Board Coverage
Board Paper Notes AQA Paper 1, 2 2D vectors in P1; 3D vectors, scalar product in P2 Edexcel P1, P2 Similar split OCR (A) Paper 1, 2 Includes vector equations of lines CIE (9709) P1, P2, P3 2D in P1; 3D and lines in P2/P3
The formula booklet gives the scalar product formula. You must be comfortable working in 3D
and converting between column and i , j , k \mathbf{i},\mathbf{j},\mathbf{k} i , j , k notation.
1. Vectors in 2D and 3D
1.1 Definition
Definition. A vector is a quantity with both magnitude and direction. A scalar is a
quantity with magnitude only.
Vectors in 2D are written as column vectors: ( a b ) \dbinom{a}{b} ( b a ) or a i + b j a\mathbf{i} + b\mathbf{j} a i + b j .
Vectors in 3D: ( a b c ) \begin{pmatrix}a\\b\\c\end{pmatrix} a b c or a i + b j + c k a\mathbf{i} + b\mathbf{j} + c\mathbf{k} a i + b j + c k .
The unit vectors i = ( 1 0 ) \mathbf{i} = \dbinom{1}{0} i = ( 0 1 ) , j = ( 0 1 ) \mathbf{j} = \dbinom{0}{1} j = ( 1 0 ) point along the positive
x x x - and y y y -axes respectively. In 3D, k = ( 0 0 1 ) \mathbf{k} = \begin{pmatrix}0\\0\\1\end{pmatrix} k = 0 0 1 .
1.2 Position vectors
The position vector of a point P P P relative to an origin O O O is the vector
O P → \overrightarrow{OP} O P , written as r P \mathbf{r}_P r P or simply p \mathbf{p} p .
2. Magnitude, Unit Vectors, Direction Cosines
2.1 Magnitude
The magnitude (length) of a = ( a 1 a 2 a 3 ) \mathbf{a} = \begin{pmatrix}a_1\\a_2\\a_3\end{pmatrix} a = a 1 a 2 a 3 is
∣ a ∣ = a 1 2 + a 2 2 + a 3 2 |\mathbf{a}| = \sqrt{a_1^2 + a_2^2 + a_3^2} ∣ a ∣ = a 1 2 + a 2 2 + a 3 2
This follows directly from Pythagoras' theorem applied in 3D.
2.2 Unit vectors
A unit vector has magnitude 1. The unit vector in the direction of a \mathbf{a} a is
a ^ = ◆ L B ◆ a ◆ R B ◆◆ L B ◆ ∣ a ∣ ◆ R B ◆ \hat{\mathbf{a}} = \frac◆LB◆\mathbf{a}◆RB◆◆LB◆|\mathbf{a}|◆RB◆ a ^ = L ◆ B ◆ a ◆ R B ◆◆ L B ◆∣ a ∣◆ R B ◆
2.3 Direction cosines
The direction cosines of a = ( a 1 a 2 a 3 ) \mathbf{a} = \begin{pmatrix}a_1\\a_2\\a_3\end{pmatrix} a = a 1 a 2 a 3 are
cos α = ◆ L B ◆ a 1 ◆ R B ◆◆ L B ◆ ∣ a ∣ ◆ R B ◆ , cos β = ◆ L B ◆ a 2 ◆ R B ◆◆ L B ◆ ∣ a ∣ ◆ R B ◆ , cos γ = ◆ L B ◆ a 3 ◆ R B ◆◆ L B ◆ ∣ a ∣ ◆ R B ◆ \cos\alpha = \frac◆LB◆a_1◆RB◆◆LB◆|\mathbf{a}|◆RB◆, \quad \cos\beta = \frac◆LB◆a_2◆RB◆◆LB◆|\mathbf{a}|◆RB◆, \quad \cos\gamma = \frac◆LB◆a_3◆RB◆◆LB◆|\mathbf{a}|◆RB◆ cos α = L ◆ B ◆ a 1 ◆ R B ◆◆ L B ◆∣ a ∣◆ R B ◆ , cos β = L ◆ B ◆ a 2 ◆ R B ◆◆ L B ◆∣ a ∣◆ R B ◆ , cos γ = L ◆ B ◆ a 3 ◆ R B ◆◆ L B ◆∣ a ∣◆ R B ◆
where α \alpha α , β \beta β , γ \gamma γ are the angles between a \mathbf{a} a and the x x x -, y y y -, z z z -axes
respectively.
