Physics 105A 28 June 2016 Manuel Calderón de la Barca Sánchez Sec 3.3: Newton’s Laws as diff. eqns. F=ma as a differential equation mx = F(t, x,v) – Force depends only on t (oscillatory driving forces) x= dv dt – Force depends only on x (mass-spring system, simple harmonic motion) x=v dv dx – Force depends only on v (drag forces, turbulence) x = dv Examples dt – Review: Falling under constant Gravitational Force – F(v) case: Falling under constant Gravitational Force + air drag 28 June 2016 MCBS Motion under constant g field. A particle of mass m is subject to a constant force F=-mg directed down. The particle starts at rest at height h. Solve for y(t) in two ways: a = dv/dt a = vdv/dx 28 June 2016 MCBS Including air drag to a falling ball A physics prof. is dropped from rest at height h. Assume that the drag force from the air takes the form Fd = -b v = -mav Solve the equations of motion to obtain v(t) and y(t). 28 June 2016 MCBS Projectiles: Throwing a ball For a given initial speed, at which inclination angle should a ball be thrown so that it travels the max. horizontal distance by the time it returns to the ground? Assume ground is horizontal, ball is released at ground level. What is the optimal angle if the ground is sloped at an angle b (where -90<b<90 degrees)? 28 June 2016 MCBS