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Physics · Ch 2 — Kinematics

Scalar Product of Two Vectors

2.5.1

Scalar Product of Two Vectors

The scalar product (or dot product) of two vectors combines them to produce an ordinary number (a scalar), not another vector — hence the name. For vectors A⃗\vec A and B⃗\vec B with angle θ\theta between them,

A⃗⋅B⃗=ABcos⁡θ\vec A \cdot \vec B = AB\cos\theta

Properties:

  1. A⃗⋅B⃗\vec A\cdot\vec B is always a scalar; it is positive when θ\theta is acute (<90°<90°) and negative when θ\theta is obtuse (90°<θ<180°90°<\theta<180°).
  2. It is commutative: A⃗⋅B⃗=B⃗⋅A⃗\vec A\cdot\vec B = \vec B\cdot\vec A.
  3. It is distributive over addition: A⃗⋅(B⃗+C⃗)=A⃗⋅B⃗+A⃗⋅C⃗\vec A\cdot(\vec B+\vec C) = \vec A\cdot\vec B + \vec A\cdot\vec C.
  4. The angle between two vectors can be recovered from their dot product: θ=cos⁡−1 ⁣(A⃗⋅B⃗AB)\theta = \cos^{-1}\!\left(\dfrac{\vec A\cdot\vec B}{AB}\right).
  5. Maximum when cos⁡θ=1\cos\theta=1, i.e. θ=0°\theta=0° (parallel vectors): (A⃗⋅B⃗)max=AB(\vec A\cdot\vec B)_{max} = AB.
  6. Minimum (most negative) when cos⁡θ=−1\cos\theta=-1, i.e. θ=180°\theta=180° (anti-parallel vectors): (A⃗⋅B⃗)min=−AB(\vec A\cdot\vec B)_{min} = -AB.
  7. If A⃗⊥B⃗\vec A \perp \vec B, then A⃗⋅B⃗=0\vec A\cdot\vec B = 0 (since cos⁡90°=0\cos90°=0) — this is exactly how orthogonality (perpendicularity) of two vectors is tested/deduced: compute the dot product; if it comes out to zero, the vectors are perpendicular.
  8. Self-dot product: A⃗⋅A⃗=AAcos⁡0°=A2\vec A\cdot\vec A = AA\cos0° = A^2, so the magnitude can also be written A=A⃗⋅A⃗A = \sqrt{\vec A\cdot\vec A}.
  9. For any unit vector, n^⋅n^=1×1×cos⁡0°=1\hat n\cdot\hat n = 1\times1\times\cos0° = 1; in particular i^⋅i^=j^⋅j^=k^⋅k^=1\hat i\cdot\hat i=\hat j\cdot\hat j=\hat k\cdot\hat k=1.
  10. Since i^,j^,k^\hat i,\hat j,\hat k are mutually perpendicular, i^⋅j^=j^⋅k^=k^⋅i^=0\hat i\cdot\hat j=\hat j\cdot\hat k=\hat k\cdot\hat i=0.
  11. In component form:

A⃗⋅B⃗=AxBx+AyBy+AzBz\vec A\cdot\vec B = A_xB_x + A_yB_y + A_zB_z

(every cross term like Axi^⋅Byj^A_x\hat i\cdot B_y\hat j vanishes because i^⋅j^=0\hat i\cdot\hat j=0). …