MHT-CET Maths · Vectors

Scalar Triple Product, Coplanarity, and Volume

The single number [a b c] = a·(b×c) — the signed volume of the box on three vectors. It is zero exactly when they are coplanar, its modulus is the parallelepiped volume, and it powers the chapter's hardest pool: volumes, coplanarity, and the vector triple product.

Why this matters

At 56 PYQs this is the chapter's BIGGEST subtopic and its hardest — about 77% are rated HARD. The scalar triple product [a b c] is the workhorse: it is the signed volume of the parallelepiped, the modulus is the actual volume, one-sixth of it is the tetrahedron volume, and it vanishes precisely when the three vectors are coplanar. The same determinant drives parameter-finding (coplanarity), min/max volume problems, and the linearity identities like [a+b b+c c+a] = 2[a b c]; the vector triple product (BAC-CAB rule) finishes the set with angle and orthogonal-coplanar problems. Master the determinant, the cyclic/sign rules, and BAC-CAB and the chapter's HARD tail collapses.

Concept 1 of 11

The scalar triple product — dot-cross and determinant form

Intuition

The scalar triple product takes THREE vectors and returns a single NUMBER: dot one vector into the cross product of the other two. You almost never compute it from the geometry — you write the three vectors as the rows of a 3x3 determinant and evaluate it. Geometrically that number is the signed volume of the box (parallelepiped) built on the three vectors.

Definition

For a=a1i^+a2j^+a3k^\vec{a} = a_1\hat{i}+a_2\hat{j}+a_3\hat{k}, b=b1i^+b2j^+b3k^\vec{b} = b_1\hat{i}+b_2\hat{j}+b_3\hat{k}, c=c1i^+c2j^+c3k^\vec{c} = c_1\hat{i}+c_2\hat{j}+c_3\hat{k}:

  • Notation: [a b c]=a(b×c)[\vec{a}\ \vec{b}\ \vec{c}] = \vec{a}\cdot(\vec{b}\times\vec{c}) — a single scalar
  • Determinant form (the workhorse): [a b c]=a1a2a3b1b2b3c1c2c3[\vec{a}\ \vec{b}\ \vec{c}] = \begin{vmatrix} a_1 & a_2 & a_3 \\ b_1 & b_2 & b_3 \\ c_1 & c_2 & c_3 \end{vmatrix}
  • Dot-cross interchange: a(b×c)=(a×b)c\vec{a}\cdot(\vec{b}\times\vec{c}) = (\vec{a}\times\vec{b})\cdot\vec{c} — the dot and cross can swap places without changing the value
  • Geometric meaning: [a b c][\vec{a}\ \vec{b}\ \vec{c}] is the SIGNED volume of the parallelepiped with edge vectors a,b,c\vec{a}, \vec{b}, \vec{c}

Scalar triple product as a determinant

[a b c]=a(b×c)=a1a2a3b1b2b3c1c2c3[\vec{a}\ \vec{b}\ \vec{c}] = \vec{a}\cdot(\vec{b}\times\vec{c}) = \begin{vmatrix} a_1 & a_2 & a_3 \\ b_1 & b_2 & b_3 \\ c_1 & c_2 & c_3 \end{vmatrix}
  • Rowsthe components of a,b,c\vec{a}, \vec{b}, \vec{c} in order
  • (a×b)c(\vec{a}\times\vec{b})\cdot\vec{c}equal value — dot and cross interchange
  • [i^ j^ k^][\hat{i}\ \hat{j}\ \hat{k}]=1= 1, the unit box

Worked example

Evaluate [a b c][\vec{a}\ \vec{b}\ \vec{c}] for a=i^+2j^+k^\vec{a} = \hat{i} + 2\hat{j} + \hat{k}, b=2i^j^+3k^\vec{b} = 2\hat{i} - \hat{j} + 3\hat{k} and c=i^+k^\vec{c} = \hat{i} + \hat{k}.
  1. Stack the components as rows: 121213101\begin{vmatrix} 1 & 2 & 1 \\ 2 & -1 & 3 \\ 1 & 0 & 1 \end{vmatrix}.
  2. Expand along the first row: 1[(1)(1)(3)(0)]2[(2)(1)(3)(1)]+1[(2)(0)(1)(1)]1\cdot[(-1)(1) - (3)(0)] - 2\cdot[(2)(1) - (3)(1)] + 1\cdot[(2)(0) - (-1)(1)].
  3. Simplify: 1(1)2(1)+1(1)=1+2+1=21\cdot(-1) - 2\cdot(-1) + 1\cdot(1) = -1 + 2 + 1 = 2.
Answer:[a b c]=2[\vec{a}\ \vec{b}\ \vec{c}] = 2
Practice this concept4 quick reps

Practice — Level 1 (4 reps)

Quick reps to lock in the method. Try each, then check.

  1. 1.
    Write [a b c][\vec{a}\ \vec{b}\ \vec{c}] as a dot-cross.
  2. 2.
    [i^ j^ k^]=?[\hat{i}\ \hat{j}\ \hat{k}] = ?
  3. 3.
    a(b×c)\vec{a}\cdot(\vec{b}\times\vec{c}) equals which other dot-cross?
  4. 4.
    The scalar triple product is a number or a vector?

The scalar triple product is a SCALAR

[a b c]=a(b×c)[\vec{a}\ \vec{b}\ \vec{c}] = \vec{a}\cdot(\vec{b}\times\vec{c}) is a single number. The vector triple product a×(b×c)\vec{a}\times(\vec{b}\times\vec{c}) is a VECTOR. Identify which one the question asks for before choosing an identity.

Dot and cross can swap, but keep the order of the three vectors

a(b×c)=(a×b)c\vec{a}\cdot(\vec{b}\times\vec{c}) = (\vec{a}\times\vec{b})\cdot\vec{c} — moving the dot/cross is free. But swapping two of the three vectors themselves flips the sign (see the cyclic-and-sign concept next).

Concept 2 of 11

Cyclic and sign properties of the scalar triple product

Intuition

Rotating the three vectors round in a cycle leaves the scalar triple product unchanged; swapping any two of them flips its sign. And if any vector repeats, the box is flat — the product is zero. These three rules let you simplify almost any [a b c] expression before touching a determinant.

Definition

For any a,b,c\vec{a}, \vec{b}, \vec{c}:

  • Cyclic (rotation is free): [a b c]=[b c a]=[c a b][\vec{a}\ \vec{b}\ \vec{c}] = [\vec{b}\ \vec{c}\ \vec{a}] = [\vec{c}\ \vec{a}\ \vec{b}]
  • Swap flips the sign: [a b c]=[b a c]=[a c b][\vec{a}\ \vec{b}\ \vec{c}] = -[\vec{b}\ \vec{a}\ \vec{c}] = -[\vec{a}\ \vec{c}\ \vec{b}]
  • Repeated vector ⇒ zero: [a a b]=0[\vec{a}\ \vec{a}\ \vec{b}] = 0 (two equal rows make the determinant vanish)
  • Linearity in each slot: [αu+βv  b  c]=α[u b c]+β[v b c][\alpha\vec{u}+\beta\vec{v}\ \ \vec{b}\ \ \vec{c}] = \alpha[\vec{u}\ \vec{b}\ \vec{c}] + \beta[\vec{v}\ \vec{b}\ \vec{c}]

Cyclic and swap rules

[a b c]=[b c a]=[c a b]=[b a c][\vec{a}\ \vec{b}\ \vec{c}] = [\vec{b}\ \vec{c}\ \vec{a}] = [\vec{c}\ \vec{a}\ \vec{b}] = -[\vec{b}\ \vec{a}\ \vec{c}]
  • Cyclic rotationabca\vec{a}\to\vec{b}\to\vec{c}\to\vec{a}: value unchanged
  • One swapvalue negated
  • Repeated rowvalue =0= 0

Worked example

Simplify [a b c]+[b c a][b a c][\vec{a}\ \vec{b}\ \vec{c}] + [\vec{b}\ \vec{c}\ \vec{a}] - [\vec{b}\ \vec{a}\ \vec{c}].
  1. Cyclic: [b c a]=[a b c][\vec{b}\ \vec{c}\ \vec{a}] = [\vec{a}\ \vec{b}\ \vec{c}].
  2. One swap: [b a c]=[a b c][\vec{b}\ \vec{a}\ \vec{c}] = -[\vec{a}\ \vec{b}\ \vec{c}], so [b a c]=+[a b c]-[\vec{b}\ \vec{a}\ \vec{c}] = +[\vec{a}\ \vec{b}\ \vec{c}].
  3. Total: [a b c]+[a b c]+[a b c]=3[a b c][\vec{a}\ \vec{b}\ \vec{c}] + [\vec{a}\ \vec{b}\ \vec{c}] + [\vec{a}\ \vec{b}\ \vec{c}] = 3[\vec{a}\ \vec{b}\ \vec{c}].
Answer:3[a b c]3[\vec{a}\ \vec{b}\ \vec{c}]
Practice this concept4 quick reps

Practice — Level 1 (4 reps)

Quick reps to lock in the method. Try each, then check.

