1.4 Reference Frames and Relative Motion
- Syllabus
- 2024
- Topic
- 1.4
- Level
- —
For one-dimensional motion, an observer measures the object’s velocity relative to the observer’s own frame. Choose a positive direction and keep every velocity signed.
vobject/observer=vobject/ground−vobserver/ground
Hypothetical example: east is positive. A passenger walks east at +2ms−1 relative to a train moving east at +10ms−1 relative to the ground. The passenger’s ground velocity is +12ms−1; equivalently, a ground observer moving at 0 measures 12 m/s east, while a train observer measures 12−10=+2ms−1.
Velocity can differ between inertial frames, but acceleration is the same in all inertial frames. AP Physics 1 restricts relative-velocity vector addition or subtraction to one dimension and assumes the stated frame is inertial unless told otherwise.
A reference frame is the coordinate system and clock attached to an observer. Identify the observer, origin, positive axis and time reference before describing position or velocity.
| Same event | Ground frame | Train frame |
|---|---|---|
| Train moving east at 10 m/s | Train velocity is +10ms−1 | Train velocity is 0 |
| Seat fixed inside the train | Seat changes ground position | Seat position is constant |
Changing frames can change the measured position and velocity—both magnitude and direction—but does not change the underlying event. State conclusions as ‘relative to the ground’ or ‘relative to the train.’
Different frame-dependent values are not contradictory. Unless a problem says otherwise, AP Physics 1 lets you assume the reference frame is inertial: it is not accelerating or rotating relative to another inertial frame.