Fluid Dynamics Lecture Notes

Fluid Dynamics Lecture Notes

Session Goals

  • By the end of this video, you should be able to:

    • Relate volume flow rate to fluid velocity and cross-sectional area.

    • Explain the concept of continuity of fluid flow in a closed system.

    • Outline Bernoulli’s Principle for the flow of an incompressible fluid.

    • Relate the concept of energy conservation to fluid flow.

    • Apply the concepts of conservation of energy, continuity of flow, and Bernoulli’s Principle in discussing fluid pressure, velocity, and volume flow rate in an enclosed system.

    • Differentiate between laminar and turbulent flow.

    • Perform simple calculations involving the flow of fluids in an enclosed system.

    • Discuss simple clinical and other real-world applications of flowing fluids.

Fluid Dynamics Introduction

  • Flowing fluid requires:

    • A ‘path’: an enclosed region along which the fluid will move.

    • A ‘push’: a pressure difference between two locations on the path.

  • A pressure difference serves as a net force causing acceleration of the fluid.

Volume Flow Rate

  • Definition: Volume flow rate ( extit{F}) is the quantity of fluid that passes through a cross-sectional area of the path per unit time.

  • This may also be referred to as current.

  • SI Unit: cubic meters per second (m3/sm^3/s).

  • Mathematical Relation: F=AvF = Av

    • Where:

    • vv = velocity of flow

    • AA = cross-sectional area

Continuity of Flow

  • The continuity equation states that the quantity of fluid entering a point on the flow path is the same as the quantity of fluid leaving that point.

  • Continuity Equation:
    A1v1=A2v2A_1v_1 = A_2v_2

  • If the cross-sectional area changes, the velocity will change inversely to maintain the volume flow rate.

  • Note: In this equation, use small vv for velocity and do not confuse it with capital VV for volume.

Poiseuille’s Law

  • Definition: Poiseuille’s Law states that the volume flow rate ( extit{F}) is directly proportional to the pressure change (drop) (extΔPext{ΔP}) along the path and inversely proportional to the resistance of the path to flow (extRext{R}).

  • Mathematical Relation:
    F=racextΔPRF = rac{ ext{ΔP}}{R}

  • Key Insight: The greater the pressure change, the more work that is done, resulting in more fluid being moved per unit time.

Energy of Fluid Flow

  • For fluid to flow, it must possess mechanical energy.

  • Implication: Work must have been done on the fluid to induce flow.

  • The work originates from the pressure applied along the distance of flow.

Pressure of Flow and Work

  • Pressure Formula:
    extPressure=racextforceextareaext{Pressure} = rac{ ext{force}}{ ext{area}}

  • If we multiply both parts of the fraction by the distance of flow, we obtain:
    extpressure=racextforceimesextdistanceextareaimesextdistanceext{pressure} = rac{ ext{force} imes ext{distance}}{ ext{area} imes ext{distance}}

  • Equivalent Relations:

    • extforceimesextdistance=extworkext{force} imes ext{distance} = ext{work}

    • extAreaimesextdistance=extvolumeext{Area} imes ext{distance} = ext{volume}

  • Thus, we deduce:
    extPressure=racextworkextvolumeext{Pressure} = rac{ ext{work}}{ ext{volume}}
    extPressure=racextenergyimpartedextvolumeext{Pressure} = rac{ ext{energy imparted}}{ ext{volume}}

  • This leads to a relation involving kinetic and potential energy of the flowing fluid.

Flow Velocity

  • Definition: Flow velocity refers to the distance traveled per unit time by fluid particles.

  • This is distinct from volume flow rate, which is the quantity of fluid that moves per unit time.

Conservation of Flow Energy

  • As fluid flows, it possesses mechanical energy originating from the applied pressure.

  • Energy can be converted between potential and kinetic energy during the flow.

  • The sum of all energy types in a fluid system remains constant:
    extpressureenergy+extkineticenergy+extpotentialenergy=extconstantext{pressure energy} + ext{kinetic energy} + ext{potential energy} = ext{constant}

  • This concept is encapsulated in Bernoulli’s Principle.

Kinetic Energy of Flow

  • Kinetic Energy Formula:
    extKE=rac12mv2ext{KE} = rac{1}{2} mv^2

  • Often, kinetic energy density (energy per unit volume) is considered: extKE/V=rac12racmv2V=rac12hov2ext{KE}/V = rac{1}{2} rac{mv^2}{V} = rac{1}{2} ho v^2

    • Where:

    • mm = mass of fluid

    • vv = velocity of fluid

    • <br>ho<br>ho = density of fluid

Potential Energy of Flow

  • Potential Energy Formula:
    extPE=mghext{PE} = mgh

  • Often, potential energy density (energy per unit volume) is derived: extPE/V=racmghV=hoghext{PE}/V = rac{mgh}{V} = ho gh

    • Where:

    • gg = acceleration due to gravity

    • hh = height above a reference position

Bernoulli’s Equation

  • The sum of all energy types in a fluid system is constant:
    extpressureenergy+extkineticenergy+extpotentialenergy=extconstantext{pressure energy} + ext{kinetic energy} + ext{potential energy} = ext{constant}

  • Bernoulli’s Equation expressed mathematically:
    PV+rac12mv2+mgh=extconstantPV + rac{1}{2} mv^2 + mgh = ext{constant}

  • In energy density form, we write:
    P+rac12<br>hov2+<br>hogh=extconstantP + rac{1}{2} <br>ho v^2 + <br>ho gh = ext{constant}

  • In any system, the sizes of the various energy components will change with conditions, but their sum remains constant.

Bernoulli Principle Restated

  • When the cross-sectional area of the path narrows, the flow velocity must increase to maintain the volume flow rate entering and leaving that location.

  • As flow velocity increases, kinetic energy increases; thus, pressure must decrease to compensate if the heights of both locations are identical.

Bernoulli Effect

  • The energy per unit volume before is equal to the energy per unit volume after:
    P1+rac12pv12+pgh1=P2+rac12pv22+pgh2P_1 + rac{1}{2} p v_1^2 + p g h_1 = P_2 + rac{1}{2} p v_2^2 + p g h_2

  • Interpretation: Increased fluid speed results in decreased internal pressure.

  • In a practical context:

    • Given that A2<A1A_2 < A_1, it follows that v2>v1v_2 > v_1.

The Importance of Flow Dynamics

  • As flow velocity increases, the flow pattern can transition from laminar to turbulent.

Laminar vs Turbulent Flow

  • Laminar Flow:

    • Characterized by regular layers.

    • Minimal energy is removed from the system due to low friction.

  • Turbulent Flow:

    • Exhibits chaotic flow patterns.

    • Increased energy is removed from the system due to friction, generating heat.

    • Turbulence leads to reduced flow rate relative to applied pressure.

    • In the cardiovascular system, this means the heart must pump harder to achieve the necessary flow rate.

Summary of Learning Outcomes

  • By the conclusion of this session, you should be able to:

    • Relate volume flow rate to fluid velocity and cross-sectional area.

    • Explain the concept of continuity of fluid flow in a closed system.

    • Outline Bernoulli’s Principle for flow of an incompressible fluid.

    • Relate the concept of energy conservation to fluid flow.

    • Perform simple calculations involving the flow of fluids in an enclosed system.

    • Differentiate between laminar and turbulent flow.

    • Discuss simple clinical applications of flowing fluids.