  1. 1.
    [b c a]=?[\vec{b}\ \vec{c}\ \vec{a}] = ? in terms of [a b c][\vec{a}\ \vec{b}\ \vec{c}].
  2. 2.
    [a c b]=?[\vec{a}\ \vec{c}\ \vec{b}] = ?
  3. 3.
    [a a c]=?[\vec{a}\ \vec{a}\ \vec{c}] = ?
  4. 4.
    [2a b c]=?[2\vec{a}\ \vec{b}\ \vec{c}] = ?

Cyclic keeps the value; ANY single swap negates it

[a b c]=[b c a][\vec{a}\ \vec{b}\ \vec{c}] = [\vec{b}\ \vec{c}\ \vec{a}] (cyclic, same value), but [a c b]=[a b c][\vec{a}\ \vec{c}\ \vec{b}] = -[\vec{a}\ \vec{b}\ \vec{c}] (one swap, flipped). Lose track of a swap and your final λ\lambda comes out with the wrong sign.

A repeated vector kills the product — spot it early

Whenever expanding by linearity, any term that ends up with two identical vectors (like [a a c][\vec{a}\ \vec{a}\ \vec{c}]) is zero. Most coplanarity-combo problems are solved entirely by deleting these zero terms.

Concept 3 of 11

Computing the value of a scalar triple product

Intuition

Sometimes you compute [a b c] not from raw components but from magnitudes and a perpendicularity setup, or you must decide which variables it depends on. When one vector is perpendicular to the plane of the other two, the box is a clean prism and [a b c]=ab×c[\vec{a}\ \vec{b}\ \vec{c}] = |\vec{a}|\,|\vec{b}\times\vec{c}|. When the determinant simplifies to a constant, the answer is independent of the parameters in the vectors.

Definition

  • Perpendicular case: if a\vec{a} is perpendicular to both b\vec{b} and c\vec{c}, then a\vec{a} is parallel to b×c\vec{b}\times\vec{c}, so [a b c]=±ab×c=±abcsinθ[\vec{a}\ \vec{b}\ \vec{c}] = \pm|\vec{a}|\,|\vec{b}\times\vec{c}| = \pm|\vec{a}|\,|\vec{b}||\vec{c}|\sin\theta where θ\theta is the angle between b\vec{b} and c\vec{c}.
  • Independence: if the determinant of the component matrix reduces to a constant, [a b c][\vec{a}\ \vec{b}\ \vec{c}] does not depend on the parameters inside the vectors.
  • Magnitude relations: a datum like b×c|\vec{b}\times\vec{c}| fixes sinθ\sin\theta, and a relation b=2c+λa\vec{b} = 2\vec{c} + \lambda\vec{a} is solved by taking magnitudes: b2c2=λ2a2|\vec{b} - 2\vec{c}|^2 = \lambda^2|\vec{a}|^2.

STP when one vector is perpendicular to the other two

[a b c]=ab×c=abcsinθ[\vec{a}\ \vec{b}\ \vec{c}] = |\vec{a}|\,|\vec{b}\times\vec{c}| = |\vec{a}||\vec{b}||\vec{c}|\sin\theta
  • ab,ac\vec{a}\perp\vec{b}, \vec{a}\perp\vec{c}so ab×c\vec{a}\,\|\,\vec{b}\times\vec{c}
  • θ\thetaangle between b\vec{b} and c\vec{c}
  • sinθ\sin\thetafrom b×c=bcsinθ|\vec{b}\times\vec{c}| = |\vec{b}||\vec{c}|\sin\theta

Worked example

a\vec{a} is perpendicular to both b\vec{b} and c\vec{c}. If a=3|\vec{a}| = 3, b=2|\vec{b}| = 2, c=5|\vec{c}| = 5 and the angle between b\vec{b} and c\vec{c} is π6\frac{\pi}{6}, find [a b c][\vec{a}\ \vec{b}\ \vec{c}].
  1. ab\vec{a}\perp\vec{b} and ac\vec{a}\perp\vec{c} means a\vec{a} is parallel to b×c\vec{b}\times\vec{c}.
  2. So [a b c]=ab×c=abcsinθ[\vec{a}\ \vec{b}\ \vec{c}] = |\vec{a}|\,|\vec{b}\times\vec{c}| = |\vec{a}||\vec{b}||\vec{c}|\sin\theta.
  3. =325sinπ6=3012=15= 3\cdot 2\cdot 5\cdot\sin\frac{\pi}{6} = 30\cdot\tfrac{1}{2} = 15.
Answer:[a b c]=15[\vec{a}\ \vec{b}\ \vec{c}] = 15
Practice this conceptself-check · 4 quick reps

Try it yourself

a,b,c\vec{a}, \vec{b}, \vec{c} are mutually perpendicular with magnitudes 2,3,42, 3, 4. Find [a b c][\vec{a}\ \vec{b}\ \vec{c}] (take it positive).

Practice — Level 1 (4 reps)

Quick reps to lock in the method. Try each, then check.

  1. 1.
    If ab\vec{a}\perp\vec{b} and ac\vec{a}\perp\vec{c}, then [a b c]=?[\vec{a}\ \vec{b}\ \vec{c}] = ?
  2. 2.
    For mutually perpendicular a,b,c\vec{a}, \vec{b}, \vec{c}, [a b c]=?[\vec{a}\ \vec{b}\ \vec{c}] = ?
  3. 3.
    If a determinant reduces to a constant, the STP depends on its parameters?
  4. 4.
    b×c=bc?|\vec{b}\times\vec{c}| = |\vec{b}||\vec{c}|\,?

From the bank · past-year question

Example 3VectorsMODERATE
If a\vec{a} is perpendicular to b\vec{b} and c\vec{c}, a=2|\vec{a}|=2, b=3|\vec{b}|=3, c=4|\vec{c}|=4 and the angle between b\vec{b} and c\vec{c} is π3\frac{\pi}{3}, then [abc]=[\vec{a}\,\vec{b}\,\vec{c}] =

[Q117 · 16th May Shift 2 · 2023]

Perpendicular to BOTH means parallel to the cross product

If ab\vec{a}\perp\vec{b} and ac\vec{a}\perp\vec{c}, then a\vec{a} lies along b×c\vec{b}\times\vec{c}, so the box is a right prism and [a b c]=ab×c[\vec{a}\ \vec{b}\ \vec{c}] = |\vec{a}|\,|\vec{b}\times\vec{c}|. Don't try to plug a single sin\sin of the angle between a\vec{a} and b\vec{b} — the relevant angle is between b\vec{b} and c\vec{c}.

"Depends on x and y" — expand the determinant first

When the vectors carry parameters, compute [a b c][\vec{a}\ \vec{b}\ \vec{c}] as a determinant and simplify. It frequently collapses to a constant, meaning the answer is independent of every parameter — a deliberately surprising option.

Concept 4 of 11

Coplanarity of three vectors (and solving for a parameter)

Intuition

Three vectors lie in a common plane through the origin exactly when the box on them is flat — zero volume. So the test is simply [a b c]=0[\vec{a}\ \vec{b}\ \vec{c}] = 0: set the determinant to zero and solve for the unknown. It also detects how many values of a parameter make them coplanar, and a vector lying in the plane of two others satisfies the same equation.

Definition

a,b,c\vec{a}, \vec{b}, \vec{c} are coplanar     [a b c]=0\iff [\vec{a}\ \vec{b}\ \vec{c}] = 0, i.e. the determinant of their components is zero. If c\vec{c} lies in the plane of a\vec{a} and b\vec{b}, then [a b c]=0[\vec{a}\ \vec{b}\ \vec{c}] = 0 too. To find a parameter λ\lambda (or xx) that makes them coplanar, set the determinant equal to zero and solve the resulting equation; a parameter that appears squared can give two distinct real values.

