Elementary Fluid Mechanics CE 156 Undergraduate Course Notes

Elementary Fluid Mechanics (CE 156): Course Overview and Foundations

  • Institution: KAAF University

  • Department: Civil Engineering Department, Faculty of Civil and Computer Science

  • Lecturer: Ing. Sampson Osei, PhD

Course Objectives and Learning Outcomes

  • Aim of the Course:

    • To offer basic knowledge in fluid mechanics.

    • To obtain an understanding of the behavior of fluids.

    • To solve some simple problems of the type encountered in Engineering practice.

  • Course Objectives: By the end of the course, students are expected to:

    • Define and use basic fluid properties.

    • Define and use basic concepts in fluid mechanics.

    • Perform simple calculations in hydrostatics and kinematics.

    • Make simple designs in hydraulics.

Mode of Delivery and Assessment

  • Mode of Delivery:

    • Lectures

    • Tutorials (2 hours per week outside the usual schedule)

    • Laboratory sessions

  • Course Assessment:

    • Examination: 70%70\%

    • Combined Mid-semester Exams, Laboratory Reports, and Class/Home assignments: 30%30\%

  • Rules and Regulations:

    • Class attendance is compulsory.

    • Class assignments and quizzes will be unannounced.

  • Laboratory Experiments:

    1. Pressure gauges

    2. Plane surfaces immersed in fluids

    3. Floating bodies

    • Note: Lab reports must be written by the group and defended on an agreed schedule.

Recommended Reading Materials

  1. Fluid Mechanics (including Hydraulic Machines) – Dr. A. K. Jain, Khanna Publishers, Delhi, 2003.

  2. Fluid Mechanics (6th edition) – Frank M. White; McGraw-Hill, 2008.

  3. Introduction to Engineering Fluid Mechanics – J. A. Fox, 1985.

  4. Fluid Mechanics (5th Edition) – J. F. Douglas; J. M. Gasiorek; J. A. Swaffield; Lynne B. Jack.

  5. Hydraulics, Fluid Mechanics and Fluid Machines – S. Ramamrutham.

Definition and Nature of Fluids

  • Molecular Structure:

    • Solids: Molecules are so closely packed that the attractive forces between them are large; solids tend to retain their shape unless compelled by external forces.

    • Fluids: Composed of molecules with relatively larger distances between them; attractive forces are smaller than in solids.

  • Definition Perspectives:

    • Natural Form: A substance capable of flowing with no definite shape, assuming the shape of its container.

    • Deformation Characteristics: A fluid is a material which constantly deforms under the action of a shearing stress, no matter how small the stress.

    • Examples: Gases (air, LPG), liquids (water, kerosene).

Distinction Between Solids and Fluids

  • Elastic Solids: These are deformable, but deformation stops in balance with the acting force. Upon release, the body recovers its original state.

  • Plastic Solids: Deformed continuously during the application of force; once released, deformation stops (nominally).

  • Fluids: Contrastingly, a fluid keeps deforming even when it is free from force.

Comparison of Liquids and Gases

  • Liquids:

    • Composed of relatively close-packed molecules with strong cohesive forces.

    • Relatively incompressible.

    • A given mass occupies a definite volume if not subjected to extreme external pressures.

  • Gases:

    • Widely spaced molecules with relatively small cohesive forces.

    • Expand to fill the entire volume of a container if external pressure is removed.

    • Readily compressible.

    • Equilibrium is achieved only when completely enclosed.

    • Volume and density are greatly affected by changes in pressure (PP) and temperature (TT).

Introduction to Fluid Mechanics

  • Definition: The science of the mechanics of liquids and gases based on the same fundamental principles employed in solid mechanics. It concerns the behavior of fluids at rest and in motion.

  • Scope: Accounts for fluid properties, flow patterns, internal forces, and interactions with boundaries.

  • Fundamental Laws Applied:

    • Conservation of mass and energy.

    • Newton’s Law of Motion (force-momentum equation).

    • Laws of Thermodynamics.

  • Subdivisions:

    • Fluid Statics: Study of fluids at rest. Since there are no shearing forces at rest, all considered forces are normal to the planes on which they act.

    • Fluid Kinematics: Deals with the geometry of motion (streamlines and velocities) without considering the forces causing the motion.

    • Fluid Dynamics: Concerned with the relationship between velocities, accelerations, and the forces causing motion.

Engineering Applications

  • Civil Engineering: Hydropower dams, river currents, erosion, hydraulic structures, pipes.

  • Biomechanics: Flow of blood.

  • Mechanical Engineering: Design of pumps, water turbines, gas turbines.

