Chapter 14. Lecture 1 Fluid Mechanics. Dr. Armen Kocharian

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1 Chapter 14 Lecture 1 Fluid Mechanics Dr. Armen Kocharian

2 States of Matter Solid Has a definite volume and shape Liquid Has a definite volume but not a definite shape Gas unconfined Has neither a definite volume nor shape

3 States of Matter, cont All of the previous definitions are somewhat artificial More generally, the time it takes a particular substance to change its shape in response to an external force determines whether the substance is treated as a solid, liquid or gas

4 Fluids A fluid is a collection of molecules that are randomly arranged and held together by weak cohesive forces and by forces exerted by the walls of a container Both liquids and gases are fluids

5 Statics and Dynamics with Fluids Fluid Statics Describes fluids at rest Fluid Dynamics Describes fluids in motion The same physical principles that have applied to statics and dynamics up to this point will also apply to fluids

6 Forces in Fluids Fluids do not sustain shearing stresses or tensile stresses The only stress that can be exerted on an object submerged in a static fluid is one that tends to compress the object from all sides The force exerted by a static fluid on an object is always perpendicular to the surfaces of the object

7 Pressure The pressure P of the fluid at the level to which the device has been submerged is the ratio of the force to the area P F A

8 Pressure, cont Pressure is a scalar quantity Because it is proportional to the magnitude of the force If the pressure varies over an area, evaluate df on a surface of area da as df = P da Unit of pressure is pascal (Pa) 1Pa = 1 N/m 2

9 Pressure vs. Force Pressure is a scalar and force is a vector The direction of the force producing a pressure is perpendicular to the area of interest

10 Measuring Pressure The spring is calibrated by a known force The force due to the fluid presses on the top of the piston and compresses the spring The force the fluid exerts on the piston is then measured

11 Variation of Pressure with Depth Fluids have pressure that varies with depth If a fluid is at rest in a container, all portions of the fluid must be in static equilibrium All points at the same depth must be at the same pressure Otherwise, the fluid would not be in equilibrium

12 Pressure and Depth Examine the darker region, a sample of liquid within a cylinder It has a crosssectional area A Extends from depth d to d + h below the surface Three external forces act on the region

13 Pressure and Depth, cont The liquid has a density of ρ Assume the density is the same throughout the fluid This means it is an incompressible liquid The three forces are: Downward force on the top, P 0 A Upward on the bottom, PA Gravity acting downward, Mg The mass can be found from the density: M = ρv = ρ Ah

14 Pressure and Depth, final Since the net force must be zero: F= PAˆj P ˆ ˆ o Aj Mgj This chooses upward as positive Solving for the pressure gives P = P 0 + ρgh The pressure P at a depth h below a point in the liquid at which the pressure is P 0 is greater by an amount ρgh

15 Density Notes Density is defined as the mass per unit volume of the substance The values of density for a substance vary slightly with temperature since volume is temperature dependent The various densities indicate the average molecular spacing in a gas is much greater than that in a solid or liquid

16 Density Table

17 Atmospheric Pressure If the liquid is open to the atmosphere, and P 0 is the pressure at the surface of the liquid, then P 0 is atmospheric pressure P 0 = 1.00 atm = x 10 5 Pa

18 Pascal s Law The pressure in a fluid depends on depth and on the value of P 0 An increase in pressure at the surface must be transmitted to every other point in the fluid This is the basis of Pascal s law

19 Pascal s Law, cont Named for French scientist Blaise Pascal A change in the pressure applied to a fluid is transmitted undiminished to every point of the fluid and to the walls of the container P1 = P2 F1 F2 = A A 1 2

20 Pascal s Law, Example Diagram of a hydraulic press (right) A large output force can be applied by means of a small input force The volume of liquid pushed down on the left must equal the volume pushed up on the right

21 Pascal s Law, Example cont. Since the volumes are equal, A1 x1 = A2 x2 Combining the equations, F x = F x which means W 1 = W 2 This is a consequence of Conservation of Energy