Coplanarity criterion

a,b,c coplanar    a1a2a3b1b2b3c1c2c3=0\vec{a},\vec{b},\vec{c}\text{ coplanar} \iff \begin{vmatrix} a_1 & a_2 & a_3 \\ b_1 & b_2 & b_3 \\ c_1 & c_2 & c_3 \end{vmatrix} = 0
  • [a b c]=0[\vec{a}\ \vec{b}\ \vec{c}] = 0zero box volume ⇒ all three lie in one plane
  • Parametersolve the determinant-equals-zero equation for it

Worked example

Find λ\lambda so that a=i^+j^k^\vec{a} = \hat{i} + \hat{j} - \hat{k}, b=2i^j^+k^\vec{b} = 2\hat{i} - \hat{j} + \hat{k} and c=i^+λj^+3k^\vec{c} = \hat{i} + \lambda\hat{j} + 3\hat{k} are coplanar.
  1. Coplanar ⇒ [a b c]=0[\vec{a}\ \vec{b}\ \vec{c}] = 0: 1112111λ3=0\begin{vmatrix} 1 & 1 & -1 \\ 2 & -1 & 1 \\ 1 & \lambda & 3 \end{vmatrix} = 0.
  2. Expand along the first row: 1(3λ)1(61)+(1)(2λ+1)1\cdot(-3 - \lambda) - 1\cdot(6 - 1) + (-1)\cdot(2\lambda + 1).
  3. Simplify: (3λ)5(2λ+1)=93λ=0(-3 - \lambda) - 5 - (2\lambda + 1) = -9 - 3\lambda = 0.
  4. Solve: λ=3\lambda = -3.
Answer:λ=3\lambda = -3
Practice this conceptself-check · 4 quick reps

Try it yourself

For how many real values of λ\lambda are λi^+j^\lambda\hat{i} + \hat{j}, i^+λj^\hat{i} + \lambda\hat{j} and i^+j^+λk^\hat{i} + \hat{j} + \lambda\hat{k} coplanar?

Practice — Level 1 (4 reps)

Quick reps to lock in the method. Try each, then check.

  1. 1.
    Three vectors are coplanar iff [a b c]=?[\vec{a}\ \vec{b}\ \vec{c}] = ?
  2. 2.
    If c\vec{c} lies in the plane of a,b\vec{a}, \vec{b}, then [a b c]=?[\vec{a}\ \vec{b}\ \vec{c}] = ?
  3. 3.
    To find a coplanarity parameter, set the determinant equal to?
  4. 4.
    [i^ j^ (i^+j^)]=?[\hat{i}\ \hat{j}\ (\hat{i}+\hat{j})] = ? — coplanar?

From the bank · past-year question

Example 4VectorsMODERATE
If the vectors pi^+j^+k^,i^+qj^+k^p\hat{i}+\hat{j}+\hat{k},\hat{i}+q\hat{j}+\hat{k} and i^+j^+rk^ (pqr1)\hat{i}+\hat{j}+r\hat{k}\ (p\neq q\neq r\neq1) are coplanar, then the value of pqr(p+q+r)pqr-(p+q+r) is

[Q119 · 13th May Shift 2 · 2024]

Coplanar ⇒ STP = 0, NOT "two of them are parallel"

Three vectors coplanar means they fit in one plane; they need not be parallel to each other. A parallel pair also makes the STP zero, but it is a stronger, separate condition — don't confuse the two.

A squared parameter can give TWO coplanarity values

When the unknown appears as λ2\lambda^2 (e.g. λ2i^+-\lambda^2\hat{i}+\dots), the determinant-equals-zero equation can have two distinct real roots. Count carefully — "number of values of λ\lambda" questions hinge exactly on this.

Concept 5 of 11

Scalar triple product of linear combinations

Intuition

When the three slots of a scalar triple product are themselves sums of a,b,c\vec{a}, \vec{b}, \vec{c}, expand by linearity — every term with a repeated vector vanishes, leaving a clean multiple of [a b c][\vec{a}\ \vec{b}\ \vec{c}]. The pattern [a+b  b+c  c+a]=2[a b c][\vec{a}+\vec{b}\ \ \vec{b}+\vec{c}\ \ \vec{c}+\vec{a}] = 2[\vec{a}\ \vec{b}\ \vec{c}] is the signature case. More generally, the coefficient is a 3x3 determinant of the combination coefficients.

Definition

Expanding by linearity and deleting repeated-vector terms:

  • [a+b  b+c  c+a]=2[a b c][\vec{a}+\vec{b}\ \ \vec{b}+\vec{c}\ \ \vec{c}+\vec{a}] = 2[\vec{a}\ \vec{b}\ \vec{c}]
  • [ma+b  mb+c  mc+a]=(m3+1)[a b c][m\vec{a}+\vec{b}\ \ m\vec{b}+\vec{c}\ \ m\vec{c}+\vec{a}] = (m^3 + 1)[\vec{a}\ \vec{b}\ \vec{c}]
  • In general the new STP equals det(M)[a b c]\det(M)\,[\vec{a}\ \vec{b}\ \vec{c}], where MM is the 3x3 matrix of the combination coefficients.

If a,b,c\vec{a}, \vec{b}, \vec{c} are coplanar, [a b c]=0[\vec{a}\ \vec{b}\ \vec{c}] = 0 so every such combination is also zero.

Linear-combination identities

[a+b  b+c  c+a]=2[a b c][ma+b  mb+c  mc+a]=(m3+1)[a b c][\vec{a}+\vec{b}\ \ \vec{b}+\vec{c}\ \ \vec{c}+\vec{a}] = 2[\vec{a}\ \vec{b}\ \vec{c}] \qquad [m\vec{a}+\vec{b}\ \ m\vec{b}+\vec{c}\ \ m\vec{c}+\vec{a}] = (m^3+1)[\vec{a}\ \vec{b}\ \vec{c}]
  • Repeated-vector termsall vanish on expansion
  • Coefficient=det= \det of the combination-coefficient matrix

Worked example

Simplify [a+b  b+c  c+a][\vec{a}+\vec{b}\ \ \vec{b}+\vec{c}\ \ \vec{c}+\vec{a}] in terms of [a b c][\vec{a}\ \vec{b}\ \vec{c}].
  1. Expand the first slot by linearity: [a  b+c  c+a]+[b  b+c  c+a][\vec{a}\ \ \vec{b}+\vec{c}\ \ \vec{c}+\vec{a}] + [\vec{b}\ \ \vec{b}+\vec{c}\ \ \vec{c}+\vec{a}].
  2. Keep expanding and delete every term with a repeated vector (e.g. [a c c]=0[\vec{a}\ \vec{c}\ \vec{c}] = 0, [b b ]=0[\vec{b}\ \vec{b}\ \dots] = 0).
  3. The surviving terms are [a b c][\vec{a}\ \vec{b}\ \vec{c}] and [b c a]=[a b c][\vec{b}\ \vec{c}\ \vec{a}] = [\vec{a}\ \vec{b}\ \vec{c}], giving 2[a b c]2[\vec{a}\ \vec{b}\ \vec{c}].
Answer:2[a b c]2[\vec{a}\ \vec{b}\ \vec{c}]
Practice this conceptself-check · 4 quick reps

Try it yourself

If a,b,c\vec{a}, \vec{b}, \vec{c} are coplanar unit vectors, find [2ab  2bc  2ca][2\vec{a}-\vec{b}\ \ 2\vec{b}-\vec{c}\ \ 2\vec{c}-\vec{a}].

Practice — Level 1 (4 reps)

Quick reps to lock in the method. Try each, then check.

  1. 1.
    [a+b  b+c  c+a]=?[\vec{a}+\vec{b}\ \ \vec{b}+\vec{c}\ \ \vec{c}+\vec{a}] = ?
  2. 2.
    [3a+b  3b+c  3c+a]=?[3\vec{a}+\vec{b}\ \ 3\vec{b}+\vec{c}\ \ 3\vec{c}+\vec{a}] = ?
  3. 3.
    If a,b,c\vec{a},\vec{b},\vec{c} coplanar, [2ab ]=?[2\vec{a}-\vec{b}\ \dots] = ?
  4. 4.
    A term like [a a c][\vec{a}\ \vec{a}\ \vec{c}] contributes what to the expansion?

