1.5 Vectors and Motion in Two Dimensions
- Syllabus
- 2024
- Topic
- 1.5
- Level
- —
Choose perpendicular x and y axes. A vector A can be replaced by components Ax and Ay whose vector sum is the original vector.
| If θ is measured from the +x-axis | Relationship |
|---|---|
| Adjacent component | Ax=Acosθ |
| Opposite component | Ay=Asinθ |
| Reconstruct magnitude | A=Ax2+Ay2 |
| Reconstruct direction | tanθ=Ay/Ax |
Hypothetical example: a 10N vector points 30∘ above +x. Then Ax=(10)cos30∘=8.66N and Ay=(10)sin30∘=5.00N. Check: 8.662+5.002=10.0N.
The trigonometric magnitudes do not replace the coordinate signs. Determine each sign from the vector’s direction relative to the chosen axes. Components are simultaneous parts of one vector—not two vectors applied one after the other.
Resolve position, velocity and acceleration into perpendicular components. Analyze the x and y motions separately with one-dimensional kinematics, then combine them at the same time t.
| Projectile component | Acceleration | Consequence |
|---|---|---|
| Horizontal x | ax=0 | vx is constant and Δx=vxt |
| Vertical y | ay=−g if up is positive | vy changes at a constant rate |
Hypothetical example: a projectile launches horizontally at vx=6ms−1 from 20m above the ground. With up positive and g=10ms−2, −20=21(−10)t2, so t=2s. During that same time, Δx=(6)(2)=12m.
Zero horizontal acceleration does not mean zero horizontal velocity. The components evolve independently under their own accelerations, but they are synchronized by the same time interval and together form one curved trajectory.