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ISC 2027
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Vectors

5 articles27 formulas26 ways the board asks it
MATScalar (Dot) Product

Scalar (Dot) Product, Angle & Projection

The scalar (dot) product combines two vectors into a number: a⃗⋅b⃗=∣a⃗∣ ∣b⃗∣cos⁡θ\vec{a}\cdot\vec{b}=|\vec{a}|\,|\vec{b}|\cos\theta. It measures alignment, so it gives the angle between vectors, tests perpendicularity, and yields the projection of one vector onto another.

ISC examines it through angle-finding, perpendicularity conditions for an unknown, scalar projections, and work-done-by-a-force problems.

Dot product (definition)
a⃗⋅b⃗=∣a⃗∣ ∣b⃗∣cos⁡θ\vec{a}\cdot\vec{b} = |\vec{a}|\,|\vec{b}|\cos\theta
θ\theta is the angle between a⃗\vec{a} and b⃗\vec{b}, 0≤θ≤π0 \le \theta \le \pi.
Dot product (components)
a⃗⋅b⃗=a1b1+a2b2+a3b3\vec{a}\cdot\vec{b} = a_1 b_1 + a_2 b_2 + a_3 b_3
a⃗=a1i^+a2j^+a3k^\vec{a}=a_1\hat{i}+a_2\hat{j}+a_3\hat{k}, b⃗=b1i^+b2j^+b3k^\vec{b}=b_1\hat{i}+b_2\hat{j}+b_3\hat{k}.
Angle between vectors
cos⁡θ=a⃗⋅b⃗∣a⃗∣ ∣b⃗∣\cos\theta = \dfrac{\vec{a}\cdot\vec{b}}{|\vec{a}|\,|\vec{b}|}
Both vectors nonzero; θ=cos⁡−1\theta = \cos^{-1} of the right side, θ∈[0,π]\theta \in [0,\pi].
Perpendicularity condition
a⃗⊥b⃗  ⟺  a⃗⋅b⃗=0\vec{a} \perp \vec{b} \iff \vec{a}\cdot\vec{b} = 0
Holds for nonzero a⃗,b⃗\vec{a},\vec{b}; gives an equation for an unknown component.
Scalar projection of a on b
projb⃗ a⃗=a⃗⋅b⃗∣b⃗∣\text{proj}_{\vec{b}}\,\vec{a} = \dfrac{\vec{a}\cdot\vec{b}}{|\vec{b}|}
Scalar component of a⃗\vec{a} along b⃗\vec{b}; the vector projection is this times b⃗∣b⃗∣\dfrac{\vec{b}}{|\vec{b}|}.
Work done by a force
W=F⃗⋅d⃗W = \vec{F}\cdot\vec{d}
F⃗\vec{F} is the constant force, d⃗=AB⃗\vec{d}=\vec{AB} is the displacement; WW is in joules.
  • The dot product is commutative: a⃗⋅b⃗=b⃗⋅a⃗\vec{a}\cdot\vec{b}=\vec{b}\cdot\vec{a}, and distributive over addition.
  • a⃗⋅a⃗=∣a⃗∣2\vec{a}\cdot\vec{a}=|\vec{a}|^2, so the magnitude is ∣a⃗∣=a⃗⋅a⃗|\vec{a}|=\sqrt{\vec{a}\cdot\vec{a}}.
  • For the standard basis: i^⋅i^=j^⋅j^=k^⋅k^=1\hat{i}\cdot\hat{i}=\hat{j}\cdot\hat{j}=\hat{k}\cdot\hat{k}=1 and i^⋅j^=j^⋅k^=k^⋅i^=0\hat{i}\cdot\hat{j}=\hat{j}\cdot\hat{k}=\hat{k}\cdot\hat{i}=0.
  • The sign of a⃗⋅b⃗\vec{a}\cdot\vec{b} tells the angle type: positive means acute, zero means right angle, negative means obtuse.
  • Scalar projection can be negative (when θ\theta is obtuse); it is a signed length, not a magnitude.