From the bank · past-year question

Example 5VectorsHARD
If a=a1i^+a2j^+a3k^\vec{a} = a_1\hat{i}+a_2\hat{j}+a_3\hat{k}, b=b1i^+b2j^+b3k^\vec{b} = b_1\hat{i}+b_2\hat{j}+b_3\hat{k}, c=c1i^+c2j^+c3k^\vec{c} = c_1\hat{i}+c_2\hat{j}+c_3\hat{k} and [3a+b,3b+c,3c+a]=λ[abc][3\vec{a}+\vec{b}, 3\vec{b}+\vec{c}, 3\vec{c}+\vec{a}] = \lambda[\vec{a}\,\vec{b}\,\vec{c}], then the value of λ\lambda is

[Q129 · 16th May Shift 2 · 2023]

[ma+b ]=(m3+1)[a b c][m\vec{a}+\vec{b}\ \dots] = (m^3+1)[\vec{a}\ \vec{b}\ \vec{c}], not m3m^3

The cyclic mm\,\cdot pattern gives m3+1m^3 + 1 — the extra +1+1 comes from the [b c a][\vec{b}\ \vec{c}\ \vec{a}] cross-term. So m=3m = 3 gives 2828, not 2727. Dropping the +1+1 is a deliberate distractor.

Track every sign through the swaps

Expansions like [a+2b+3c ][\vec{a}+2\vec{b}+3\vec{c}\ \dots] generate many cross-terms; a single mis-signed swap throws off the coefficient. Use cyclic to standardise every surviving term to [a b c][\vec{a}\ \vec{b}\ \vec{c}] before summing.

Concept 6 of 11

Volume of a parallelepiped (and min/max problems)

Intuition

The volume of the box (parallelepiped) on three edge vectors is the MODULUS of their scalar triple product — the sign just tells you the orientation. Set the determinant equal to a given volume to find an unknown component, or differentiate the determinant in a parameter to find where the volume is smallest or largest.

Definition

For edge vectors a,b,c\vec{a}, \vec{b}, \vec{c}:

  • Volume =[a b c]=det(component matrix)= |[\vec{a}\ \vec{b}\ \vec{c}]| = \left|\det\text{(component matrix)}\right|.
  • Find a component: set [a b c]=V|[\vec{a}\ \vec{b}\ \vec{c}]| = V (given) and solve.
  • Min/max in a parameter: write the determinant as a function V(m)V(m), set V(m)=0V'(m) = 0, and use the sign of V(m)V''(m) to classify minimum vs maximum.
  • The dihedral angle between two faces of a tetrahedron is the angle between the two face normals, each found as a cross product of edge vectors.

Parallelepiped volume

V=[a b c]=a1a2a3b1b2b3c1c2c3V = |[\vec{a}\ \vec{b}\ \vec{c}]| = \left|\begin{vmatrix} a_1 & a_2 & a_3 \\ b_1 & b_2 & b_3 \\ c_1 & c_2 & c_3 \end{vmatrix}\right|
  • |\cdot|modulus — volume is always non-negative
  • V(m)=0V'(m)=0stationary volume; VV'' sign decides min/max

Diagram · triple product = box volume (SVG, drag to rotate)

abc
[a b c] = a · (b × c) = 13.22 (signed volume of the box)

The box spanned by a, b, c has volume |[a b c]|. Painter's-ordered faces fake the solidity — edges don't truly hide behind nearer faces, which is the SVG limit this comparison is testing.

Worked example

Find the value of mm for which the volume of the parallelepiped on i^+mj^+k^\hat{i}+m\hat{j}+\hat{k}, j^+mk^\hat{j}+m\hat{k} and mi^+k^m\hat{i}+\hat{k} is minimum.
  1. Volume function: 1m101mm01=1(1)m(0m2)+1(0m)=m3m+1\begin{vmatrix} 1 & m & 1 \\ 0 & 1 & m \\ m & 0 & 1 \end{vmatrix} = 1(1) - m(0 - m^2) + 1(0 - m) = m^3 - m + 1.
  2. Take V(m)=m3m+1V(m) = m^3 - m + 1; set V(m)=3m21=0m=±13V'(m) = 3m^2 - 1 = 0 \Rightarrow m = \pm\frac{1}{\sqrt{3}}.
  3. V(m)=6mV''(m) = 6m: positive at m=13m = \frac{1}{\sqrt{3}}, so that gives the minimum.
Answer:m=13m = \dfrac{1}{\sqrt{3}}
Practice this conceptself-check · 4 quick reps

Try it yourself

Find the volume of the parallelepiped with edges a=i^\vec{a} = \hat{i}, b=j^\vec{b} = \hat{j} and c=i^+j^+2k^\vec{c} = \hat{i} + \hat{j} + 2\hat{k}.

Practice — Level 1 (4 reps)

Quick reps to lock in the method. Try each, then check.

  1. 1.
    Volume of the parallelepiped on a,b,c\vec{a}, \vec{b}, \vec{c}?
  2. 2.
    If [a b c]=7[\vec{a}\ \vec{b}\ \vec{c}] = -7, the volume is?
  3. 3.
    To find a min/max volume in mm, set what to zero?
  4. 4.
    Dihedral angle between two faces = angle between their?

From the bank · past-year question

Example 6VectorsHARD
The volume of parallelopiped formed by vectors i^+mj^+k^\hat{i} + m\hat{j} + \hat{k}, j^+mk^\hat{j} + m\hat{k} and mi^+k^m\hat{i} + \hat{k} becomes minimum when mm is

[Q113 · 2nd May Shift 1 · 2023]

Volume is the MODULUS — never a negative number

The scalar triple product can be negative (it is a SIGNED volume), but a physical volume is [a b c]|[\vec{a}\ \vec{b}\ \vec{c}]|. When a volume is given (e.g. 158 cu units), set the modulus equal to it, which may give two parameter values ±\pm.

Min vs max: check the second derivative

V(m)=0V'(m) = 0 at m=±13m = \pm\frac{1}{\sqrt{3}}, but only one is a minimum. V(m)=6m>0V''(m) = 6m > 0 at m=+13m = +\frac{1}{\sqrt{3}} (minimum) and <0< 0 at m=13m = -\frac{1}{\sqrt{3}} (maximum). The two questions share roots but want opposite answers.

Concept 7 of 11

Volume of a tetrahedron

Intuition

A tetrahedron is one-sixth of the parallelepiped on the same three edge vectors. So its volume is one-sixth the modulus of the scalar triple product of the three edges meeting at one vertex. Build the edges by subtracting the chosen vertex from the other three, then apply the formula.

Definition

For a tetrahedron with vertices A,B,C,DA, B, C, D, form the edge vectors from one vertex: AB,AC,AD\overrightarrow{AB}, \overrightarrow{AC}, \overrightarrow{AD}. Then Volume =16[AB AC AD]= \dfrac{1}{6}\,|[\overrightarrow{AB}\ \overrightarrow{AC}\ \overrightarrow{AD}]|. Setting this equal to a given volume yields an equation for an unknown coordinate.

Tetrahedron volume

V=16[AB AC AD]V = \tfrac{1}{6}\,\bigl|[\overrightarrow{AB}\ \overrightarrow{AC}\ \overrightarrow{AD}]\bigr|
  • 16\tfrac{1}{6}a tetrahedron is one-sixth of the parallelepiped
  • AB,AC,AD\overrightarrow{AB}, \overrightarrow{AC}, \overrightarrow{AD}three edges from the SAME vertex AA

Worked example

Find the volume of the tetrahedron with vertices A(0,0,0)A(0,0,0), B(2,0,0)B(2,0,0), C(0,3,0)C(0,3,0) and D(0,0,4)D(0,0,4).
  1. Edges from AA: AB=2i^\overrightarrow{AB} = 2\hat{i}, AC=3j^\overrightarrow{AC} = 3\hat{j}, AD=4k^\overrightarrow{AD} = 4\hat{k}.
  2. [AB AC AD]=200030004=24[\overrightarrow{AB}\ \overrightarrow{AC}\ \overrightarrow{AD}] = \begin{vmatrix} 2 & 0 & 0 \\ 0 & 3 & 0 \\ 0 & 0 & 4 \end{vmatrix} = 24.
  3. Volume =1624=4= \tfrac{1}{6}\cdot 24 = 4.
Answer:Volume =4= 4 cubic units
Practice this conceptself-check · 4 quick reps

Try it yourself

The volume of the tetrahedron with vertices A(1,1,1)A(1,1,1), B(2,1,1)B(2,1,1), C(1,3,1)C(1,3,1), D(1,1,5)D(1,1,5) is?

Practice — Level 1 (4 reps)

Quick reps to lock in the method. Try each, then check.

