1.5 Vectors and Motion in Two Dimensions

Syllabus
2024
Topic
1.5
Level

Learning objectives

A vector is the resultant of its perpendicular components

Choose perpendicular axes

Choose perpendicular xx and yy axes. A vector A\vec A can be replaced by components AxA_x and AyA_y whose vector sum is the original vector.

Resolve and reconstruct

If θ\theta is measured from the +x-axis Relationship
Adjacent component Ax=AcosθA_x=A\cos\theta
Opposite component Ay=AsinθA_y=A\sin\theta
Reconstruct magnitude A=Ax2+Ay2A=\sqrt{A_x^2+A_y^2}
Reconstruct direction tanθ=Ay/Ax\tan\theta=A_y/A_x

Calculate both components

Hypothetical example: a 10N10\,\mathrm{N} vector points 3030^\circ above +x. Then Ax=(10)cos30=8.66NA_x=(10)\cos30^\circ=8.66\,\mathrm{N} and Ay=(10)sin30=5.00NA_y=(10)\sin30^\circ=5.00\,\mathrm{N}. Check: 8.662+5.002=10.0N\sqrt{8.66^2+5.00^2}=10.0\,\mathrm{N}.

Keep coordinate signs

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.

Two-dimensional motion is two synchronized one-dimensional motions

Separate the components

Resolve position, velocity and acceleration into perpendicular components. Analyze the xx and yy motions separately with one-dimensional kinematics, then combine them at the same time tt.

Compare horizontal and vertical motion

Projectile component Acceleration Consequence
Horizontal xx ax=0a_x=0 vxv_x is constant and Δx=vxt\Delta x=v_xt
Vertical yy ay=ga_y=-g if up is positive vyv_y changes at a constant rate

Use one shared time

Hypothetical example: a projectile launches horizontally at vx=6ms1v_x=6\,\mathrm{m\,s^{-1}} from 20m20\,\mathrm{m} above the ground. With up positive and g=10ms2g=10\,\mathrm{m\,s^{-2}}, 20=12(10)t2-20=\tfrac12(-10)t^2, so t=2st=2\,\mathrm{s}. During that same time, Δx=(6)(2)=12m\Delta x=(6)(2)=12\,\mathrm{m}.

Recombine the story

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.