Physics 105A Analytical Mechanics Constraints Generalized Coordinates Cyclic Coordinates and Conserved Quantities 28 June 2016 Manuel Calderón de la Barca Sánchez Forces of Constraint Revisit particle sliding off frictionless sphere. Solve using Lagrangian, leaving r=R from beginning. Solve using Lagrangian and find Normal force Force of Constraint Lagrange Multipliers m Rq 28 June 2016 MCBS Coordinate Transformations Cartesian to Spherical r x2 y 2 z 2 atan2 y, x z q cos x2 y 2 z 2 1 Cartesian to Cylindrical x2 y 2 atan2( y, x) zz Generalized coordinates 28 June 2016 qi qi ( x1 , x2 , x3 , x4 ,..., xN , t ) xi xi (q1 , q2 , q3 , q4 ,..., qN , t ) MCBS E-L Equations in Generalized Coordinates If the E-L equations hold for the xi coordinates, d L L 0, for 1 i N dt xi xi and the qi coordinates are related to the xi coordinates by qi qi ( x1 , x2 , x3 , x4 ,..., xN , t ) xi xi (q1 , q2 , q3 , q4 ,..., qN , t ) then the E-L equations hold for the qi coordinates. 28 June 2016 d L L 0, for 1 j N dt q j q j MCBS Analogy with functions Function has stationary points at f’(xmin)=0. Change coordinates x=g(y) Functions has stationary points at f’(ymin)=0, where ymin=g-1(xmin) E-L Equations: Variational derivative = 0. Streching coordinates does not change the existence of stationary values. 28 June 2016 MCBS From Stationary Action to F=ma Hamilton’s Principle of Stationary Action is equivalent to Newton’s Laws Stationary Action E-L equations Newton’s 2nd Law F=ma We showed it in cartesian coordinates We showed that if it E-L eqs. hold in one coordinate system, they are true in all other (sensible) coordinates. Comments: Deals only with scalars, makes problems easier. – Recall inclined plane, problem 3.8 and problem 6.1. d L L dt x x Local, not global. Multiple coordinates? Multiple E-L equations. Better suited for generalizations. Feynman’s approach to Quantum Mechanics: Based on Hamilton’s Principle. Maxwell’s Equations: Can be derived applying stationary action to Quantum Electrodynamics. 28 June 2016 MCBS