  1. 1.
    Tetrahedron volume from edges a,b,c\vec{a}, \vec{b}, \vec{c}?
  2. 2.
    A tetrahedron is what fraction of the parallelepiped on the same edges?
  3. 3.
    If [AB AC AD]=30[\overrightarrow{AB}\ \overrightarrow{AC}\ \overrightarrow{AD}] = 30, the volume is?
  4. 4.
    From vertices A,B,C,DA,B,C,D, which three edges do you use?

From the bank · past-year question

Example 7VectorsHARD
If the volume of tetrahedron whose vertices are A(1,6,10)A\equiv(1,-6,10), B(1,3,7)B\equiv(-1,-3,7), C(5,1,k)C\equiv(5,-1,k) and D(7,4,7)D\equiv(7,-4,7) is 11 cu. units, then the value of k is

[Q141 · 11th May Shift 1 · 2023]

The one-sixth is on the tetrahedron, not the parallelepiped

Tetrahedron volume =16[a b c]= \tfrac{1}{6}|[\vec{a}\ \vec{b}\ \vec{c}]|; the parallelepiped is the full [a b c]|[\vec{a}\ \vec{b}\ \vec{c}]|. Forgetting the 16\tfrac{1}{6} over-counts the volume six-fold — a classic distractor when a volume is given.

Build all three edges from the SAME vertex

Use AB,AC,AD\overrightarrow{AB}, \overrightarrow{AC}, \overrightarrow{AD} — all starting at AA. Mixing base points (e.g. AB,BC,\overrightarrow{AB}, \overrightarrow{BC}, \dots) gives the wrong determinant and a wrong unknown.

Concept 8 of 11

Reciprocal-basis identities and the STP-squared rule

Intuition

From a non-coplanar triple a,b,c\vec{a}, \vec{b}, \vec{c}, the vectors b×c[a b c]\dfrac{\vec{b}\times\vec{c}}{[\vec{a}\ \vec{b}\ \vec{c}]} and its cyclic partners form a "reciprocal" set that dots cleanly with the originals: each matched pair gives 11, each mismatched pair gives 00. That single fact collapses long-looking sums to small integers. A close relative is the identity [a×b  b×c  c×a]=[a b c]2[\vec{a}\times\vec{b}\ \ \vec{b}\times\vec{c}\ \ \vec{c}\times\vec{a}] = [\vec{a}\ \vec{b}\ \vec{c}]^2.

Definition

For non-coplanar a,b,c\vec{a}, \vec{b}, \vec{c}, set p=b×c[a b c]\vec{p} = \dfrac{\vec{b}\times\vec{c}}{[\vec{a}\ \vec{b}\ \vec{c}]}, q=c×a[a b c]\vec{q} = \dfrac{\vec{c}\times\vec{a}}{[\vec{a}\ \vec{b}\ \vec{c}]}, r=a×b[a b c]\vec{r} = \dfrac{\vec{a}\times\vec{b}}{[\vec{a}\ \vec{b}\ \vec{c}]}:

  • Matched pairs: ap=bq=cr=1\vec{a}\cdot\vec{p} = \vec{b}\cdot\vec{q} = \vec{c}\cdot\vec{r} = 1
  • Mismatched pairs: aq=ar=bp==0\vec{a}\cdot\vec{q} = \vec{a}\cdot\vec{r} = \vec{b}\cdot\vec{p} = \dots = 0 (the cross product is perpendicular to its own factors)
  • STP-squared rule: [a×b  b×c  c×a]=[a b c]2[\vec{a}\times\vec{b}\ \ \vec{b}\times\vec{c}\ \ \vec{c}\times\vec{a}] = [\vec{a}\ \vec{b}\ \vec{c}]^2

Reciprocal pairings and STP-squared

ap=bq=cr=1,aq=bp==0[a×b  b×c  c×a]=[a b c]2\vec{a}\cdot\vec{p} = \vec{b}\cdot\vec{q} = \vec{c}\cdot\vec{r} = 1, \quad \vec{a}\cdot\vec{q} = \vec{b}\cdot\vec{p} = \dots = 0 \qquad [\vec{a}\times\vec{b}\ \ \vec{b}\times\vec{c}\ \ \vec{c}\times\vec{a}] = [\vec{a}\ \vec{b}\ \vec{c}]^2
  • Matchedap=1\vec{a}\cdot\vec{p} = 1 etc.
  • Mismatchedaq=0\vec{a}\cdot\vec{q} = 0 (perpendicularity)
  • STP-squaredcross-of-pairs box =[a b c]2= [\vec{a}\ \vec{b}\ \vec{c}]^2

Worked example

With p=b×c[a b c]\vec{p} = \dfrac{\vec{b}\times\vec{c}}{[\vec{a}\ \vec{b}\ \vec{c}]}, q=c×a[a b c]\vec{q} = \dfrac{\vec{c}\times\vec{a}}{[\vec{a}\ \vec{b}\ \vec{c}]}, r=a×b[a b c]\vec{r} = \dfrac{\vec{a}\times\vec{b}}{[\vec{a}\ \vec{b}\ \vec{c}]}, find ap+bq+cr\vec{a}\cdot\vec{p} + \vec{b}\cdot\vec{q} + \vec{c}\cdot\vec{r}.
  1. ap=a(b×c)[a b c]=[a b c][a b c]=1\vec{a}\cdot\vec{p} = \dfrac{\vec{a}\cdot(\vec{b}\times\vec{c})}{[\vec{a}\ \vec{b}\ \vec{c}]} = \dfrac{[\vec{a}\ \vec{b}\ \vec{c}]}{[\vec{a}\ \vec{b}\ \vec{c}]} = 1.
  2. By the same cyclic argument, bq=1\vec{b}\cdot\vec{q} = 1 and cr=1\vec{c}\cdot\vec{r} = 1.
  3. Sum =1+1+1=3= 1 + 1 + 1 = 3.
Answer:33
Practice this conceptself-check · 4 quick reps

Try it yourself

With the same p,q,r\vec{p}, \vec{q}, \vec{r}, evaluate aq+br+cp\vec{a}\cdot\vec{q} + \vec{b}\cdot\vec{r} + \vec{c}\cdot\vec{p}.

Practice — Level 1 (4 reps)

Quick reps to lock in the method. Try each, then check.

  1. 1.
    ab×c[a b c]=?\vec{a}\cdot\dfrac{\vec{b}\times\vec{c}}{[\vec{a}\ \vec{b}\ \vec{c}]} = ?
  2. 2.
    bb×c[a b c]=?\vec{b}\cdot\dfrac{\vec{b}\times\vec{c}}{[\vec{a}\ \vec{b}\ \vec{c}]} = ?
  3. 3.
    [a×b  b×c  c×a]=?[\vec{a}\times\vec{b}\ \ \vec{b}\times\vec{c}\ \ \vec{c}\times\vec{a}] = ?
  4. 4.
    2ap+bq+cr=?2\vec{a}\cdot\vec{p} + \vec{b}\cdot\vec{q} + \vec{c}\cdot\vec{r} = ?

From the bank · past-year question

Example 8VectorsMODERATE
Let a,b,c\vec{a},\vec{b},\vec{c} be three non-coplanar vectors and p,q,r\vec{p},\vec{q},\vec{r} defined by p=b×c[a b c], q=c×a[a b c], r=a×b[a b c]\vec{p}=\frac{\vec{b}\times\vec{c}}{[\vec{a}\ \vec{b}\ \vec{c}]},\ \vec{q}=\frac{\vec{c}\times\vec{a}}{[\vec{a}\ \vec{b}\ \vec{c}]},\ \vec{r}=\frac{\vec{a}\times\vec{b}}{[\vec{a}\ \vec{b}\ \vec{c}]}, then the value of (a+b)p+(b+c)q+(c+a)r(\vec{a}+\vec{b})\cdot\vec{p}+(\vec{b}+\vec{c})\cdot\vec{q}+(\vec{c}+\vec{a})\cdot\vec{r} is equal to

[Q148 · 3rd May 2nd Shift · 2023]

Matched pairs are 1, mismatched pairs are 0

ab×c[a b c]=1\vec{a}\cdot\dfrac{\vec{b}\times\vec{c}}{[\vec{a}\ \vec{b}\ \vec{c}]} = 1, but ac×a[a b c]=0\vec{a}\cdot\dfrac{\vec{c}\times\vec{a}}{[\vec{a}\ \vec{b}\ \vec{c}]} = 0 because c×aa\vec{c}\times\vec{a}\perp\vec{a}. Read each dot pair to decide whether it survives — most of the terms in these sums vanish.

