Physics 451551 Theoretical Mechanics G A Krafft Old

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Physics 451/551 Theoretical Mechanics G. A. Krafft Old Dominion University Jefferson Lab Lecture 18

Physics 451/551 Theoretical Mechanics G. A. Krafft Old Dominion University Jefferson Lab Lecture 18 Theoretical Mechanics Fall 2018

Sound Waves • Properties of Sound – Requires medium for propagation – Mainly longitudinal

Sound Waves • Properties of Sound – Requires medium for propagation – Mainly longitudinal (displacement along propagation direction) – Wavelength much longer than interatomic spacing so can treat medium as continuous • Fundamental functions – Mass density – Velocity field • Two fundamental equations – Continuity equation (Conservation of mass) – Velocity equation (Conservation of momentum) • Newton’s Law in disguise Theoretical Mechanics Fall 2018

Fundamental Functions • Density ρ(x, y, z), mass per unit volume • Velocity field

Fundamental Functions • Density ρ(x, y, z), mass per unit volume • Velocity field Theoretical Mechanics Fall 2018

Continuity Equation • Consider mass entering differential volume element • Mass entering box in

Continuity Equation • Consider mass entering differential volume element • Mass entering box in a short time Δt • Take limit Δt→ 0 Theoretical Mechanics Fall 2018

 • By Stoke’s Theorem. Because true for all d. V • Mass current

• By Stoke’s Theorem. Because true for all d. V • Mass current density (flux) (kg/(sec m 2)) • Sometimes rendered in terms of the total time derivative (moving along with the flow) • Incompressible flow and ρ constant Theoretical Mechanics Fall 2018

Pressure Scalar • Displace material from a small volume d. V with sides given

Pressure Scalar • Displace material from a small volume d. V with sides given by d. A. The pressure p is defined to the force acting on the area element – Pressure is normal to the area element – Doesn’t depend on orientation of volume • External forces (e. g. , gravitational force) must be balanced by a pressure gradient to get a stationary fluid in equilibrium • Pressure force (per unit volume) Theoretical Mechanics Fall 2018

Hydrostatic Equilibrium • Fluid at rest • Fluid in motion • As with density

Hydrostatic Equilibrium • Fluid at rest • Fluid in motion • As with density use total derivative (sometimes called material derivative or convective derivative) Theoretical Mechanics Fall 2018

Fluid Dynamic Equations • Manipulate with vector identity • Final velocity equation • One

Fluid Dynamic Equations • Manipulate with vector identity • Final velocity equation • One more thing: equation of state relating p and ρ Theoretical Mechanics Fall 2018

Energy Conservation • For energy in a fixed volume ε internal energy per unit

Energy Conservation • For energy in a fixed volume ε internal energy per unit mass • Work done (first law in co-moving frame) • Isentropic process (s constant, no heat transfer in) Theoretical Mechanics Fall 2018

Theoretical Mechanics Fall 2018

Theoretical Mechanics Fall 2018

Bernoulli’s Theorem • Exact first integral of velocity equation when – Irrotational motion –

Bernoulli’s Theorem • Exact first integral of velocity equation when – Irrotational motion – External force conservative – Flow incompressible with fixed ρ • Bernouli’s Theorem • If flow compressible but isentropic Theoretical Mechanics Fall 2018

Kelvin’s Theorem on Circulation • Already discussed this in the Arnold material • To

Kelvin’s Theorem on Circulation • Already discussed this in the Arnold material • To linear order Theoretical Mechanics Fall 2018

 • The circulation is constant about any closed curve that moves with the

• The circulation is constant about any closed curve that moves with the fluid. If a fluid is stationary and acted on by a conservative force, the flow in a simply connected region necessarily remains irrotational. Theoretical Mechanics Fall 2018

Lagrangian for Isentropic Flow • Two independent field variables: ρ and Φ • Lagrangian

Lagrangian for Isentropic Flow • Two independent field variables: ρ and Φ • Lagrangian density • Canonical momenta Theoretical Mechanics Fall 2018

 • Euler Lagrange Equations • Hamiltonian Density internal energy plus potential energy plus

• Euler Lagrange Equations • Hamiltonian Density internal energy plus potential energy plus kinetic energy Theoretical Mechanics Fall 2018

Sound Waves • Linearize about a uniform stationary state • Continuity equation • Velocity

Sound Waves • Linearize about a uniform stationary state • Continuity equation • Velocity equation • Eisentropic equation of state Theoretical Mechanics Fall 2018

Flow Irrotational • Take curl of velocity equation. Conclude flow irrotational • Scalar wave

Flow Irrotational • Take curl of velocity equation. Conclude flow irrotational • Scalar wave equation • Boundary conditions Theoretical Mechanics Fall 2018

3 -D Plane Wave Solutions • Ansatz • Energy flux Theoretical Mechanics Fall 2018

3 -D Plane Wave Solutions • Ansatz • Energy flux Theoretical Mechanics Fall 2018

Helmholz Equation and Organ Pipes Theoretical Mechanics Fall 2018

Helmholz Equation and Organ Pipes Theoretical Mechanics Fall 2018

Theoretical Mechanics Fall 2018

Theoretical Mechanics Fall 2018

Green Function for Wave Equation • Green Function in 3 -D • Apply Fourier

Green Function for Wave Equation • Green Function in 3 -D • Apply Fourier Transforms • Fourier transform equation to solve and integrate by parts twice Theoretical Mechanics Fall 2018

Green Function Solution • The Fourier transform of the solution is • The Green

Green Function Solution • The Fourier transform of the solution is • The Green function is Theoretical Mechanics Fall 2018

 • Alternate equation for Green function • Simplify • Yukawa potential (Green function)

• Alternate equation for Green function • Simplify • Yukawa potential (Green function) Theoretical Mechanics Fall 2018

Helmholtz Equation • Driven (Inhomogeneous) Wave Equation • Time Fourier Transform • Wave Equation

Helmholtz Equation • Driven (Inhomogeneous) Wave Equation • Time Fourier Transform • Wave Equation Fourier Transformed Theoretical Mechanics Fall 2018

Green Function • Green function satisfies Theoretical Mechanics Fall 2018

Green Function • Green function satisfies Theoretical Mechanics Fall 2018

 • Green function is • Satisfies • Also, with causal boundary conditions is

• Green function is • Satisfies • Also, with causal boundary conditions is Theoretical Mechanics Fall 2018

Causal Boundary Conditions • Can get causal B. C. by correct pole choice ω

Causal Boundary Conditions • Can get causal B. C. by correct pole choice ω k plane • Gives so-called retarded Green function • Green function evaluated Theoretical Mechanics Fall 2018