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CHAPTER-14

CHAPTER-14. Fluids. Ch 14-2, 3 Fluid Density and Pressure. Fluid: a substance that can flow Density  of a fluid having a mass m and a volume V is given by :  = m/V (uniform density) Density Units: kg/m 3

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CHAPTER-14

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  1. CHAPTER-14 Fluids

  2. Ch 14-2, 3 Fluid Density and Pressure • Fluid: a substance that can flow • Density  of a fluid having a mass m and a volume V is given by :  = m/V (uniform density) Density Units: kg/m3 • Density of a compressible material such as gases depends upon the pressure P, where P is given by: P=F/A

  3. Ch 14-4 Fluid at Rest • Hydrostatic Pressure: (Pressure due to fluid at rest) The pressure at a point in a fluid in static equilibrium depends upon the depth of that point but not on any horizontal dimension of the fluid or container. Consider the imaginary water cylinder with horizontal base , with weight mg, enclosed between two depths y1 and y2.The cylinder has a volume V, face area A and height y1-y2, Water is in static equilibrium. Three forces F1, F2 and mg acts such that F2-F1-mg=0; F2=F1+mg But p1=F1/A; p2=F2/A; m=Vg= A(y1-y2) p2=p1+g(y1-y2)

  4. Ch 14-4 Absolute Pressure and Gauge Pressure p2=p1+g(y1-y2) If p2=p;p1=p0 and y1=0 ; y2=-h p=p0+gh p =p-p0=gh P is Absolute pressure p is Gauge pressure

  5. Ch 14-4 Absolute Pressure and Gauge Pressure

  6. Ch 14-6 Pascal’s Principle • Pascal’s Principle :A change in the pressure applied to an enclosed incompressible fluid is transmitted undiminished to every portion of the fluid and to the walls of its container. • A change in pressure P at input of hydraulic lever is converted to change in pressure P at output of hydraulic lever P=Fi/Ai=Fo/Ao; Fo= Ao(Fi/Ai),FoFi • If input piston moves through a distance di , then the output piston moves through a smaller distance do because V=Aidi=Aodo • With a hydraulic lever, a given force applied over a given distance can be transformed to a greater force applied over a smaller distance

  7. Ch 14-7 Archimedes’ Principle • Archimedes’ Principle: • Buoyant Force FB: Upward force on a fully or partially submerged object by the fluid surrounding the object , magnitude of the force FB equal to weight of the displaced fluid mfg= Vfg. Vf is volume of the displaced fluid. • Floating Object: When an object floats in a fluid, the magnitude of FB is equal to magnitude of the gravitational force Fg (=mg). Then FB= Fg =mg= mfg= Vfg • A floating object displaces its own weight of fluid • For objects submerged in a fluid, its Apparent weight Wapp is less than true weight W Apparent weight Wapp= W-FB

  8. Ch 14-8 Ideal Fluid in Motion Four assumptions related to ideal flow: • Steady flow: the velocity of the moving fluid at any fixed point does not change with time • Incompressible Flow: Fluid has constant density • Nonviscous flow: an object can move through the fluid at constant speed- no resistive force within the fluid to moving objects through it • Irrotational flow: Objects moving through the fluid do not rotate about an axis through its center of mass

  9. Ch 14-9 Equation of Continuity • Equation of Continuity: A relation between the speed v of an ideal fluid flowing through a tube of cross sectional area A in steady flow state • Since fluid is incompressible, equal volume of fluid enters and leaves the tube in equal time • Volume V flowing through a tube in time t is V = Ax =Avt Then V = A1v1t =A2v2t • A1v1=A2v2 • RV=A1v1=constant (Volume flow rate) • Rm=A1v1=constant (Mass flow rate)

  10. Ch 14-10 Bernoulli’s Equation • Bernoulli’s Equation: • If y1,v1 and p1 are the elevation, speed and pressure of the fluid entering the tube and and y2,v2 and p2 are the elevation, speed and pressure of the fluid leaving the tube • Then p1+(v12)/2+gy1=p2+(v22)/2+gy2 or p+(v2)/2+gy = constant

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