Cross-of-pairs box is the SQUARE, not the cube

[a×b  b×c  c×a]=[a b c]2[\vec{a}\times\vec{b}\ \ \vec{b}\times\vec{c}\ \ \vec{c}\times\vec{a}] = [\vec{a}\ \vec{b}\ \vec{c}]^2 — so the coefficient λ\lambda in λ[a b c]2\lambda[\vec{a}\ \vec{b}\ \vec{c}]^2 is 11, not 33 or 22.

Concept 9 of 11

Vector triple product (BAC-CAB rule)

Intuition

A triple product with TWO crosses returns a VECTOR, expanded by the BAC-CAB rule: a×(b×c)=(ac)b(ab)c\vec{a}\times(\vec{b}\times\vec{c}) = (\vec{a}\cdot\vec{c})\vec{b} - (\vec{a}\cdot\vec{b})\vec{c}. Read it as "outer-dot-far times near, minus outer-dot-near times far". The result lies in the plane of the two innermost vectors — a structural fact that powers most of the chapter's angle problems.

Definition

For any a,b,c\vec{a}, \vec{b}, \vec{c}:

  • a×(b×c)=(ac)b(ab)c\vec{a}\times(\vec{b}\times\vec{c}) = (\vec{a}\cdot\vec{c})\,\vec{b} - (\vec{a}\cdot\vec{b})\,\vec{c}
  • (a×b)×c=(ac)b(bc)a(\vec{a}\times\vec{b})\times\vec{c} = (\vec{a}\cdot\vec{c})\,\vec{b} - (\vec{b}\cdot\vec{c})\,\vec{a}
  • The vector triple product is NOT associative: a×(b×c)(a×b)×c\vec{a}\times(\vec{b}\times\vec{c}) \neq (\vec{a}\times\vec{b})\times\vec{c} in general — the two lie in different planes.

Equating a given expansion to a stated multiple of b\vec{b} and c\vec{c} lets you read off ab\vec{a}\cdot\vec{b} (hence the angle), since b,c\vec{b}, \vec{c} are independent.

BAC-CAB rule

a×(b×c)=(ac)b(ab)c\vec{a}\times(\vec{b}\times\vec{c}) = (\vec{a}\cdot\vec{c})\,\vec{b} - (\vec{a}\cdot\vec{b})\,\vec{c}
  • ac,ab\vec{a}\cdot\vec{c}, \vec{a}\cdot\vec{b}scalar coefficients
  • b,c\vec{b}, \vec{c}the plane the result lies in
  • Resultperpendicular to a\vec{a}, inside the b\vec{b}-c\vec{c} plane

Worked example

Three unit vectors satisfy a×(b×c)=12(b+c)\vec{a}\times(\vec{b}\times\vec{c}) = \dfrac{1}{2}(\vec{b} + \vec{c}) with b\vec{b} not parallel to c\vec{c}. Find the angle between a\vec{a} and b\vec{b}.
  1. BAC-CAB: (ac)b(ab)c=12b+12c(\vec{a}\cdot\vec{c})\vec{b} - (\vec{a}\cdot\vec{b})\vec{c} = \tfrac{1}{2}\vec{b} + \tfrac{1}{2}\vec{c}.
  2. Since b,c\vec{b}, \vec{c} are independent, match coefficients: ac=12\vec{a}\cdot\vec{c} = \tfrac{1}{2} and (ab)=12-(\vec{a}\cdot\vec{b}) = \tfrac{1}{2}, so ab=12\vec{a}\cdot\vec{b} = -\tfrac{1}{2}.
  3. Unit vectors: cosθ=ab=12\cos\theta = \vec{a}\cdot\vec{b} = -\tfrac{1}{2}, so θ=2π3\theta = \dfrac{2\pi}{3}.
Answer:θ=2π3\theta = \dfrac{2\pi}{3}
Practice this conceptself-check · 4 quick reps

Try it yourself

Using BAC-CAB, find a×(b×c)\vec{a}\times(\vec{b}\times\vec{c}) for a=i^\vec{a} = \hat{i}, b=j^\vec{b} = \hat{j}, c=i^+k^\vec{c} = \hat{i} + \hat{k}.

Practice — Level 1 (4 reps)

Quick reps to lock in the method. Try each, then check.

  1. 1.
    a×(b×c)=?\vec{a}\times(\vec{b}\times\vec{c}) = ? (BAC-CAB)
  2. 2.
    a×(b×c)\vec{a}\times(\vec{b}\times\vec{c}) lies in the plane of?
  3. 3.
    Is the vector triple product associative?
  4. 4.
    If unit a\vec{a} gives ab=12\vec{a}\cdot\vec{b} = -\tfrac{1}{2}, the angle between them is?

From the bank · past-year question

Example 9VectorsHARD
a\vec{a}, b\vec{b}, and c\vec{c} are three unit vectors such that a×(b×c)=32(b+c)\vec{a} \times (\vec{b} \times \vec{c}) = \dfrac{\sqrt{3}}{2}(\vec{b} + \vec{c}). If b\vec{b} is not parallel to c\vec{c}, then the angle between a\vec{a} and b\vec{b} is

[Q127 · 2nd May Shift 1 · 2023]

Inner pair sets the plane: a×(b×c)\vec{a}\times(\vec{b}\times\vec{c}) is in the b\vec{b}-c\vec{c} plane

a×(b×c)=(ac)b(ab)c\vec{a}\times(\vec{b}\times\vec{c}) = (\vec{a}\cdot\vec{c})\vec{b} - (\vec{a}\cdot\vec{b})\vec{c} lies in the plane of b,c\vec{b}, \vec{c}; (a×b)×c=(ac)b(bc)a(\vec{a}\times\vec{b})\times\vec{c} = (\vec{a}\cdot\vec{c})\vec{b} - (\vec{b}\cdot\vec{c})\vec{a} lies in the plane of a,b\vec{a}, \vec{b}. They are DIFFERENT vectors.

Match coefficients only when the basis vectors are independent

Reading off ab\vec{a}\cdot\vec{b} by comparing coefficients of b\vec{b} and c\vec{c} is valid because "b\vec{b} not parallel to c\vec{c}" makes them independent. Watch the sign: the coefficient of c\vec{c} is (ab)-(\vec{a}\cdot\vec{b}), so a positive RHS coefficient gives a NEGATIVE dot product (obtuse angle).

Two crosses ⇒ BAC-CAB; one cross + one dot ⇒ scalar triple product

If the shape is a(b×c)\vec{a}\cdot(\vec{b}\times\vec{c}) (a number), it is NOT a BAC-CAB case. Count the crosses and dots first to pick the right identity.

Concept 10 of 11

Vector orthogonal to one vector and coplanar with two others

Intuition

A standard PYQ shape: find a unit vector that is perpendicular to a given vector AND lies in the plane of two others. The vector c×(a×b)\vec{c}\times(\vec{a}\times\vec{b}) is exactly that — it is coplanar with a,b\vec{a}, \vec{b} (a BAC-CAB combination of them) and perpendicular to c\vec{c}. Equivalently, write the unknown as v=λa+μb\vec{v} = \lambda\vec{a} + \mu\vec{b} (coplanar) and impose the perpendicularity / projection condition.

Definition

To find a vector **coplanar with a,b\vec{a}, \vec{b} and perpendicular to c\vec{c}**:

  • Shortcut: c×(a×b)=(cb)a(ca)b\vec{c}\times(\vec{a}\times\vec{b}) = (\vec{c}\cdot\vec{b})\vec{a} - (\vec{c}\cdot\vec{a})\vec{b} is coplanar with a,b\vec{a}, \vec{b} and perpendicular to c\vec{c}; normalise it for a unit vector.
  • Linear-combination method: set v=λa+μb\vec{v} = \lambda\vec{a} + \mu\vec{b} (this makes it coplanar with a,b\vec{a}, \vec{b}), then impose vc=0\vec{v}\cdot\vec{c} = 0 (perpendicular) or a given projection vcc\dfrac{\vec{v}\cdot\vec{c}}{|\vec{c}|} to fix the ratio λ:μ\lambda : \mu.
  • For three given POINTS, coplanarity of position-difference vectors is the same []=0[\cdots] = 0 test.

