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Chapter 12

Vectors and Advanced Mathematics Topics

Teacher Service Commission past exam questions

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1 question set from this chapter. Most repeated first.

  • 2081 · Subjective Questions · 1+4 marks

a) State and explain parallelogram law of vector addition. Derive the magnitude and direction of the resultant vector. b) Differentiate scalar product from the vector product of two vectors with suitable examples.

Answer

a) Parallelogram Law of Vector Addition

Statement: If two vectors acting simultaneously at a point are represented in magnitude and direction by the two adjacent sides of a parallelogram drawn from a point, then their resultant is represented in magnitude and direction by the diagonal of the parallelogram passing through that point.

Explanation: Let two vectors P⃗\vec{P} and Q⃗\vec{Q} act at a point O, inclined at an angle θ\theta. They are represented by the sides OA and OB of a parallelogram OACB. The resultant R⃗\vec{R} is represented by the diagonal OC.

Derivation of magnitude:

Drop a perpendicular from C on the extended line of OA, meeting it at N. In right-angled triangle ONC:

  • ON=OA+AN=P+Qcos⁡θON = OA + AN = P + Q\cos\theta
  • CN=Qsin⁡θCN = Q\sin\theta
  • OC2=ON2+CN2OC^2 = ON^2 + CN^2

R2=(P+Qcos⁡θ)2+(Qsin⁡θ)2R^2 = (P + Q\cos\theta)^2 + (Q\sin\theta)^2 R2=P2+2PQcos⁡θ+Q2cos⁡2θ+Q2sin⁡2θR^2 = P^2 + 2PQ\cos\theta + Q^2\cos^2\theta + Q^2\sin^2\theta R2=P2+Q2+2PQcos⁡θR^2 = P^2 + Q^2 + 2PQ\cos\theta

R=P2+Q2+2PQcos⁡θ\boxed{R = \sqrt{P^2 + Q^2 + 2PQ\cos\theta}}

Derivation of direction:

Let the resultant make an angle α\alpha with P⃗\vec{P}. In triangle ONC:

tan⁡α=CNON=Qsin⁡θP+Qcos⁡θ\tan\alpha = \frac{CN}{ON} = \frac{Q\sin\theta}{P + Q\cos\theta}

α=tan⁡−1(Qsin⁡θP+Qcos⁡θ)\boxed{\alpha = \tan^{-1}\left(\frac{Q\sin\theta}{P + Q\cos\theta}\right)}

Special cases:

  • When θ=0°\theta = 0°: R=P+QR = P + Q (maximum)
  • When θ=180°\theta = 180°: R=P−QR = P - Q (minimum)
  • When θ=90°\theta = 90°: R=P2+Q2R = \sqrt{P^2 + Q^2}

b) Difference between Scalar Product and Vector Product

Scalar (Dot) ProductVector (Cross) Product
A⃗⋅B⃗=ABcos⁡θ\vec{A}\cdot\vec{B} = AB\cos\thetaA⃗×B⃗=ABsin⁡θ n^\vec{A}\times\vec{B} = AB\sin\theta\,\hat{n}
Result is a scalar quantityResult is a vector quantity
Commutative: A⃗⋅B⃗=B⃗⋅A⃗\vec{A}\cdot\vec{B} = \vec{B}\cdot\vec{A}Not commutative: A⃗×B⃗=−B⃗×A⃗\vec{A}\times\vec{B} = -\vec{B}\times\vec{A}
Zero when vectors are perpendicular (θ=90°\theta = 90°)Zero when vectors are parallel or antiparallel (θ=0°\theta = 0° or 180°180°)
Follows distributive lawFollows distributive law
Direction is not requiredDirection is perpendicular to the plane of the two vectors

Examples:

  • Scalar product: Work done W=F⃗⋅d⃗=Fdcos⁡θW = \vec{F}\cdot\vec{d} = Fd\cos\theta (a scalar); Power P=F⃗⋅v⃗P = \vec{F}\cdot\vec{v}.
  • Vector product: Torque τ⃗=r⃗×F⃗\vec{\tau} = \vec{r}\times\vec{F}; angular momentum L⃗=r⃗×p⃗\vec{L} = \vec{r}\times\vec{p}; magnetic force F⃗=q(v⃗×B⃗)\vec{F} = q(\vec{v}\times\vec{B}).

Answer checked by Claude Haiku · Oct 21, 2026

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