = v, the rate of flow = vA.

24 If the flow is continuous, the rate of flow must be the same at any point along the pipe.
If the cross-sectional area A decreases, the speed v must increase to maintain the same rate of flow.

25 The speed will also usually be greatest near the middle of the stream or pipe.
The fluid can be imagined as flowing in layers. Because of frictional or viscous forces, a thin layer that does not move is usually next to the walls of the pipe or trough. The fluid speed increases as the distance from the wall increases. Each layer moves more slowly than the one above.

26 For a fluid with low viscosity, the transition to the maximum speed occurs over a short distance from the wall. For a fluid with high viscosity, the transition takes place over a larger distance, and the speed may vary throughout the pipe or trough.

27 Laminar flow is smooth flow, with no eddies or other disturbances.
The streamlines are roughly parallel. The speeds of different layers may vary, but one layer moves smoothly past another. Turbulent flow does have eddies and whorls; the streamlines are no longer parallel.

28 Higher speeds are more likely to exhibit turbulent flow.
Turbulent flow increases the fluid’s resistance to flowing through a pipe. Higher speeds are more likely to exhibit turbulent flow. Higher viscosities are less likely to exhibit turbulent flow. Examples: Narrowing of a stream Water from a spigot Smoke rising from a cigarette or candle.

29 Huge example: the famous red spot of Jupiter
Whorls and eddies can be seen in the atmospheric gases. The giant red spot is thought to be a giant and very stable atmospheric eddy.

30 Bernoulli’s Principle
Simple harmonic motion occurs when the energy of a system repeatedly changes from potential energy to kinetic energy and back again. Energy added by doing work to stretch the spring is transformed back and forth between potential energy and kinetic energy.

31 Bernoulli’s Principle
How does a large passenger jet manage to get off the ground? What forces keep it in the air? How is a ball suspended in mid-air by a leaf blower? What happens if we do work on a fluid? Bernoulli’s principle applies conservation of energy to the flow of fluids: The sum of the pressure plus the kinetic energy per unit volume of a flowing fluid must remain constant.

32 How does pressure vary in pipes and hoses?
Will the pressure be greatest in the narrow section or the wide section? The speed will be greater in the narrow section. To keep the sum P + 1/2 dv2 constant, the pressure must be larger where the fluid speed is smaller. If the speed increases, the pressure decreases. (This goes against our intuition.) This can be shown using vertical open pipes as pressure gauges. The height of the column of water is proportional to the pressure.

33 Pressure decreases with increasing speed.
Blowing across the top of a limp piece of paper causes the paper to rise, demonstrating Bernoulli’s principle.

34 How does an airplane wing work?
The shape and tilt of the wing cause the air to move faster across the top than across the bottom. This causes a lower pressure on the top of the wing. The pressure difference produces a net upward force, or lift, acting on the wing. When the lift balances the airplane’s weight, the airplane will fly.

35 How can a ball be suspended in mid-air?
A ball is suspended in an upward-moving column of air produced by a hair dryer. The air pressure is smallest in the center of the column, where the air is moving the fastest.

36 Why does a curveball curve?
The whirlpool of air created by the spin of the ball causes the air to move more rapidly on one side than the other. The difference in pressure produces a force toward the lower-pressure, higher-airspeed side.


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