Orthogonal-and-coplanar vector

c×(a×b)=(cb)a(ca)b\vec{c}\times(\vec{a}\times\vec{b}) = (\vec{c}\cdot\vec{b})\,\vec{a} - (\vec{c}\cdot\vec{a})\,\vec{b}
  • Coplanar with a,b\vec{a}, \vec{b}it is a combination λa+μb\lambda\vec{a} + \mu\vec{b}
  • Perpendicular to c\vec{c}by construction of the outer cross
  • Normalisedivide by its magnitude for a UNIT answer

Worked example

Find a unit vector coplanar with a=i^+j^+k^\vec{a} = \hat{i} + \hat{j} + \hat{k} and b=2i^+j^+k^\vec{b} = 2\hat{i} + \hat{j} + \hat{k}, and perpendicular to c=i^+j^k^\vec{c} = \hat{i} + \hat{j} - \hat{k}.
  1. Write v=λa+μb=(λ+2μ)i^+(λ+μ)j^+(λ+μ)k^\vec{v} = \lambda\vec{a} + \mu\vec{b} = (\lambda + 2\mu)\hat{i} + (\lambda + \mu)\hat{j} + (\lambda + \mu)\hat{k}.
  2. Perpendicular to c\vec{c}: vc=(λ+2μ)+(λ+μ)(λ+μ)=λ+2μ=0\vec{v}\cdot\vec{c} = (\lambda + 2\mu) + (\lambda + \mu) - (\lambda + \mu) = \lambda + 2\mu = 0, so λ=2μ\lambda = -2\mu.
  3. Take μ=1,λ=2\mu = 1, \lambda = -2: v=0i^j^k^=(j^+k^)\vec{v} = 0\hat{i} - \hat{j} - \hat{k} = -(\hat{j} + \hat{k}).
  4. Normalise: v=2|\vec{v}| = \sqrt{2}, so v^=±12(j^+k^)\hat{v} = \pm\dfrac{1}{\sqrt{2}}(\hat{j} + \hat{k}).
Answer:v^=±12(j^k^)\hat{v} = \pm\dfrac{1}{\sqrt{2}}(-\hat{j} - \hat{k})
Practice this conceptself-check · 4 quick reps

Try it yourself

Find a unit vector coplanar with i^+j^\hat{i} + \hat{j} and j^+k^\hat{j} + \hat{k}, perpendicular to i^+k^\hat{i} + \hat{k}.

Practice — Level 1 (4 reps)

Quick reps to lock in the method. Try each, then check.

  1. 1.
    A vector coplanar with a,b\vec{a}, \vec{b} is written as?
  2. 2.
    c×(a×b)\vec{c}\times(\vec{a}\times\vec{b}) is perpendicular to?
  3. 3.
    c×(a×b)\vec{c}\times(\vec{a}\times\vec{b}) is coplanar with?
  4. 4.
    To impose perpendicular to c\vec{c}, set what to zero?

From the bank · past-year question

Example 10VectorsHARD
The unit vector which is orthogonal to the vector 5i^+2j^+6k^5\hat{i}+2\hat{j}+6\hat{k} and is coplanar with the vectors 2i^+j^+k^2\hat{i}+\hat{j}+\hat{k} and i^j^+k^\hat{i}-\hat{j}+\hat{k} is

[Q104 · 2nd May Shift 2 · 2023]

Coplanar means a COMBINATION, not just "in the same plane"

Encode coplanarity with a,b\vec{a}, \vec{b} by writing the unknown as λa+μb\lambda\vec{a} + \mu\vec{b} from the start. Then the only freedom left is the ratio λ:μ\lambda:\mu, which the perpendicularity or projection condition pins down.

Both signs of the UNIT answer are valid

The normalised result is ±v^\pm\hat{v} — both directions satisfy "perpendicular and coplanar" unless the question fixes orientation. Pick whichever sign appears in the options.

Confirm orthogonality AND coplanarity at the end

A tempting distractor satisfies one condition but not the other. Verify vc=0\vec{v}\cdot\vec{c} = 0 (perpendicular) and that v\vec{v} is a combination of a,b\vec{a}, \vec{b} (coplanar) before selecting.

Concept 11 of 11

Solving a vector equation: a cross condition plus a magnitude/dot condition

Intuition

A condition like r×b=c×b\vec{r}\times\vec{b} = \vec{c}\times\vec{b} does not pin down r\vec{r} — it only forces rc\vec{r} - \vec{c} to be parallel to b\vec{b}. Pairing it with a scalar (dot) condition such as ra=0\vec{r}\cdot\vec{a} = 0 closes the system and gives a unique r\vec{r}. Problems mixing a×b\vec{a}\times\vec{b}, a magnitude, and an angle are solved the same way: peel off the vector identity, then use the scalar data.

Definition

To solve r×b=c×b\vec{r}\times\vec{b} = \vec{c}\times\vec{b} with a scalar condition:

  • Rewrite as (rc)×b=0(\vec{r} - \vec{c})\times\vec{b} = \vec{0}, so rc=tb\vec{r} - \vec{c} = t\vec{b}, i.e. r=c+tb\vec{r} = \vec{c} + t\vec{b}.
  • Substitute into the scalar condition (e.g. ra=0\vec{r}\cdot\vec{a} = 0) to find tt, then r\vec{r}.
  • For (a×b)×c|(\vec{a}\times\vec{b})\times\vec{c}| given c|\vec{c}| and an angle: (a×b)×c=a×bcsinϕ|(\vec{a}\times\vec{b})\times\vec{c}| = |\vec{a}\times\vec{b}|\,|\vec{c}|\sin\phi, where ϕ\phi is the angle between a×b\vec{a}\times\vec{b} and c\vec{c}, and the auxiliary conditions fix c|\vec{c}|.

Cross condition reduces to a parallel offset

r×b=c×b    r=c+tb,then use the scalar condition for t\vec{r}\times\vec{b} = \vec{c}\times\vec{b} \;\Longrightarrow\; \vec{r} = \vec{c} + t\,\vec{b}, \quad\text{then use the scalar condition for } t
  • (rc)×b=0(\vec{r} - \vec{c})\times\vec{b} = \vec{0}so rcb\vec{r} - \vec{c}\,\|\,\vec{b}
  • ttthe one free scalar — fixed by the dot/magnitude condition

Worked example

Let A=2i^+k^\vec{A} = 2\hat{i} + \hat{k}, B=i^+j^+k^\vec{B} = \hat{i} + \hat{j} + \hat{k}, C=4i^3j^+7k^\vec{C} = 4\hat{i} - 3\hat{j} + 7\hat{k}. Find R\vec{R} with R×B=C×B\vec{R}\times\vec{B} = \vec{C}\times\vec{B} and RA=0\vec{R}\cdot\vec{A} = 0.
  1. R×B=C×B\vec{R}\times\vec{B} = \vec{C}\times\vec{B}(RC)×B=0(\vec{R} - \vec{C})\times\vec{B} = \vec{0}R=C+tB\vec{R} = \vec{C} + t\vec{B}.
  2. So R=(4+t)i^+(3+t)j^+(7+t)k^\vec{R} = (4 + t)\hat{i} + (-3 + t)\hat{j} + (7 + t)\hat{k}.
  3. Impose RA=0\vec{R}\cdot\vec{A} = 0: 2(4+t)+0(3+t)+1(7+t)=08+2t+7+t=03t=15t=52(4 + t) + 0(-3 + t) + 1(7 + t) = 0 \Rightarrow 8 + 2t + 7 + t = 0 \Rightarrow 3t = -15 \Rightarrow t = -5.
  4. Substitute: R=i^8j^+2k^\vec{R} = -\hat{i} - 8\hat{j} + 2\hat{k}.
Answer:R=i^8j^+2k^\vec{R} = -\hat{i} - 8\hat{j} + 2\hat{k}
Practice this conceptself-check · 4 quick reps

Try it yourself

Find r\vec{r} with r×b=c×b\vec{r}\times\vec{b} = \vec{c}\times\vec{b} and ra=4\vec{r}\cdot\vec{a} = 4, where a=i^+j^+k^\vec{a} = \hat{i} + \hat{j} + \hat{k}, b=k^\vec{b} = \hat{k} and c=2i^+j^k^\vec{c} = 2\hat{i} + \hat{j} - \hat{k}.

Practice — Level 1 (4 reps)

Quick reps to lock in the method. Try each, then check.

  1. 1.
    r×b=c×b\vec{r}\times\vec{b} = \vec{c}\times\vec{b} implies rc\vec{r} - \vec{c} is?
  2. 2.
    So r=?\vec{r} = ?
  3. 3.
    What fixes the scalar tt?
  4. 4.
    (a×b)×c=?|(\vec{a}\times\vec{b})\times\vec{c}| = ?

