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PHY 711 Classical Mechanics and Mathematical Methods
11-11:50 AM MWF Olin 102 Plan for Lecture 38 General review Classical mechanics – traditional topics Classical mechanics – related topics Mathematical methods Course assessment 12/05/2016 PHY 711 Fall Lecture 38
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Review of course topics
Classical mechanics – traditional topics Particle scattering; scattering cross section Inertial and accelerated reference frames Calculus of variations Lagrangian and Hamiltonian formalisms Small oscillations near equilibrium Rigid body rotations Classical mechanics – additional topics Mechanics of continuous media Mechanics of fluids; bulk and surface motions Heat conduction Elastic continua Mathematical methods 12/05/2016 PHY 711 Fall Lecture 38
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Scattering theory: detector 12/05/2016 PHY 711 Fall Lecture 38
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If we can assume that the process is isotropic in f; results depend on b and q:
Figure from Marion & Thorton, Classical Dynamics 12/05/2016 PHY 711 Fall Lecture 38
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In general, scattering is most easily analyzed in the center of mass frame -- relationship between center of mass and laboratory frames of reference: v1 V1 VCM y q lab CM for elastic case 12/05/2016 PHY 711 Fall Lecture 38
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Differential cross sections in different reference frames
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Differential cross sections in different reference frames –
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Physics of rotating coordinate system
Effects on acceleration (rotation only): 12/05/2016 PHY 711 Fall Lecture 38
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Equation of motion on Earth’s surface
w y (east) z (up) q x (south) 12/05/2016 PHY 711 Fall Lecture 38
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Calculus of variation example for a pure integral functions
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Lamp shade shape y(x) y xi yi x xf yf 12/05/2016
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Application of calculus of variation to Lagrangian mechanics:
Potential energy Kinetic energy 12/05/2016 PHY 711 Fall Lecture 38
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Recipe for constructing the Hamiltonian and analyzing the equations of motion
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Use of Lagrangian/Hamiltonian formalism for molecular dynamics
rij Pairwise interaction between particles From this Lagrangian, can find the 3N coupled 2nd order differential equations of motion and/or find the corresponding Hamiltonian, representing the system at constant energy, volume, and particle number N (N,V,E ensemble). 12/05/2016 PHY 711 Fall Lecture 38
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H. C. Andersen’s effective Lagrangian for constant pressure
simulations Equations of motion in “original” coordinates: 12/05/2016 PHY 711 Fall Lecture 38
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Normal modes of vibration about equilibrium:
Example – linear molecule m1 m2 m3 12/05/2016 PHY 711 Fall Lecture 38
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m1 m2 m3 m1 m2 m3 m1 m2 m3 12/05/2016 PHY 711 Fall Lecture 38
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Consider an extended system of masses and springs:
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3-dimensional periodic lattices
Extension of ideas -- 3-dimensional periodic lattices Example – face-centered-cubic unit cell (Al or Ni) Diagram of atom positions Diagram of q-space n(q) 12/05/2016 PHY 711 Fall Lecture 38
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From: PRB 59 3395 (1999); Mishin et. al. n(q)
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Euler angles for expressing rigid body rotation:
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Rotational kinetic energy for “symmetric” top:
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Equations of motion for continuous media
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Stress tensor for fluids
Stress tensor for elastic media (Hooke’s law in terms of displacement u; linear terms only ) 12/05/2016 PHY 711 Fall Lecture 38
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