22 Pascal s Law, Other Applications Hydraulic brakes Car lifts Hydraulic jacks Forklifts

23 Pressure Measurements: Barometer Invented by Torricelli A long closed tube is filled with mercury and inverted in a dish of mercury The closed end is nearly a vacuum Measures atmospheric pressure as P = ρ 0 Hg gh One 1 atm = m (of Hg)

24 Pressure Measurements: Manometer A device for measuring the pressure of a gas contained in a vessel One end of the U-shaped tube is open to the atmosphere The other end is connected to the pressure to be measured Pressure at B is P 0 +ρgh

25 Absolute vs. Gauge Pressure P = P 0 + ρgh P is the absolute pressure The gauge pressure is P P 0 This is also ρgh This is what you measure in your tires

26 Buoyant Force The buoyant force is the upward force exerted by a fluid on any immersed object The parcel is in equilibrium There must be an upward force to balance the downward force

27 Buoyant Force, cont The upward force, B, must equal (in magnitude) the downward gravitational force The upward force is called the buoyant force The buoyant force is the resultant force due to all forces applied by the fluid surrounding the parcel

28 Archimedes s Principle The magnitude of the buoyant force always equals the weight of the fluid displaced by the object This is called Archimedes s Principle Archimedes s Principle does not refer to the makeup of the object experiencing the buoyant force The object s composition is not a factor since the buoyant force is exerted by the fluid

29 Archimedes s Principle, cont The pressure at the top of the cube causes a downward force of P t A The pressure at the bottom of the cube causes an upward force of P b A B = (P b P ) t A = Mg

30 Archimedes's Principle: Totally Submerged Object An object is totally submerged in a fluid of density ρ fluid The upward buoyant force is B = ρ gv = ρ gv fluid fluid obj The downward gravitational force is w = mg = ρobjgvobj The net force is B - F g = ( ρ ρ )gv fluid obj obj

31 Archimedes s Principle: Totally Submerged Object, cont If the density of the object is less than the density of the fluid, the unsupported object accelerates upward If the density of the object is more than the density of the fluid, the unsupported object sinks The motion of an object in a fluid is determined by the densities of the fluid and the object

32 Archimedes s Principle: Floating Object The object is in static equilibrium The upward buoyant force is balanced by the downward force of gravity Volume of the fluid displaced corresponds to the volume of the object beneath the fluid level ρobj Vfluid = V ρ fluid obj

33 Archimedes s Principle: Floating Object, cont The fraction of the volume of a floating object that is below the fluid surface is equal to the ratio of the density of the object to that of the fluid

34 Archimedes s Principle, Crown Example Archimedes was (supposedly) asked, Is the crown made of pure gold? Crown s weight in air = 7.84 N Weight in water (submerged) = 6.84 N Buoyant force will equal the apparent weight loss Difference in scale readings will be the buoyant force

35 Archimedes s Principle, Crown Example, cont. Σ F = B+ T2 F g = 0 B = F g T 2 (Weight in air weight in water) Archimedes s principle says B = ρgv Then to find the material of the crown, ρ crown = m crown in air / V

36 Archimedes s Principle, Iceberg Example What fraction of the iceberg is below water? The iceberg is only partially submerged and so V fluid / V object = ρ / ρ object fluid applies The fraction below the water will be the ratio of the volumes (V water / V ice )

37 Archimedes s Principle, Iceberg Example, cont V ice is the total volume of the iceberg V water is the volume of the water displaced This will be equal to the volume of the iceberg submerged About 89% of the ice is below the water s surface

38 Types of Fluid Flow Laminar Laminar flow Steady flow Each particle of the fluid follows a smooth path The paths of the different particles never cross each other The path taken by the particles is called a streamline

39 Types of Fluid Flow Turbulent An irregular flow characterized by small whirlpool like regions Turbulent flow occurs when the particles go above some critical speed

