All Study Guides Mathematical Fluid Dynamics Unit 2
💨 Mathematical Fluid Dynamics Unit 2 – Kinematics of Fluid MotionKinematics of fluid motion forms the foundation of fluid dynamics, describing how fluids move without considering the forces involved. This unit covers essential concepts like velocity and acceleration fields, streamlines, and the differences between Eulerian and Lagrangian descriptions.
Students learn about fluid properties, conservation laws, and vorticity, which are crucial for understanding complex fluid behaviors. These principles apply to various fields, from aerodynamics and hydrodynamics to meteorology and cardiovascular systems, highlighting the broad relevance of fluid kinematics.
Got a Unit Test this week? we crunched the numbers and here's the most likely topics on your next test Key Concepts and Definitions
Fluid dynamics studies the motion and behavior of fluids, both liquids and gases
Kinematics describes the motion of fluids without considering the forces causing the motion
Fluid properties include density, viscosity, compressibility, and surface tension
Velocity field represents the velocity of fluid particles at each point in space and time
Acceleration field describes the acceleration of fluid particles at each point in space and time
Streamlines are curves tangent to the velocity field at a given instant in time
Pathlines trace the path of individual fluid particles over time
Streaklines are the locus of fluid particles that have passed through a particular point in the flow
Fluid Properties and Characteristics
Density ( ρ ) (\rho) ( ρ ) is the mass per unit volume of a fluid and affects its inertia and buoyancy
Viscosity ( μ ) (\mu) ( μ ) measures a fluid's resistance to deformation and is responsible for internal friction
Dynamic viscosity relates shear stress to velocity gradients in the fluid
Kinematic viscosity ( ν = μ / ρ ) (\nu = \mu/\rho) ( ν = μ / ρ ) is the ratio of dynamic viscosity to density
Compressibility describes how much a fluid's density changes with pressure (ideal gases, liquids)
Surface tension arises from intermolecular forces and affects the formation of droplets and bubbles
Newtonian fluids have a linear relationship between shear stress and strain rate (water, air)
Non-Newtonian fluids have a nonlinear or time-dependent relationship between shear stress and strain rate (blood, paint)
Fundamental Equations of Fluid Motion
Continuity equation expresses the conservation of mass in a fluid: ∂ ρ ∂ t + ∇ ⋅ ( ρ u ⃗ ) = 0 \frac{\partial \rho}{\partial t} + \nabla \cdot (\rho \vec{u}) = 0 ∂ t ∂ ρ + ∇ ⋅ ( ρ u ) = 0
For incompressible fluids, the continuity equation simplifies to ∇ ⋅ u ⃗ = 0 \nabla \cdot \vec{u} = 0 ∇ ⋅ u = 0
Momentum equation (Navier-Stokes equations) describes the conservation of momentum in a fluid: ρ ( ∂ u ⃗ ∂ t + u ⃗ ⋅ ∇ u ⃗ ) = − ∇ p + μ ∇ 2 u ⃗ + ρ g ⃗ \rho \left(\frac{\partial \vec{u}}{\partial t} + \vec{u} \cdot \nabla \vec{u}\right) = -\nabla p + \mu \nabla^2 \vec{u} + \rho \vec{g} ρ ( ∂ t ∂ u + u ⋅ ∇ u ) = − ∇ p + μ ∇ 2 u + ρ g
Includes pressure gradients, viscous forces, and body forces (gravity)
Energy equation represents the conservation of energy in a fluid, considering heat transfer and work done
Constitutive equations relate stress and strain in the fluid, depending on its rheological properties
Boundary conditions specify the behavior of the fluid at the boundaries of the domain (no-slip, free-slip)
Eulerian vs. Lagrangian Descriptions
Eulerian description focuses on fluid properties at fixed points in space as time passes
Observes fluid motion from a fixed reference frame
Uses spatial coordinates ( x , y , z ) (x, y, z) ( x , y , z ) and time ( t ) (t) ( t ) as independent variables
Lagrangian description tracks individual fluid particles as they move through space and time
Follows fluid particles along their trajectories
Uses initial position ( X ⃗ ) (\vec{X}) ( X ) and time ( t ) (t) ( t ) as independent variables
Eulerian and Lagrangian descriptions are related through the material derivative: D D t = ∂ ∂ t + u ⃗ ⋅ ∇ \frac{D}{Dt} = \frac{\partial}{\partial t} + \vec{u} \cdot \nabla D t D = ∂ t ∂ + u ⋅ ∇
