m V DEFINITION OF MASS DENSITY The mass density of a substance is the mass of a substance divided by its volume: SI Unit of Mass Density: kg/m 3


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1 Chapter Fluids
2 . Mass Density DEFINITION OF MASS DENSITY The mass density of a substance is the mass of a substance divided by its volume: m V SI Unit of Mass Density: kg/m 3
3 . Mass Density
4 . Mass Density Example Blood as a Fraction of Body Weight The body of a man whose weight is 690 N contains about 5.x03 m 3 of blood. (a) Find the blood s weight and (b) express it as a percentage of the body weight. m V m 060kg m 5.5 kg
5 . Mass Density (a) W mg 5.5 kg9.80m s 54 N (b) Percentage 54 N 690 N 00% 7.8%
6 . Pressure P F A SI Unit of Pressure: N/m = Pa Pascal
7 . Pressure Example The Force on a Swimmer Suppose the pressure acting on the back of a swimmer s hand is.x0 5 Pa. The surface area of the back of the hand is 8.4x03 m. (a) Determine the magnitude of the force that acts on it. (b) Discuss the direction of the force.
8 . Pressure P F A F PA N m 8.40 m N Since the water pushes perpendicularly against the back of the hand, the force is directed downward in the drawing.
9 . Pressure Atmospheric Pressure at Sea Level:.03x0 5 Pa = atmosphere
10 .3 Pressure and Depth in a Static Fluid F y P A P A mg 0 P A P A mg m V
11 .3 Pressure and Depth in a Static Fluid V Ah P A P A Vg P A P A Ahg P P hg
12 .3 Pressure and Depth in a Static Fluid Conceptual Example 3 The Hoover Dam Lake Mead is the largest wholly artificial reservoir in the United States. The water in the reservoir backs up behind the dam for a considerable distance (0 miles). Suppose that all the water in Lake Mead were removed except a relatively narrow vertical column. Would the Hoover Same still be needed to contain the water, or could a much less massive structure do the job?
13 .3 Pressure and Depth in a Static Fluid Example 4 The Swimming Hole Points A and B are located a distance of 5.50 m beneath the surface of the water. Find the pressure at each of these two locations.
14 .3 Pressure and Depth in a Static Fluid P P gh P atmospheric pressure Pa.000 kg m 9.80m s 5.50 m Pa
15 .4 Pressure Gauges P P gh P atm gh h Patm g 5.00 Pa kg m 9.80m s m 760 mm
16 .4 Pressure Gauges P P B P A P A P gh absolute pressure P Patm gh gaugepressure
17 .4 Pressure Gauges
18 .5 Pascal s Principle PASCAL S PRINCIPLE Any change in the pressure applied to a completely enclosed fluid is transmitted undiminished to all parts of the fluid and enclosing walls.
19 .5 Pascal s Principle P P g 0 m F A F A F F A A
20 .5 Pascal s Principle Example 7 A Car Lift The input piston has a radius of 0.00 m and the output plunger has a radius of 0.50 m. The combined weight of the car and the plunger is 0500 N. Suppose that the input piston has a negligible weight and the bottom surfaces of the piston and plunger are at the same level. What is the required input force?
21 .5 Pascal s Principle F F A A F 0.00 m 0500 N 0.50 m 3 N
22 .6 Archimedes Principle P P gh F B P A P A P P A F B gha V ha F B V g mass of displaced fluid
23 .6 Archimedes Principle ARCHIMEDES PRINCIPLE Any fluid applies a buoyant force to an object that is partially or completely immersed in it; the magnitude of the buoyant force equals the weight of the fluid that the object displaces: F B Magnitudeof buoyant force W fluid Weight of displacedfluid
24 .6 Archimedes Principle If the object is floating then the magnitude of the buoyant force is equal to the magnitude of its weight.
25 .6 Archimedes Principle Example 9 A Swimming Raft The raft is made of solid square pinewood. Determine whether the raft floats in water and if so, how much of the raft is beneath the surface.
26 .6 Archimedes Principle V raft m4.0 m0.30 m 4.8 m F Vg max B water V water g kg m 4.8m 9.80m s N
27 .6 Archimedes Principle W raft m raft g pine V raft g kg m 4.8m 9.80m s 6000 N N The raft floats!
28 .6 Archimedes Principle If the raft is floating: Wraft F B 6000 N water V water g 3 000kg m 4.0 m4.0 m 9.80m s 6000 N h h 6000 N 000 kg m 4.0 m4.0 m9.80m s m
29 .6 Archimedes Principle Conceptual Example 0 How Much Water is Needed to Float a Ship? A ship floating in the ocean is a familiar sight. But is all that water really necessary? Can an ocean vessel float in the amount of water than a swimming pool contains?
