Concept understanding — Applications of Dot and Cross Product
The dot product a⋅b=∣a∣∣b∣cosθ and cross product a×b (magnitude ∣a∣∣b∣sinθ, direction perpendicular to both) are not just formulas — placed carefully, they reprove classical geometry theorems and compute two real mechanical quantities.
Vector proofs in geometry and trigonometry. The standard technique: put a convenient point (a triangle's vertex, a circle's centre) at the origin, write every other point as a position vector, and express every needed segment as a difference of position vectors. Then:
Perpendicularity is proved by showing a dot product is 0. E.g. if O is a circle's centre and M is the midpoint of chord AB (position vectors a,b with ∣a∣=∣b∣=r), then OM=2a+b and AB=b−a, and OM⋅AB=21(∣b∣2−∣a∣2)=0.
Equal lengths / rectangles come from expanding ∣p±q∣2=∣p∣2±2p⋅q+∣q∣2 and comparing.
Areas come from area of a parallelogram=∣p×q∣ for adjacent sides p,q; a triangle is half that, and a general quadrilateral with diagonals d1,d2 has area 21∣d1×d2∣ (proved by splitting along one diagonal, since the two triangles on either side add — same-sense cross products — instead of subtracting).
Compound-angle identities (cos(α∓β), sin(α±β)) drop out of dotting or crossing two unit vectors i^cosα+j^sinα and i^cosβ±j^sinβ placed at angles α,±β to the x-axis. …
Part (i) expands the cross product (a−d)×(b−c) and shows it vanishes using the two given vector conditions; part (ii) finds direction cosines from direction ratios via the distance formula.
(i)
Given: a×b=c×d …(1) and a×c=b×d …(2)
Expand (a−d)×(b−c)=a×b−a×c−d×b+d×c
Rewrite using anti-commutativity of the cross product (−d×b=b×d and d×c=−c×d):
(a−d)×(b−c)=a×b−a×c+b×d−c×d
Substitute (1) (a×b=c×d), so those two terms cancel:
(a−d)×(b−c)=−a×c+b×d