  • Aeronautical Engineering: Airflow over aircraft to reduce drag and increase lift.

Units and Dimensions

  • Base Units: Fundamental quantities such as Length (LL), Mass (MM), and Time (TT) in an absolute system.

  • Derived Units: Combinations of base units.

  • SI Units (Systeme International d’Unites):

    • Area: L2L^2 (m2^2)

    • Volume: L3L^3 (m3^3)

    • Velocity: L/TL/T (m/s)

    • Density: M/L3M/L^3 (kg/m3^3)

    • Pressure: M/LT2M/LT^2 (N/m2^2 or Pascal)

    • Work: ML2/T2ML^2/T^2 (N.m)

    • Power: ML2/T3ML^2/T^3 (J/s or Watt)

    • Viscosity: M/LTM/LT (N.s/m2^2)

    • Flow Rate: L3/TL^3/T (m3^3/s)

Forces Acting on Fluids

  • Body Forces: Distributed forces acting on matter without direct contact (e.g., gravity, magnetic, inertia). Expressed as force per unit mass.

  • Surface Forces: Forces arising from direct contact with surrounding media (e.g., pressure force, frictional force, surface tension).

Fluid Properties

  • Property: A characteristic of a substance that is invariant when in a particular state. Properties uniquely determine the state of a system.

  • Extensive Properties: Depend on the amount of substance present (weight, momentum, volume, energy).

  • Intensive Properties: Independent of the amount of substance (temperature, pressure, viscosity, surface tension, mass density).

Density and Specific Gravity

  • Density (ρ\rho): Mass per unit volume.

    • ρ=mV\rho = \frac{m}{V}

    • At standard atmospheric pressure (760mmHg760\,mmHg or 101.3kPa101.3\,kPa) and 4C4^{\circ} C, ρ=1000kg/m3\rho = 1000\,kg/m^3.

  • Specific Volume (vsv_s): Reciprocal of density; volume per unit mass.

    • vs=1ρv_s = \frac{1}{\rho}

  • Specific (Unit) Weight (γ\gamma): Weight per unit volume.

    • γ=wV=mgV=ρg\gamma = \frac{w}{V} = \frac{mg}{V} = \rho g

  • Specific Gravity (SG): Ratio of the weight of a substance to the weight of an equal volume of water at standard conditions.

Physical Properties Data (Select SI values at 15.6-20°C)

  • Water (15.6C15.6^{\circ} C): ρ=999kg/m3\rho = 999\,kg/m^3, γ=9.80kN/m3\gamma = 9.80\,kN/m^3, μ=1.12×103N.s/m2\mu = 1.12 \times 10^{-3}\,N.s/m^2.

  • Mercury (20C20^{\circ} C): ρ=13,600kg/m3\rho = 13,600\,kg/m^3, γ=133kN/m3\gamma = 133\,kN/m^3.

  • Gasoline (15.6C15.6^{\circ} C): ρ=680kg/m3\rho = 680\,kg/m^3, γ=6.67kN/m3\gamma = 6.67\,kN/m^3.

  • Air (15C15^{\circ} C): ρ=1.23kg/m3\rho = 1.23\,kg/m^3, γ=1.20×101N/m3\gamma = 1.20 \times 10^1\,N/m^3, Gas constant R=2.869×102J/kgKR = 2.869 \times 10^2\,J/kg\cdot K.

Viscosity

  • Definition: The property of a fluid to offer resistance to shear stress.

  • Temperature Effects:

    • Liquids: Viscosity varies inversely with temperature.

    • Gases: Viscosity varies directly with temperature.

  • Newton’s Law of Viscosity: Shear stress (τ\tau) is proportional to the rate of shear strain.

    • τ=μdudy\tau = \mu \frac{du}{dy}

    • Dynamic Viscosity (μ\mu): Proportionality factor with units N.s/m2N.s/m^2.

    • Kinematic Viscosity (ν\nu): ν=μρ\nu = \frac{\mu}{\rho}, with units m2/sm^2/s.

  • Fluid Classification:

    • Newtonian Fluids: Shear stress is directly proportional to the rate of angular deformation; μ\mu is constant for fixed TT and PP (e.g., air, water, kerosene).

    • Non-Newtonian Fluids: Variable proportionality; may depend on time or magnitude of stress (e.g., plastics, paint, blood).

Compressibility and Surface Tension

  • Compressibility: Measure of volume change when subjected to external force. Defined by Bulk Modulus (KK):

    • K=ΔpΔV/VK = \frac{\Delta p}{\Delta V/V}

  • Incompressible Fluids: Density does not change due to external forces. Incompressible study is "Hydrodynamics"; compressible is "Gas Dynamics".