Note: cos 2 α + cos 2 β + cos 2 γ = 1 \cos^2\alpha + \cos^2\beta + \cos^2\gamma = 1 cos 2 α + cos 2 β + cos 2 γ = 1 .
3. Vector Addition
3.1 Triangle law
To go from A A A to C C C via B B B : A C → = A B → + B C → \overrightarrow{AC} = \overrightarrow{AB} + \overrightarrow{BC} A C = A B + B C .
3.2 Parallelogram law (geometric proof)
Theorem. If two vectors a \mathbf{a} a and b \mathbf{b} b are represented as adjacent sides of a
parallelogram, then the diagonal a + b \mathbf{a} + \mathbf{b} a + b represents their sum.
Proof. Consider parallelogram O A C B OACB O A C B where O A → = a \overrightarrow{OA} = \mathbf{a} O A = a and
O B → = b \overrightarrow{OB} = \mathbf{b} O B = b .
Since O A C B OACB O A C B is a parallelogram, A C → = O B → = b \overrightarrow{AC} = \overrightarrow{OB} = \mathbf{b} A C = O B = b .
By the triangle law:
O C → = O A → + A C → = a + b \overrightarrow{OC} = \overrightarrow{OA} + \overrightarrow{AC} = \mathbf{a} + \mathbf{b} O C = O A + A C = a + b .
Similarly, B C → = O A → = a \overrightarrow{BC} = \overrightarrow{OA} = \mathbf{a} B C = O A = a , so
O C → = O B → + B C → = b + a \overrightarrow{OC} = \overrightarrow{OB} + \overrightarrow{BC} = \mathbf{b} + \mathbf{a} O C = O B + B C = b + a .
This proves a + b = b + a \mathbf{a} + \mathbf{b} = \mathbf{b} + \mathbf{a} a + b = b + a (vector addition is commutative) and
that the diagonal of the parallelogram represents the sum. ■ \blacksquare ■
3.3 Vector addition in 3D
Vector addition extends naturally to three dimensions. Given
a = ( a 1 a 2 a 3 ) \mathbf{a} = \begin{pmatrix}a_1\\a_2\\a_3\end{pmatrix} a = a 1 a 2 a 3 and
b = ( b 1 b 2 b 3 ) \mathbf{b} = \begin{pmatrix}b_1\\b_2\\b_3\end{pmatrix} b = b 1 b 2 b 3 :
a + b = ( a 1 + b 1 a 2 + b 2 a 3 + b 3 ) \mathbf{a} + \mathbf{b} = \begin{pmatrix}a_1+b_1\\a_2+b_2\\a_3+b_3\end{pmatrix} a + b = a 1 + b 1 a 2 + b 2 a 3 + b 3
The same triangle and parallelogram laws apply. The key properties are:
Commutativity: a + b = b + a \mathbf{a} + \mathbf{b} = \mathbf{b} + \mathbf{a} a + b = b + a
Associativity:
( a + b ) + c = a + ( b + c ) (\mathbf{a} + \mathbf{b}) + \mathbf{c} = \mathbf{a} + (\mathbf{b} + \mathbf{c}) ( a + b ) + c = a + ( b + c )
Zero vector: a + 0 = a \mathbf{a} + \mathbf{0} = \mathbf{a} a + 0 = a where
0 = ( 0 0 0 ) \mathbf{0} = \begin{pmatrix}0\\0\\0\end{pmatrix} 0 = 0 0 0
Additive inverse: a + ( − a ) = 0 \mathbf{a} + (-\mathbf{a}) = \mathbf{0} a + ( − a ) = 0
Scalar multiplication also satisfies the distributive laws:
λ ( a + b ) = λ a + λ b \lambda(\mathbf{a} + \mathbf{b}) = \lambda\mathbf{a} + \lambda\mathbf{b} λ ( a + b ) = λ a + λ b and
( λ + μ ) a = λ a + μ a (\lambda + \mu)\mathbf{a} = \lambda\mathbf{a} + \mu\mathbf{a} ( λ + μ ) a = λ a + μ a for scalars λ , μ \lambda, \mu λ , μ .
