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Properties of Fluids for Fluid Mechanics

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## Properties of Fluids for Fluid Mechanics

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**Properties of Fluids for Fluid Mechanics**P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Basic Steps to Design………….**Continuum Hypothesis**• In this course, the assumption is made that the fluid behaves as a continuum, i.e., the number of molecules within the smallest region of interest (a point) are sufficient that all fluid properties are point functions (single valued at a point). • For example: • Consider definition of density ρ of a fluid • δV* = limiting volume below which molecular variations may be important and above which macroscopic variations may be important.**Static Fluid**For a static fluid Shear Stress should be zero. For A generalized Three dimensional fluid Element, Many forms of shear stress is possible.**One dimensional Fluid Element**+Y u=U u=0 +X +**tyx**tzx txy tzy tyz txz Fluid Statics • Pressure : For a static fluid, the only stress is the normal stress since by definition a fluid subjected to a shear stress must deform and undergo motion. Y X Z • What is the significance of Diagonal Elements? • Vectorial significance : Normal stresses. • Physical Significance : ? • For the general case, the stress on a fluid element or at a point is a tensor**Y**tyx tzx tyy tzy txy txx tyz X tzz txz txz Z Stress Tensor**First Law of Pascal**Proof ?**Fluid Statics for Power Generation**P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Steps for Design of Flow Devices………….**Pressure Variation with Elevation**• For a static fluid, pressure varies only with elevation within the fluid. • This can be shown by consideration of equilibrium of forces on a fluid element • Basic Differential Equation: • Newton's law (momentum principle) applied to a static fluid • ΣF = ma = 0 for a static fluid • i.e., ΣFx = ΣFy = ΣFz = 0 1st order Taylor series estimate for pressure variation over dz**For a static fluid, the pressure only varies with elevation**z and is constant in horizontal xy planes. • The basic equation for pressure variation with elevation can be integrated depending on • whether ρ = constant i.e., the fluid is incompressible (liquid or low-speed gas) • or ρ = ρ(z), or compressible (high-speed gas) since g is constant.**Reading Material**• Fluid Mechanics – Frank M White, McGraw Hill International Editions. • Introduction to Fluid Mechanics – Fox & McDOnald, John Wiley & Sons, Inc. • Fluid Mechanics – V L Streeter, E Benjamin Wylie & K W Bedfore, WCB McGraw Hill. • Fluid Mechanics – P K Kundu & I M Cohen, Elsevier Inc.**Pressure Variation for Compressible Fluids**Basic equation for pressure variation with elevation Pressure variation equation can be integrated for γ(p,z) known. For example, here we solve for the pressure in the atmosphere assuming ρ(p,T) given from ideal gas law, T(z) known, and g ≠ g(z).**Draft Required to Establish Air Flow**Flue gas out Air in**Natural Draft**Zref,,pref pA = pref +Dp Hchimney Tgas Tatm B A**Zref,,pref**pA = pref +Dp Hchimney Tgas Tatm B A**Pressure variations in Troposphere:**Linear increase towards earth surface Tref & pref are known at Zref. a : Adiabatic Lapse rate : 6.5 K/km**Reference condition:**At Zref : T=Tref & p = pref**Pressure at A:**Pressure variation inside chimney differs from atmospheric pressure. The variation of chimney pressure depends on temperature variation along Chimney. Temperature variation along chimney depends on rate of cooling of hot gas Due to natural convection. Using principles of Heat transfer, one can calculate, Tgas(Z). If this is also linear: T = Tref,gas + agas(Zref-Z). Lapse rate of gas, agas is obtained from heat transfer analysis.**Natural Draft**• Natural Draft across the furnace, • Dpnat = pA – pB • The difference in pressure will drive the exhaust. • Natural draft establishes the furnace breathing by • Continuous exhalation of flue gas • Continuous inhalation of fresh air. • The amount of flow is limited by the strength of the draft.**Pressure Measurement**Another Application of Fluid Statics**Pressure Measurement**Pressure is an important variable in fluid mechanics and many instruments have been devised for its measurement. Many devices are based on hydrostatics such as barometers and manometers, i.e., determine pressure through measurement of a column (or columns) of a liquid using the pressure variation with elevation equation for an incompressible fluid.**PRESSURE**• Force exerted on a unit area : Measured in kPa • Atmospheric pressure at sea level is 1 atm, 76.0 mm Hg, 101 kPa • In outer space the pressure is essentially zero. The pressure in a vacuum is called absolute zero. • All pressures referenced with respect to this zero pressure are termed absolute pressures.**Many pressure-measuring devices measure not absolute**pressure but only difference in pressure. This type of pressure reading is called gage pressure. • Whenever atmospheric pressure is used as a reference, the possibility exists that the pressure thus measured can be either positive or negative. • Negative gage pressure are also termed as vacuum pressures.**Enlarged Leg**Inverted U Tube U Tube Two Fluid Inclined Tube Manometers**U-tube or differential manometer**Right Limb fluid statics : Left Limb fluid statics : Point 3 and 2 are at the same elevation and same fluid**Absolute, Gauge & Vacuum Pressures**System Pressure Gauge Pressure Absolute Pressure Atmospheric Pressure Absolute zero pressure**Absolute, Gauge & Vacuum Pressures**Atmospheric Pressure Vacuum Pressure System Pressure Absolute Pressure Absolute zero pressure**Y**tyy txx X tzz Z Stress Tensor for A Static Fluid 0 0 0 0 0 0**Shear stress(t): Tangential force on per unit area of**contact between solid & fluid**Elasticity (Compressibility)**• Increasing/decreasing pressure corresponds to contraction/expansion of a fluid. • The amount of deformation is called elasticity.