  • Surface Tension (σ\sigma): Magnitude of force per unit length caused by unbalanced molecular attractive forces at the surface.

    • Force due to internal pressure: Pπr2P \pi r^2

    • Force due to surface tension: 2πrσ2 \pi r \sigma

    • Equilibrium for a spherical drop: p=2σrp = \frac{2\sigma}{r}

  • Capillarity: Rise or fall of a fluid in a narrow tube.

    • Cohesive forces > Adhesive forces: Convex meniscus (capillary depression).

    • Adhesive forces > Cohesive forces: Concave meniscus (capillary rise).

    • Capillary height formula: h=4σcos(θ)γdh = \frac{4\sigma \cos(\theta)}{\gamma d}

Hydrostatics: Fluid at Rest

  • Basic Principle: In a fluid at rest, shear stress is zero; only normal stresses (pressure) exist.

  • Hydrostatic Pressure (pp): Compressive stress acting along the inside normal to the area element. Magnitude is independent of surface orientation.

  • Differential Equation of Hydrostatics:

    • 1ρdp=Xdx+Ydy+Zdz\frac{1}{\rho} dp = Xdx + Ydy + Zdz

    • X, Y, Z are body force projections per unit mass.

    • A fluid is in equilibrium only when acted upon by potential forces (UU).

  • Integration of Basic Equation:

    • p=p0+ρ(UU0)p = p_0 + \rho(U - U_0)

  • Gravity as the Only Body Force:

    • X=0,Y=0,Z=gX=0, Y=0, Z=-g

    • dp=ρgdzdp = -\rho g dz

    • Fundamental Equation: p=p0+γhp = p_0 + \gamma h

    • Absolute Pressure (pabsp_{abs}): Sum of external surface pressure and the pressure from the fluid column.

    • Gauge (Manometric) Pressure: Pressure excess above atmospheric (pgauge=γhp_{gauge} = \gamma h).

Pascal’s Law and Hydraulic Press

  • Pascal’s Law: Pressure applied to the surface of a liquid at rest is transmitted throughout the liquid in all directions without change.

  • Hydraulic Press: Ability to produce large output forces (F2F_2) from small input forces (F1F_1).

    • F2=p1A2=(F1A1)A2F_2 = p_1 A_2 = \left( \frac{F_1}{A_1} \right) A_2

    • F2=F1D2d2F_2 = F_1 \frac{D^2}{d^2}

Piezometric Height and Potential Energy

  • Piezometric Head: Pressure at a point measured as a column of fluid.

    • Absolute head: hA=pAγh_A = \frac{p_A}{\gamma}

    • Gauge head: hexh_{ex}

  • Potential Energy of Fluid at Rest:

    1. Energy by position: (P.E.)z=z×G(P.E.)_z = z \times G

    2. Energy by pressure: (P.E.)p=hex×G(P.E.)_p = h_{ex} \times G

  • Total Potential Head (HH): Specific potential energy (energy per unit weight).

    • H=z+hex=z+pγH = z + h_{ex} = z + \frac{p}{\gamma}

    • zz is Geometric Head; p/γp/\gamma is Pressure Head.

Pressure Variation in the Earth’s Atmosphere

  • Perfect Gas Equation of State:

    • pv=RTpv = RT

    • pρ=RT\frac{p}{\rho} = RT

    • γ=ρg=pgRT\gamma = \rho g = \frac{pg}{RT}

  • Process Equation:

    • pvn=constantp v^n = \text{constant}

    • T2T1=(v1v2)n1=(p2p1)n1n\frac{T_2}{T_1} = \left(\frac{v_1}{v_2}\right)^{n-1} = \left(\frac{p_2}{p_1}\right)^{\frac{n-1}{n}}

Practice Examples and Quizzes

  • Example (Oil/Water Tank): Oil (SG=0.80,0.90mSG=0.80, 0.90\,m deep) over water (2.1m2.1\,m deep).

    • Pressure at bottom: 27.7kPa27.7\,kPa.

  • Example (Bubble Nozzle): Bubble diameter 2mm2\,mm, σ=72.7×103N/m\sigma = 72.7 \times 10^{-3}\,N/m. Calculate required nozzle pressure excess.

  • Example (Capillary Glass): Find diameter for water rise h < 1.0\,mm at 20C20^{\circ} C.

    • Answer: 29.8mm29.8\,mm.

  • Hydraulic Jack Problem: Hand force F=100NF=100\,N.

    • Support load F2=12.2kNF_2 = 12.2\,kN.