  • To find work done, first compute the displacement d⃗=AB⃗=b⃗−a⃗\vec{d}=\vec{AB}=\vec{b}-\vec{a} (position of BB minus position of AA), then take the dot product with F⃗\vec{F}.
  • The projection of a⃗\vec{a} on b⃗\vec{b} divides by ∣b⃗∣|\vec{b}| (the vector projected onto), not by ∣a⃗∣|\vec{a}|.
Where the marks go
  • Dividing by ∣a⃗∣|\vec{a}| instead of ∣b⃗∣|\vec{b}| when finding the projection of a⃗\vec{a} on b⃗\vec{b}.
  • Forgetting that θ\theta from cos⁡−1\cos^{-1} lies in [0,π][0,\pi], so a negative cosine gives an obtuse angle, not a sign to discard.
  • Treating the dot product as a vector; the result is a scalar, so writing it with i^,j^,k^\hat{i},\hat{j},\hat{k} is wrong.
  • Using the position vectors a⃗,b⃗\vec{a},\vec{b} directly as the displacement in work problems instead of the difference b⃗−a⃗\vec{b}-\vec{a}.
How the board asks it
  • Numericala⃗⋅b⃗=∣a⃗∣∣b⃗∣cos⁡θ\vec{a}\cdot\vec{b}=|\vec{a}||\vec{b}|\cos\theta
    Find the angle between the vectors a⃗=2i^−j^+3k^\vec{a}=2\hat{i}-\hat{j}+3\hat{k} and b⃗=i^+2j^−k^\vec{b}=\hat{i}+2\hat{j}-\hat{k}.
  • Numericalperpendicularity condition a⃗⋅b⃗=0\vec{a}\cdot\vec{b}=0
    Find the value of λ\lambda for which the vectors a⃗=λi^+2j^+k^\vec{a}=\lambda\hat{i}+2\hat{j}+\hat{k} and b⃗=4i^−9j^+2k^\vec{b}=4\hat{i}-9\hat{j}+2\hat{k} are perpendicular to each other.
  • Numericalscalar projection a⃗⋅b⃗∣b⃗∣\dfrac{\vec{a}\cdot\vec{b}}{|\vec{b}|}
    Find the scalar projection of the vector a⃗=i^+3j^+7k^\vec{a}=\hat{i}+3\hat{j}+7\hat{k} on the vector b⃗=7i^−j^+8k^\vec{b}=7\hat{i}-\hat{j}+8\hat{k}.
  • Numericala⃗⋅a⃗=∣a⃗∣2\vec{a}\cdot\vec{a}=|\vec{a}|^2 and distributivity
    If ∣a⃗∣=3|\vec{a}|=3, ∣b⃗∣=4|\vec{b}|=4 and a⃗⋅b⃗=6\vec{a}\cdot\vec{b}=6, evaluate (2a⃗−b⃗)⋅(a⃗+3b⃗)(2\vec{a}-\vec{b})\cdot(\vec{a}+3\vec{b}).
  • Derive / prove∣a⃗±b⃗∣2=∣a⃗∣2±2a⃗⋅b⃗+∣b⃗∣2|\vec{a}\pm\vec{b}|^2=|\vec{a}|^2\pm 2\vec{a}\cdot\vec{b}+|\vec{b}|^2
    If a⃗\vec{a} and b⃗\vec{b} are two vectors such that ∣a⃗+b⃗∣=∣a⃗−b⃗∣|\vec{a}+\vec{b}|=|\vec{a}-\vec{b}|, prove that a⃗\vec{a} is perpendicular to b⃗\vec{b}.
  • Numericalwork F⃗⋅d⃗\vec{F}\cdot\vec{d} with d⃗=b⃗−a⃗\vec{d}=\vec{b}-\vec{a}
    A constant force F⃗=3i^+2j^−4k^\vec{F}=3\hat{i}+2\hat{j}-4\hat{k} acts on a particle that is displaced from the point A(1,0,2)A(1,0,2) to the point B(4,3,−1)B(4,3,-1). Calculate the work done by the force.

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Written for Sublevo. Question text quoted anywhere in these notes is the Council’s and carries its year and paper; the board’s own diagrams are not reproduced.