Example. Given points A ( 1 , 2 , − 1 ) A(1, 2, -1) A ( 1 , 2 , − 1 ) , B ( 4 , 0 , 3 ) B(4, 0, 3) B ( 4 , 0 , 3 ) , C ( 2 , 5 , 1 ) C(2, 5, 1) C ( 2 , 5 , 1 ) , find
A B → + B C → \overrightarrow{AB} + \overrightarrow{BC} A B + B C .
A B → = ( 3 − 2 4 ) \overrightarrow{AB} = \begin{pmatrix}3\\-2\\4\end{pmatrix} A B = 3 − 2 4 ,
B C → = ( − 2 5 − 2 ) \overrightarrow{BC} = \begin{pmatrix}-2\\5\\-2\end{pmatrix} B C = − 2 5 − 2 .
A B → + B C → = ( 1 3 2 ) = A C → \overrightarrow{AB} + \overrightarrow{BC} = \begin{pmatrix}1\\3\\2\end{pmatrix} = \overrightarrow{AC} A B + B C = 1 3 2 = A C ,
confirming the triangle law in 3D.
4. The Scalar (Dot) Product
4.1 Definition
Definition. The scalar (dot) product of a = ( a 1 a 2 a 3 ) \mathbf{a} = \begin{pmatrix}a_1\\a_2\\a_3\end{pmatrix} a = a 1 a 2 a 3
and b = ( b 1 b 2 b 3 ) \mathbf{b} = \begin{pmatrix}b_1\\b_2\\b_3\end{pmatrix} b = b 1 b 2 b 3 is
a ⋅ b = a 1 b 1 + a 2 b 2 + a 3 b 3 \mathbf{a}\cdot\mathbf{b} = a_1b_1 + a_2b_2 + a_3b_3 a ⋅ b = a 1 b 1 + a 2 b 2 + a 3 b 3
4.2 Geometric interpretation
Theorem. a ⋅ b = ∣ a ∣ ∣ b ∣ cos θ \mathbf{a}\cdot\mathbf{b} = |\mathbf{a}||\mathbf{b}|\cos\theta a ⋅ b = ∣ a ∣∣ b ∣ cos θ , where θ \theta θ is the
angle between a \mathbf{a} a and b \mathbf{b} b .
Proof using the cosine rule. Consider the triangle formed by vectors a \mathbf{a} a , b \mathbf{b} b ,
and a − b \mathbf{a} - \mathbf{b} a − b .
By the cosine rule:
∣ a − b ∣ 2 = ∣ a ∣ 2 + ∣ b ∣ 2 − 2 ∣ a ∣ ∣ b ∣ cos θ |\mathbf{a}-\mathbf{b}|^2 = |\mathbf{a}|^2 + |\mathbf{b}|^2 - 2|\mathbf{a}||\mathbf{b}|\cos\theta ∣ a − b ∣ 2 = ∣ a ∣ 2 + ∣ b ∣ 2 − 2∣ a ∣∣ b ∣ cos θ .
