PHY 711 Classical Mechanics and Mathematical Methods

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Presentation transcript:

PHY 711 Classical Mechanics and Mathematical Methods 9-9:50 AM MWF Olin 107 Plan for Lecture 2: Brief comment on quiz Particle interactions Notion of center of mass reference fame Introduction to scattering theory 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

8/30/2017 PHY 711 Fall 2017 -- Lecture 2

8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Schedule additional office hours by email: natalie@wfu.edu 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Comment on quiz questions 1. 3. 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Scattering theory: detector 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

b Figure from Marion & Thorton, Classical Dynamics 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Note: We are assuming that the process is isotropic in f Note: Notion of cross section is common to many areas of physics including classical mechanics, quantum mechanics, optics, etc. Only in the classical mechanics can we calculate it using geometric considerations b Figure from Marion & Thorton, Classical Dynamics Note: We are assuming that the process is isotropic in f 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Simple example – collision of hard spheres Microscopic view: 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Simple example – collision of hard spheres -- continued 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Relationship of scattering cross-section to particle interactions -- Classical mechanics of a conservative 2-particle system. 1 2 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Typical two-particle interactions – 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Relationship between center of mass and laboratory frames of reference 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Classical mechanics of a conservative 2-particle system -- continued 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

In laboratory frame: In center-of-mass frame: Note: The following analysis will be carried out in the center of mass frame of reference. In laboratory frame: In center-of-mass frame: v1 V1 m m1 r vCM origin mtarget Also note: We are assuming that the interaction between particle and target V(r) conserves energy and angular momentum. 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Need to relate these parameters to differential cross section For a continuous potential interaction in center of mass reference frame: Need to relate these parameters to differential cross section  to be discussed on Friday V(r) Erel rmin 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Relationship between normal laboratory reference and center of mass: It is often convenient to analyze the scattering cross section in the center of mass reference frame. Relationship between normal laboratory reference and center of mass: Laboratory reference frame: Before After m1 m2 v1 u1 y u2=0 z v2 Center of mass reference frame: Before After m1 m2 V1 U1 U2 q q V2 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Relationship between center of mass and laboratory frames of reference -- continued 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Relationship between center of mass and laboratory frames of reference V1 VCM v1 y q For elastic scattering 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Digression – elastic scattering Also note: 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Relationship between center of mass and laboratory frames of reference – continued (elastic scattering) v1 V1 VCM y q 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Differential cross sections in different reference frames 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Differential cross sections in different reference frames – continued: 8/30/2017 PHY 711 Fall 2017 -- Lecture 2

Example: suppose m1 = m2 8/30/2017 PHY 711 Fall 2017 -- Lecture 2