02 · Falling without landing

How can a satellite keep falling without reaching the ground?

Without gravity, would it move radially outward or along the tangent?

  1. Start a circular orbit and show vectors.
  2. Pause and advance one step at a time.
  3. Compare how velocity and acceleration turn.

Measurement

Compare x, y, v_x, v_y and |a| at two positions.

Velocity carries the body along a tangent while gravity bends its path inward. Apparent weightlessness is shared free fall, not the absence of gravity. In circular motion acceleration changes direction without changing speed.

r is position vector in m; a in m/s²; v in m/s.

a = −μr/|r|³; a_c = v²/r; v·a = 0 (circular)

Worked example 1

At r=7×10⁶ m, acceleration is 8.13 m/s², far from zero.

Worked example 2

In 1 s the small inward fall is approximately aΔt²/2=4.07 m while tangential travel is about 7.55 km.

Use a dot product to check perpendicular velocity and acceleration.

Assumptions

Newtonian two-body model with fixed central mass. No drag, third bodies, oblateness or relativity. Visual sizes are illustrative; initial conditions are fictional, not live ephemerides.

University Physics Volume 1, 13.2 Gravitation Near Earth’s Surface

University Physics Volume 1, 13.4 Satellite Orbits and Energy