Now compute ∣ a − b ∣ 2 |\mathbf{a}-\mathbf{b}|^2 ∣ a − b ∣ 2 algebraically:
∣ a − b ∣ 2 = ( a 1 − b 1 ) 2 + ( a 2 − b 2 ) 2 + ( a 3 − b 3 ) 2 = ( a 1 2 + a 2 2 + a 3 2 ) + ( b 1 2 + b 2 2 + b 3 2 ) − 2 ( a 1 b 1 + a 2 b 2 + a 3 b 3 ) = ∣ a ∣ 2 + ∣ b ∣ 2 − 2 a ⋅ b \begin{aligned}
|\mathbf{a}-\mathbf{b}|^2 &= (a_1-b_1)^2 + (a_2-b_2)^2 + (a_3-b_3)^2 \\
&= (a_1^2+a_2^2+a_3^2) + (b_1^2+b_2^2+b_3^2) - 2(a_1b_1+a_2b_2+a_3b_3) \\
&= |\mathbf{a}|^2 + |\mathbf{b}|^2 - 2\,\mathbf{a}\cdot\mathbf{b}
\end{aligned} ∣ a − b ∣ 2 = ( a 1 − b 1 ) 2 + ( a 2 − b 2 ) 2 + ( a 3 − b 3 ) 2 = ( a 1 2 + a 2 2 + a 3 2 ) + ( b 1 2 + b 2 2 + b 3 2 ) − 2 ( a 1 b 1 + a 2 b 2 + a 3 b 3 ) = ∣ a ∣ 2 + ∣ b ∣ 2 − 2 a ⋅ b
Comparing with the cosine rule:
∣ a ∣ 2 + ∣ b ∣ 2 − 2 a ⋅ b = ∣ a ∣ 2 + ∣ b ∣ 2 − 2 ∣ a ∣ ∣ b ∣ cos θ |\mathbf{a}|^2 + |\mathbf{b}|^2 - 2\,\mathbf{a}\cdot\mathbf{b} = |\mathbf{a}|^2 + |\mathbf{b}|^2 - 2|\mathbf{a}||\mathbf{b}|\cos\theta ∣ a ∣ 2 + ∣ b ∣ 2 − 2 a ⋅ b = ∣ a ∣ 2 + ∣ b ∣ 2 − 2∣ a ∣∣ b ∣ cos θ
a ⋅ b = ∣ a ∣ ∣ b ∣ cos θ ■ \mathbf{a}\cdot\mathbf{b} = |\mathbf{a}||\mathbf{b}|\cos\theta \quad \blacksquare a ⋅ b = ∣ a ∣∣ b ∣ cos θ ■
4.3 Perpendicularity test
a ⊥ b ⟺ a ⋅ b = 0 \mathbf{a} \perp \mathbf{b} \iff \mathbf{a}\cdot\mathbf{b} = 0 a ⊥ b ⟺ a ⋅ b = 0 (when neither vector is zero).
This follows since cos ( π / 2 ) = 0 \cos(\pi/2) = 0 cos ( π /2 ) = 0 .
Intuition. The dot product a ⋅ b \mathbf{a}\cdot\mathbf{b} a ⋅ b measures the extent to which a \mathbf{a} a
and b \mathbf{b} b point in the same direction. It equals the product of the magnitude of a \mathbf{a} a
and the projection of b \mathbf{b} b onto a \mathbf{a} a :
a ⋅ b = ∣ a ∣ ⋅ ( s h a d o w o f b o n a ) \mathbf{a}\cdot\mathbf{b} = |\mathbf{a}| \cdot (\mathrm{shadow of }\mathbf{b}\mathrm{ on }\mathbf{a}) a ⋅ b = ∣ a ∣ ⋅ ( shadowof b on a ) .
If they are perpendicular, the shadow is zero. If they point the same way, the dot product is
positive; if opposite, negative.
5. Vector Equation of a Line
5.1 Definition
Definition. The vector equation of a line passing through point A A A with position vector
a \mathbf{a} a , in the direction of vector b \mathbf{b} b , is
r = a + t b , t ∈ R \mathbf{r} = \mathbf{a} + t\mathbf{b}, \quad t \in \mathbb{R} r = a + t b , t ∈ R
where r \mathbf{r} r is the position vector of a general point on the line, and t t t is a parameter.
