Chapter 8 Dynamics II: Motion in a Plane

Dynamics in Two Dimensions

  • Newton's second law applies in 2D and 3D motion: a=Fnetm\vec{a} = \frac{\vec{F}_{net}}{m}
  • Forces can be decomposed along orthogonal axes.

Uniform Circular Motion

  • Uses the rtz-coordinate system.
    • tt-axis: Tangential to the circle, counterclockwise.
    • rr-axis: Radial, from particle to circle's center.
    • zz-axis: Perpendicular to the motion plane.
  • Velocity vector: Only a tangential component (vt=ωrv_t = \omega r).
  • Acceleration vector: Only a radial component (ar=v2r=ω2ra_r = \frac{v^2}{r} = \omega^2 r).
  • Net force (central force) is directed towards the circle's center: Fnet=mv2r=mω2rF_{net} = m\frac{v^2}{r} = m\omega^2 r

Key Concepts and Clicker Questions

  • Inertia: Without a central force, an object moves in a straight path.
  • Static Friction: Provides the necessary centripetal force for a car to round a curve. μs=v2Rg\mu_s = \frac{v^2}{Rg}
    • μ<em>s>1\mu<em>s > 1 for tires on dry asphalt, \mus < 0.1 for tires on icy roads.
  • Banked Track: On an icy banked road, the net force is horizontal (towards the center) with Fnet=mv2RF_{net} = \frac{mv^2}{R}.
  • Banked Curve with Friction: Car 1 (no friction) vs. Car 2 (moving slower) - Static friction on Car 2 is directed up the banked curve.

Circular Orbits

  • Occur when the trajectory curvature is parallel to the planet's curvature.
  • Objects are perpetually in free fall.
  • Gravitational force: FG=mg\vec{F}_G = m\vec{g}, toward the center of the planet.

Reasoning About Circular Motion

  • Centrifugal Force: A fictitious force in a non-inertial reference frame.
  • On the rotating Earth, FG=mgF_G = mg where gg accounts for the rotation.

Nonuniform Circular Motion

  • Tangential force component leads to tangential acceleration.
  • Net force is the sum of radial and tangential forces and does not point towards the center.

Loop-the-Loop

  • Top: Normal force and weight are in the same direction.
    • Minimum speed to stay on track: v<em>min=gRv<em>{min} = \sqrt{gR}, where F</em>cent=mv2R=mgF</em>{cent} = \frac{mv^2}{R} = mg
  • Bottom: Fcent=mv2R=nmgF_{cent} = \frac{mv^2}{R} = n - mg
  • Side: Fcent=mv2R=nF_{cent} = \frac{mv^2}{R} = n
  • Tangential Acceleration: Occurs when the net force has a tangential component.

Well of Death Stunt

  • Normal force provides the centripetal force: F<em>cent=n</em>wc=mv2rF<em>{cent} = n</em>{wc} = \frac{mv^2}{r}
  • Minimum speed to maintain height: v=grμsv = \sqrt{\frac{gr}{\mu_s}}