Eulerian description is more common in fluid dynamics due to its simplicity and ease of measurement
Streamlines, Pathlines, and Streaklines
Streamlines are curves tangent to the velocity field at a given instant in time
Represent the direction of fluid motion at each point
Do not intersect each other in steady flows
Pathlines trace the path of individual fluid particles over time
Show the trajectory of a fluid particle from its initial position
Can intersect each other in unsteady flows
Streaklines are the locus of fluid particles that have passed through a particular point in the flow
Formed by injecting dye or smoke into the fluid at a fixed point
Reveal the history of fluid motion and can highlight unsteady flow features
In steady flows, streamlines, pathlines, and streaklines coincide
In unsteady flows, streamlines, pathlines, and streaklines can differ significantly
Conservation Laws in Fluid Dynamics
Conservation of mass ensures that mass is neither created nor destroyed in a fluid: ∂ ρ ∂ t + ∇ ⋅ ( ρ u ⃗ ) = 0 \frac{\partial \rho}{\partial t} + \nabla \cdot (\rho \vec{u}) = 0 ∂ t ∂ ρ + ∇ ⋅ ( ρ u ) = 0
Conservation of momentum (Newton's second law) relates the change in momentum to the forces acting on a fluid: ρ ( ∂ u ⃗ ∂ t + u ⃗ ⋅ ∇ u ⃗ ) = − ∇ p + μ ∇ 2 u ⃗ + ρ g ⃗ \rho \left(\frac{\partial \vec{u}}{\partial t} + \vec{u} \cdot \nabla \vec{u}\right) = -\nabla p + \mu \nabla^2 \vec{u} + \rho \vec{g} ρ ( ∂ t ∂ u + u ⋅ ∇ u ) = − ∇ p + μ ∇ 2 u + ρ g
Conservation of energy (first law of thermodynamics) states that energy is conserved in a fluid, considering heat transfer and work done
Conservation of angular momentum is important in rotating flows and leads to the concept of vorticity
Conservation laws form the basis for the governing equations of fluid motion (continuity, Navier-Stokes, energy equations)
Vorticity and Circulation
Vorticity ( ω ⃗ ) (\vec{\omega}) ( ω ) is a measure of the local rotation in a fluid, defined as the curl of the velocity field: ω ⃗ = ∇ × u ⃗ \vec{\omega} = \nabla \times \vec{u} ω = ∇ × u
Vorticity is a vector quantity, with its direction indicating the axis of rotation
Vorticity magnitude represents the strength of the local rotation
Circulation ( Γ ) (\Gamma) ( Γ ) is a scalar measure of the total rotation in a fluid, defined as the line integral of velocity along a closed curve: Γ = ∮ C u ⃗ ⋅ d l ⃗ \Gamma = \oint_C \vec{u} \cdot d\vec{l} Γ = ∮ C u ⋅ d l
Kelvin's circulation theorem states that circulation is conserved in inviscid, barotropic flows
Helmholtz's vorticity theorems describe the behavior of vorticity in inviscid flows:
Vortex lines move with the fluid and maintain their strength
Vortex tubes have constant circulation along their length
Vorticity and circulation are important in understanding rotational flows, such as vortices and turbulence
Applications and Real-World Examples
Aerodynamics: Study of fluid motion around aircraft, vehicles, and buildings (lift, drag, wind loading)
Streamlined shapes reduce drag and improve efficiency (airfoils, bullet trains)
Vortex shedding can cause vibrations and structural damage (bridges, towers)
Hydrodynamics: Study of fluid motion in water bodies and hydraulic systems (rivers, oceans, pipes)
Pressure gradients drive flow in pipes and channels (water supply, hydropower)
Tides and currents transport heat, nutrients, and pollutants in oceans and lakes
Cardiovascular system: Blood flow through the heart, arteries, and veins
Pulsatile flow and non-Newtonian fluid properties affect blood circulation
Vortices and turbulence can occur in heart valves and aneurysms
Meteorology: Study of atmospheric fluid dynamics (weather patterns, climate)
Pressure gradients, Coriolis force, and buoyancy drive atmospheric circulation
Vorticity plays a key role in the formation and evolution of cyclones and hurricanes
Environmental fluid mechanics: Study of fluid motion in natural systems (rivers, estuaries, atmosphere)
Mixing and dispersion of pollutants in air and water bodies
Sediment transport and morphodynamics in rivers and coastal areas