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Section I: (Chapter 1) Review of Classical Mechanics Newtonian mechanics Coordinate transformations Lagrangian approach Hamiltonian with generalized momenta.

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Presentation on theme: "Section I: (Chapter 1) Review of Classical Mechanics Newtonian mechanics Coordinate transformations Lagrangian approach Hamiltonian with generalized momenta."— Presentation transcript:

1 Section I: (Chapter 1) Review of Classical Mechanics Newtonian mechanics Coordinate transformations Lagrangian approach Hamiltonian with generalized momenta

2 Session 1. (Chapter 1) Review of Classical Mechanics Newtonian Mechanics Given force F, determine position of an object at anytime: F ~ d 2 r/dt 2 Proportionality constant = m, property of the object. Integration of eq. (1) gives r=r(t) ---the solution: prediction of the motion. In Cartesian coordinates: F x = md 2 x/dt 2 F y = md 2 y/dt 2 F z = md 2 z/dt 2

3 Examples of position or velocity dependent forces: Gravitational force: F = Gm 1 m 2 /r 2 (=mg, on Earth surface) Electrostatic force: F = kq 1 q 2 /r 2 Charge moving in Magnetic field: F = qvxB Other forces (not “fundamental”) Harmonic force: F = -kr

4 Coordinate transformations Polar coordinates: x=rsin  ; y=rcos  Spherical coordinates: x=rsin  cos  ; y=rsin  sin  ; z=rcos  Cylindrical coordinates: x=  cos  ; y=  sin  ; z=z It is harder to do a vector transformation such as from a Cartesian coordinate system to other coordinate systems. But it is easier to transform scalar such as

5 Inclass I-1. a) Write down Newton equation of motion in Cartesian coordinates for an object moving under the influence of a two-dimensional central force of the form F=k/r 2, where k is a constant. b) What difficulty you will encounter if you would like to derive the Newton equations of motion in polar coordinates? y F x 0 y F x 0 r 

6 Lagrangian approach: Instead of force, one uses potential to construct equations of motion---Much easier. Also, potential is more fundamental: sometimes there is no force in a system but still has a potential that can affect the motion. Use generalized coordinates: (x,y,z), (r, ,  ), …..In general: (q 1,q 2,q 3 ….) Define Lagrangian: Equations of motion becomes:

7 Inclass I-2. Write down the Lagrangian in polar coordinates for an object moving under the influence of a two-dimensional central potential of the form V(r)=k/r, where k is a constant. Derive the equations of motion using Lagrangian approach. Compare this result with that obtained in Inclass I-1. y x 0 r  V(r)=k/r

8 Hamiltonian Definition of generalized momenta: If L  L(q j ), then p j =constant, “cyclic” in q j. Definition of Hamiltonian: What are the differences between L and H ?

9 Inclass I-3. An object is moving under the influence of a two-dimensional central potential of the form V(r)=k/r, where k is a constant. Determine the Hamiltonian in a) the Cartesian coordinate system; b) in polar coordinate system. (Hint: determine the generalized momenta first before you determine the Hamiltonian.)

10 (Inclass) I-4. An electron is placed in between two electrostatic plates separated by d. The potential difference between the plates is  o. a) Derive the equations of motion using Lagrangian method (3-dimensional motion) in Cartesian coordinate system. b) Determine the Hamiltonian using Cartesian coordinate system. c) Determine the Hamiltonian using cylindrical coordinate system. z e-e- d

11 Introduction to Quantum Mechanics Homework 1: Due:Jan 20, 12.00pm (Will not accept late homework) Inclass I-1 to I-4. Problems: 1.5, 1.7, 1.11, 1.12


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