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 (m^3/s).
Mathematical Relation: F = Av
Where:
v = velocity of flow
A = 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:
A_1v_1 = A_2v_2If the cross-sectional area changes, the velocity will change inversely to maintain the volume flow rate.
Note: In this equation, use small v for velocity and do not confuse it with capital V 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) ( ext{ΔP}) along the path and inversely proportional to the resistance of the path to flow ( ext{R}).
Mathematical Relation:
F = 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:
ext{Pressure} = rac{ ext{force}}{ ext{area}}If we multiply both parts of the fraction by the distance of flow, we obtain:
ext{pressure} = rac{ ext{force} imes ext{distance}}{ ext{area} imes ext{distance}}Equivalent Relations:
ext{force} imes ext{distance} = ext{work}
ext{Area} imes ext{distance} = ext{volume}
Thus, we deduce:
ext{Pressure} = rac{ ext{work}}{ ext{volume}}
ext{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:
ext{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:
ext{KE} = rac{1}{2} mv^2Often, kinetic energy density (energy per unit volume) is considered: ext{KE}/V = rac{1}{2} rac{mv^2}{V} = rac{1}{2} ho v^2
Where:
m = mass of fluid
v = velocity of fluid
ho = density of fluid
Potential Energy of Flow
Potential Energy Formula:
ext{PE} = mghOften, potential energy density (energy per unit volume) is derived: ext{PE}/V = rac{mgh}{V} = ho gh
Where:
g = acceleration due to gravity
h = height above a reference position
Bernoulli’s Equation
The sum of all energy types in a fluid system is constant:
ext{pressure energy} + ext{kinetic energy} + ext{potential energy} = ext{constant}Bernoulli’s Equation expressed mathematically:
PV + rac{1}{2} mv^2 + mgh = ext{constant}In energy density form, we write:
P + rac{1}{2}
ho v^2 +
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:
P_1 + rac{1}{2} p v_1^2 + p g h_1 = P_2 + rac{1}{2} p v_2^2 + p g h_2Interpretation: Increased fluid speed results in decreased internal pressure.
In a practical context:
Given that A_2 < A_1, it follows that v_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.