30 .6 Archimedes Principle
31 .7 Fluids in Motion In steady flow the velocity of the fluid particles at any point is constant as time passes. Unsteady flow exists whenever the velocity of the fluid particles at a point changes as time passes. Turbulent flow is an extreme kind of unsteady flow in which the velocity of the fluid particles at a point change erratically in both magnitude and direction.
32 .7 Fluids in Motion Fluid flow can be compressible or incompressible. Most liquids are nearly incompressible. Fluid flow can be viscous or nonviscous. An incompressible, nonviscous fluid is called an ideal fluid.
33 .7 Fluids in Motion When the flow is steady, streamlines are often used to represent the trajectories of the fluid particles.
34 .7 Fluids in Motion Making streamlines with dye and smoke.
35 .8 The Equation of Continuity The mass of fluid per second that flows through a tube is called the mass flow rate.
36 .8 The Equation of Continuity m V A vt distance m t Av m t A v
37 .8 The Equation of Continuity EQUATION OF CONTINUITY The mass flow rate has the same value at every position along a tube that has a single entry and a single exit for fluid flow. A v Av SI Unit of Mass Flow Rate: kg/s
38 .8 The Equation of Continuity Incompressible fluid: A v Av Volume flow rate Q: Q Av
39 .8 The Equation of Continuity Example A Garden Hose A garden hose has an unobstructed opening with a cross sectional area of.85x04 m. It fills a bucket with a volume of 8.00x03 m 3 in 30 seconds. Find the speed of the water that leaves the hose through (a) the unobstructed opening and (b) an obstructed opening with half as much area.
40 .8 The Equation of Continuity (a) Q Av v Q A m 30.0 s m 0.936m s (b) A v Av v A 0.936m s.87 m s v A
41 .9 Bernoulli s Equation The fluid accelerates toward the lower pressure regions. According to the pressuredepth relationship, the pressure is lower at higher levels, provided the area of the pipe does not change.
42 .9 Bernoulli s Equation Fs Fs PAs P P V W W nc mv mgy mv mgy
43 .9 Bernoulli s Equation mgy mv mgy mv V P P gy v gy v P P BERNOULLI S EQUATION In steady flow of a nonviscous, incompressible fluid, the pressure, the fluid speed, and the elevation at two points are related by: gy v P gy v P
44 .0 Applications of Bernoulli s Equation Conceptual Example 4 Tarpaulins and Bernoulli s Equation When the truck is stationary, the tarpaulin lies flat, but it bulges outward when the truck is speeding down the highway. Account for this behavior.
45 .0 Applications of Bernoulli s Equation
46 .0 Applications of Bernoulli s Equation
47 .0 Applications of Bernoulli s Equation
48 .0 Applications of Bernoulli s Equation Example 6 Efflux Speed The tank is open to the atmosphere at the top. Find an expression for the speed of the liquid leaving the pipe at the bottom.
49 .0 Applications of Bernoulli s Equation v 0 P P atm P P v gy P v gy y y h v gh v gh
50 . Viscous Flow Flow of an ideal fluid. Flow of a viscous fluid.
51 . Viscous Flow FORCE NEEDED TO MOVE A LAYER OF VISCOUS FLUID WITH CONSTANT VELOCITY The magnitude of the tangential force required to move a fluid layer at a constant speed is given by: F Av y coefficient of viscosity SI Unit of Viscosity: Pa s Common Unit of Viscosity: poise (P) poise (P) = 0. Pa s
52 . Viscous Flow POISEUILLE S LAW 4 R P P The volume flow rate is given by: Q 8 L
53 . Viscous Flow Example 7 Giving and Injection A syringe is filled with a solution whose viscosity is.5x03 Pa s. The internal radius of the needle is 4.0x04 m. The gauge pressure in the vein is 900 Pa. What force must be applied to the plunger, so that.0x06 m 3 of fluid can be injected in 3.0 s?
54 . Viscous Flow P P 8 LQ 4 R Pas 0.05 m.00 m 3.0 s m Pa
55 . Viscous Flow P 900 Pa P P 00 Pa P 300 Pa F P A Pa 8.00 m 0.5N
Fluidi. Copyright 2015 John Wiley & Sons, Inc. All rights reserved.
Fluidi 11.1 Mass Density DEFINITION OF MASS DENSITY The mass density of a substance is the mass of a substance divided by its volume: m V SI Unit of Mass Density: kg/m3 11.1 Mass Density 11.1 Mass Density
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Chapter 11 Fluids 11.1 Mass Density DEFINITION OF MASS DENSITY The mass density of a substance is the mass of a substance divided by its volume: ρ m V SI Unit of Mass Density: kg/m 3 11.1 Mass Density
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