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Wave Physics PHYS 2023 Tim Freegarde.

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Presentation on theme: "Wave Physics PHYS 2023 Tim Freegarde."— Presentation transcript:

1 Wave Physics PHYS 2023 Tim Freegarde

2 Coming up in Wave Physics...
today’s lecture: local and macroscopic definitions of a wave transverse waves on a string: wave equation travelling wave solutions other wave systems: electromagnetic waves in coaxial cables shallow-water gravity waves sinusoidal and complex exponential waveforms

3 Wave Physics Local/microscopic definition:
a collective bulk disturbance in which what happens at any given position is a delayed response to the disturbance at adjacent points speed of propagation is derived particles (Lagrange) fields (Euler) static dynamic equilibrium eg Poisson’s equation SHM WAVES Macroscopic definition: a time-dependent feature in the field of an interacting body, due to the finite speed of propagation of a causal effect speed of propagation is assumed

4 Wave Physics Local/microscopic definition:
a collective bulk disturbance in which what happens at any given position is a delayed response to the disturbance at adjacent points speed of propagation is derived What is the net force on the penguin? rest position For an elastic penguin, Hooke’s law gives separation displacement If the penguin has mass , Newton’s law gives pressure elasticity density where

5 Waves on long strings

6 Solving the wave equation
shallow waves on a long thin flexible string use physics/mechanics to write partial differential wave equation for system travelling wave insert generic trial form of solution wave velocity find parameter values for which trial form is a solution

7 Travelling wave solutions
consider a wave shape at which is merely translated with time use physics/mechanics to write partial differential wave equation for system where insert generic trial form of solution use chain rule for derivatives find parameter values for which trial form is a solution

8 General solutions wave equation is linear – i.e. if
use physics/mechanics to write partial differential wave equation for system are solutions to the wave equation, then so is insert generic trial form of solution arbitrary constants find parameter values for which trial form is a solution note that two solutions to our example:

9 Particular solutions fit general solution to particular constraints – e.g. use physics/mechanics to write partial differential wave equation for system insert generic trial form of solution x find parameter values for which trial form is a solution

10 Plucked guitar string x

11 Wave propagation transverse motion of taut string
use physics/mechanics to write partial differential wave equation for system e-m waves along coaxial cable shallow-water waves flexure waves string with friction travelling wave: general form sinusoidal insert generic trial form of solution complex exponential damped standing wave soliton speed of propagation find parameter values for which trial form is a solution dispersion relation string motion from initial conditions

12 Wave equations waves are collective bulk disturbances, whereby the motion at one position is a delayed response to the motion at neighbouring points use physics/mechanics to write partial differential wave equation for system propagation is defined by differential equations, determined by the physics of the system, relating derivatives with respect to time and position insert generic trial form of solution e.g. find parameter values for which trial form is a solution but note that not all wave equations are of the same form

13 Electromagnetic waves
aliexpress.com NASA/DOE/Fermi LAT Collaboration Light Radio Gamma radiation

14 Waves along a coaxial cable
V(x) V(x+δx) r a I x -δQ δQ x x+δx

15 Waves along a coaxial cable
r a x -δQ δQ x x+δx

16 Waves along a coaxial cable
r a I x x x+δx

17 Water waves Ocean waves Severn bore Kelvin ship wake Tsunami
theguardian.com © Jason Hawkes / Getty Images © Reuters / Mainichi Shimbun Ocean waves Severn bore Kelvin ship wake Tsunami

18 Shallow-water waves ε1 ε2 h(x) volume = h(x) (δx+ε2-ε1) δy v1 v2 δx

19 Shallow-water waves h(x) volume = h(x) (δx+ε2-ε1) δy v1 δx x-δx x x+δx

20 Velocities of waves on a string
x x phase velocity (group velocity) transverse string velocity


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