From the bank · past-year question

Example 11VectorsHARD
Let A=2i^+k^\vec{A} = 2\hat{i}+\hat{k}, B=i^+j^+k^\vec{B} = \hat{i}+\hat{j}+\hat{k} and C=4i^3j^+7k^\vec{C} = 4\hat{i}-3\hat{j}+7\hat{k}. If a vector R\vec{R} satisfies R×B=C×B\vec{R}\times\vec{B} = \vec{C}\times\vec{B} and RA=0\vec{R}\cdot\vec{A} = 0, then R\vec{R} is given by

[Q108 · 2nd May Shift 2 · 2023]

You cannot cancel the cross product

r×b=c×b\vec{r}\times\vec{b} = \vec{c}\times\vec{b} does NOT give r=c\vec{r} = \vec{c}. The correct deduction is (rc)×b=0(\vec{r} - \vec{c})\times\vec{b} = \vec{0}, i.e. r=c+tb\vec{r} = \vec{c} + t\vec{b}; the scalar condition then fixes tt.

The cross condition alone leaves one free scalar

A single cross equation can never determine r\vec{r} uniquely — any multiple of b\vec{b} can be added. Always use the accompanying scalar (dot or magnitude) condition to close the system.

Summary — formulas & gotchas at a glance

A revision cheat-sheet for the formulas and gotchas above. Click any concept name to jump back to its full explanation.

Formulas (11)

  • The scalar triple product — dot-cross and determinant form

    Scalar triple product as a determinant

    [a b c]=a(b×c)=a1a2a3b1b2b3c1c2c3[\vec{a}\ \vec{b}\ \vec{c}] = \vec{a}\cdot(\vec{b}\times\vec{c}) = \begin{vmatrix} a_1 & a_2 & a_3 \\ b_1 & b_2 & b_3 \\ c_1 & c_2 & c_3 \end{vmatrix}
  • Cyclic and sign properties of the scalar triple product

    Cyclic and swap rules

    [a b c]=[b c a]=[c a b]=[b a c][\vec{a}\ \vec{b}\ \vec{c}] = [\vec{b}\ \vec{c}\ \vec{a}] = [\vec{c}\ \vec{a}\ \vec{b}] = -[\vec{b}\ \vec{a}\ \vec{c}]
  • Computing the value of a scalar triple product

    STP when one vector is perpendicular to the other two

    [a b c]=ab×c=abcsinθ[\vec{a}\ \vec{b}\ \vec{c}] = |\vec{a}|\,|\vec{b}\times\vec{c}| = |\vec{a}||\vec{b}||\vec{c}|\sin\theta
  • Coplanarity of three vectors (and solving for a parameter)

    Coplanarity criterion

    a,b,c coplanar    a1a2a3b1b2b3c1c2c3=0\vec{a},\vec{b},\vec{c}\text{ coplanar} \iff \begin{vmatrix} a_1 & a_2 & a_3 \\ b_1 & b_2 & b_3 \\ c_1 & c_2 & c_3 \end{vmatrix} = 0
  • Scalar triple product of linear combinations

    Linear-combination identities

    [a+b  b+c  c+a]=2[a b c][ma+b  mb+c  mc+a]=(m3+1)[a b c][\vec{a}+\vec{b}\ \ \vec{b}+\vec{c}\ \ \vec{c}+\vec{a}] = 2[\vec{a}\ \vec{b}\ \vec{c}] \qquad [m\vec{a}+\vec{b}\ \ m\vec{b}+\vec{c}\ \ m\vec{c}+\vec{a}] = (m^3+1)[\vec{a}\ \vec{b}\ \vec{c}]
  • Volume of a parallelepiped (and min/max problems)

    Parallelepiped volume

    V=[a b c]=a1a2a3b1b2b3c1c2c3V = |[\vec{a}\ \vec{b}\ \vec{c}]| = \left|\begin{vmatrix} a_1 & a_2 & a_3 \\ b_1 & b_2 & b_3 \\ c_1 & c_2 & c_3 \end{vmatrix}\right|
  • Volume of a tetrahedron

    Tetrahedron volume

    V=16[AB AC AD]V = \tfrac{1}{6}\,\bigl|[\overrightarrow{AB}\ \overrightarrow{AC}\ \overrightarrow{AD}]\bigr|
  • Reciprocal-basis identities and the STP-squared rule

    Reciprocal pairings and STP-squared

    ap=bq=cr=1,aq=bp==0[a×b  b×c  c×a]=[a b c]2\vec{a}\cdot\vec{p} = \vec{b}\cdot\vec{q} = \vec{c}\cdot\vec{r} = 1, \quad \vec{a}\cdot\vec{q} = \vec{b}\cdot\vec{p} = \dots = 0 \qquad [\vec{a}\times\vec{b}\ \ \vec{b}\times\vec{c}\ \ \vec{c}\times\vec{a}] = [\vec{a}\ \vec{b}\ \vec{c}]^2
  • Vector triple product (BAC-CAB rule)

    BAC-CAB rule

    a×(b×c)=(ac)b(ab)c\vec{a}\times(\vec{b}\times\vec{c}) = (\vec{a}\cdot\vec{c})\,\vec{b} - (\vec{a}\cdot\vec{b})\,\vec{c}
  • Vector orthogonal to one vector and coplanar with two others

    Orthogonal-and-coplanar vector

    c×(a×b)=(cb)a(ca)b\vec{c}\times(\vec{a}\times\vec{b}) = (\vec{c}\cdot\vec{b})\,\vec{a} - (\vec{c}\cdot\vec{a})\,\vec{b}
  • Solving a vector equation: a cross condition plus a magnitude/dot condition

    Cross condition reduces to a parallel offset

    r×b=c×b    r=c+tb,then use the scalar condition for t\vec{r}\times\vec{b} = \vec{c}\times\vec{b} \;\Longrightarrow\; \vec{r} = \vec{c} + t\,\vec{b}, \quad\text{then use the scalar condition for } t

Watch out for (24)

Mastery check — 5 interleaved questions

Try each one before clicking. Questions are interleaved across the concepts above, not grouped — interleaving sharpens transfer.

Example 1VectorsMODERATE
If a,b,c\vec{a}, \vec{b}, \vec{c} are three vectors, a=2|\vec{a}|=2, b=4|\vec{b}|=4, c=1|\vec{c}|=1, b×c=15|\vec{b}\times\vec{c}|=\sqrt{15} and b=2c+λa\vec{b}=2\vec{c}+\lambda\vec{a}, then the value of λ\lambda is

[Q101 · 12th May Shift 1 · 2024]

Example 2VectorsMODERATE
If the vector c\vec{c} lies in the plane of a\vec{a} and b\vec{b}, where a=i^j^+2k^,b=i^+j^+k^\vec{a}=\hat{i}-\hat{j}+2\hat{k},\, \vec{b}=\hat{i}+\hat{j}+\hat{k} and c=xi^(2x)j^k^\vec{c}=x\hat{i}-(2-x)\hat{j}-\hat{k}, then the value of xx is

[Q139 · 15th May Shift 2 · 2023]

Example 3VectorsHARD
If a,b,c\vec{a},\vec{b},\vec{c} are mutually perpendicular vectors having magnitudes 1, 2, 3 respectively, then the value of [a+b+c    ba    c][\vec{a}+\vec{b}+\vec{c} \;\; \vec{b}-\vec{a} \;\; \vec{c}] is

[Q105 · 10th May Shift 2 · 2023]

Example 4VectorsHARD
If the volume of the parallelepiped is 158 cu. units whose coterminous edges are given by the vectors a=(i^+j^+nk^)\vec{a} = (\hat{i}+\hat{j}+n\hat{k}), b=2i^+4j^nk^\vec{b} = 2\hat{i}+4\hat{j}-n\hat{k} and c=i^+nj^+3k^\vec{c} = \hat{i}+n\hat{j}+3\hat{k}, where n0n \geq 0, then the value of n is

[Q114 · 11th May Shift 1 · 2024]

Example 5VectorsHARD
If the volume of tetrahedron, whose vertices are with position vectors i^6j^+10k^,i^3j^+7k^\hat{i}-6\hat{j}+10\hat{k},\,-\hat{i}-3\hat{j}+7\hat{k}, 5i^j^+λk^5\hat{i}-\hat{j}+\lambda\hat{k} and 7i^4j^+7k^7\hat{i}-4\hat{j}+7\hat{k} is 11 cubic units, then value of λ\lambda is

[Q101 · 10th May Shift 2 · 2024]

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