40 Viscosity Characterizes the degree of internal friction in the fluid This internal friction, viscous force, is associated with the resistance that two adjacent layers of fluid have to moving relative to each other It causes part of the kinetic energy of a fluid to be converted to internal energy

41 Ideal Fluid Flow There are four simplifying assumptions made to the complex flow of fluids to make the analysis easier (1) The fluid is nonviscous internal friction is neglected (2) The flow is steady the velocity of each point remains constant

42 Ideal Fluid Flow, cont (3) The fluid is incompressible the density remains constant (4) The flow is irrotational the fluid has no angular momentum about any point

43 Streamlines The path the particle takes in steady flow is a streamline The velocity of the particle is tangent to the streamline A set of streamlines is called a tube of flow

44 Equation of Continuity Consider a fluid moving through a pipe of nonuniform size (diameter) The particles move along streamlines in steady flow The mass that crosses A 1 in some time interval is the same as the mass that crosses A 2 in that same time interval

45 Equation of Continuity, cont m 1 = m 2 ρa 1 v 1 = ρa 2 v 2 Since the fluid is incompressible, ρ is a constant A 1 v 1 = A 2 v 2 This is called the equation of continuity for fluids The product of the area and the fluid speed at all points along a pipe is constant for an incompressible fluid

46 Equation of Continuity, Implications The speed is high where the tube is constricted (small A) The speed is low where the tube is wide (large A) The product, Av, is called the volume flux or the flow rate Av = constant is equivalent to saying the volume that enters one end of the tube in a given time interval equals the volume leaving the other end in the same time If no leaks are present

47 Bernoulli s Equation As a fluid moves through a region where its speed and/or elevation above the Earth s surface changes, the pressure in the fluid varies with these changes The relationship between fluid speed, pressure and elevation was first derived by Daniel Bernoulli

48 Bernoulli s Equation, 2 Consider the two shaded segments The volumes of both segments are equal The net work done on the segment is W =(P 1 P 2 ) V Part of the work goes into changing the kinetic energy and some to changing the gravitational potential energy

49 Bernoulli s Equation, 3 The change in kinetic energy: K = ½ mv 22 -½mv 1 2 There is no change in the kinetic energy of the unshaded portion since we are assuming streamline flow The masses are the same since the volumes are the same

50 Bernoulli s Equation, 4 The change in gravitational potential energy: U = mgy 2 mgy 1 The work also equals the change in energy Combining: W = (P 1 P 2 )V =½ mv 22 -½mv 12 + mgy 2 mgy 1

51 Bernoulli s Equation, 5 Rearranging and expressing in terms of density: P 1 + ½ ρv 12 + mgy 1 = P 2 + ½ ρv 22 + mgy 2 This is Bernoulli s Equation and is often expressed as P + ½ ρv 2 + ρgy = constant When the fluid is at rest, this becomes P 1 P 2 = ρgh which is consistent with the pressure variation with depth we found earlier

52 Bernoulli s Equation, Final The general behavior of pressure with speed is true even for gases As the speed increases, the pressure decreases

53 Applications of Fluid Dynamics Streamline flow around a moving airplane wing Lift is the upward force on the wing from the air Drag is the resistance The lift depends on the speed of the airplane, the area of the wing, its curvature, and the angle between the wing and the horizontal

54 Lift General In general, an object moving through a fluid experiences lift as a result of any effect that causes the fluid to change its direction as it flows past the object Some factors that influence lift are: The shape of the object The object s orientation with respect to the fluid flow Any spinning of the object The texture of the object s surface

55 Golf Ball The ball is given a rapid backspin The dimples increase friction Increases lift It travels farther than if it was not spinning

56 Atomizer A stream of air passes over one end of an open tube The other end is immersed in a liquid The moving air reduces the pressure above the tube The fluid rises into the air stream The liquid is dispersed into a fine spray of droplets

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