Physics 321 Hour 22 Central Force Problems Straight-line Motion in Spherical or Cylindrical Coordinates Coordinates y r r x a t We want to treat r like a Cartesian coordinate, but if we do, if appears that there’s a force on the mass even when there is no force! Understanding the “Fictitious” Force Think of r like x : πΉ 0 a The force acts in the +r direction. r Understanding the “Fictitious” Force π₯=π π¦ = π£π‘ → π= π2 + π£ 2 π‘ 2 2π£ 2 π‘ π£ 2 π‘ π= = 2π π π£ 2 π£ 2π‘ π£ 2π‘ π£ 2 π£ 2π‘2 π= − 2 = 1− 2 π π π π π π£ 2 π2 − π£ 2π‘ 2 π£ 2 π2 π£ 2 π2 = = = 3 2 2 π π π π π Understanding the “Fictitious” Force ππ£ 2 π2 πΉ = ππ = π3 π = ππ£π π2 πΉ= ππ 3 We can define a corresponding potential energy: π=− πΉππ = − π2 π2 ππ = + 3 ππ 2ππ 2 Before we even consider real forces, we have to “add” a repulsive centrifugal force or centrifugal potential to the problem: π2 πΉ= ππ 3 π2 π=+ 2ππ 2 Centrifugal Potential πππππ‘ β2 =+ 2μπ 2 ππππ = πππππ‘ + ππ ππ = −πΊ ππ π Central Force • Force is in the radial direction in spherical coordinates • The curl is always zero – even if the force isn’t inverse square • Source at the origin πΌ πΌπ πΉ = π π = π+1 π π • Source at π1 πΌ(π2 − π1 ) πΉ21 = |π2 − π1 |π+1 Central Force • Source at π2 πΉ12 • Potential energy πΌ(π1 − π2 ) = |π2 − π1 |π+1 πΌ π−1 π π = , π−1 π2 − π1 π≠1 Inverse-square Force • Source at π1 πΉ21 • Potential energy πΌ(π2 − π1 ) = |π2 − π1 |3 πΌ π π = π2 − π1 Example moon_orbit.nb