If a = ( a 1 a 2 a 3 ) \mathbf{a} = \begin{pmatrix}a_1\\a_2\\a_3\end{pmatrix} a = a 1 a 2 a 3 and
b = ( b 1 b 2 b 3 ) \mathbf{b} = \begin{pmatrix}b_1\\b_2\\b_3\end{pmatrix} b = b 1 b 2 b 3 , the parametric equations are
x = a 1 + t b 1 , y = a 2 + t b 2 , z = a 3 + t b 3 x = a_1 + tb_1, \quad y = a_2 + tb_2, \quad z = a_3 + tb_3 x = a 1 + t b 1 , y = a 2 + t b 2 , z = a 3 + t b 3
In 2D, eliminating t t t : x − a 1 b 1 = y − a 2 b 2 \dfrac{x - a_1}{b_1} = \dfrac{y - a_2}{b_2} b 1 x − a 1 = b 2 y − a 2 .
warning
a \mathbf{a} a , and the direction vector b \mathbf{b} b can be any non-zero scalar multiple of the
direction. Always check your answer gives a point and direction consistent with the question.
5.4 Vector equation of a line in 3D
The vector equation of a line in 3D has the same form as in 2D, but now operates in three
dimensions. Given a point A ( x 0 , y 0 , z 0 ) A(x_0, y_0, z_0) A ( x 0 , y 0 , z 0 ) on the line and a direction vector
d = ( d 1 d 2 d 3 ) \mathbf{d} = \begin{pmatrix}d_1\\d_2\\d_3\end{pmatrix} d = d 1 d 2 d 3 :
r = ( x 0 y 0 z 0 ) + t ( d 1 d 2 d 3 ) , t ∈ R \mathbf{r} = \begin{pmatrix}x_0\\y_0\\z_0\end{pmatrix} + t\begin{pmatrix}d_1\\d_2\\d_3\end{pmatrix}, \quad t \in \mathbb{R} r = x 0 y 0 z 0 + t d 1 d 2 d 3 , t ∈ R
The parametric form is:
x = x 0 + t d 1 , y = y 0 + t d 2 , z = z 0 + t d 3 x = x_0 + td_1, \quad y = y_0 + td_2, \quad z = z_0 + td_3 x = x 0 + t d 1 , y = y 0 + t d 2 , z = z 0 + t d 3
tip
and A B → \overrightarrow{AB} A B as the direction vector. Alternatively, use B B B and B A → \overrightarrow{BA} B A
--- both give the same line.
Example. Find the vector equation of the line through P ( 2 , − 1 , 3 ) P(2, -1, 3) P ( 2 , − 1 , 3 ) and Q ( 5 , 1 , − 2 ) Q(5, 1, -2) Q ( 5 , 1 , − 2 ) .
Direction: P Q → = ( 3 2 − 5 ) \overrightarrow{PQ} = \begin{pmatrix}3\\2\\-5\end{pmatrix} P Q = 3 2 − 5 .
r = ( 2 − 1 3 ) + t ( 3 2 − 5 ) \mathbf{r} = \begin{pmatrix}2\\-1\\3\end{pmatrix} + t\begin{pmatrix}3\\2\\-5\end{pmatrix} r = 2 − 1 3 + t 3 2 − 5
To check: at t = 0 t = 0 t = 0 we get P P P ; at t = 1 t = 1 t = 1 we get ( 5 1 − 2 ) = Q \begin{pmatrix}5\\1\\-2\end{pmatrix} = Q 5 1 − 2 = Q . ✓
6. Intersection of Lines
6.1 Two lines in 3D
Given r 1 = a 1 + t b 1 \mathbf{r}_1 = \mathbf{a}_1 + t\mathbf{b}_1 r 1 = a 1 + t b 1 and
r 2 = a 2 + s b 2 \mathbf{r}_2 = \mathbf{a}_2 + s\mathbf{b}_2 r 2 = a 2 + s b 2 :
Method:
Equate the x x x -, y y y -, and z z z -components.
Solve two equations for t t t and s s s .
Check the third equation is consistent.
If consistent: the lines intersect at the point found.
If inconsistent: the lines are skew (non-parallel and non-intersecting).
If b 1 = k b 2 \mathbf{b}_1 = k\mathbf{b}_2 b 1 = k b 2 for some scalar k k k : the lines are parallel (coincident if
also a 2 − a 1 \mathbf{a}_2 - \mathbf{a}_1 a 2 − a 1 is parallel to b 1 \mathbf{b}_1 b 1 ).
6.2 Skew lines
Definition. Two lines in 3D are skew if they are not parallel and do not intersect.
To verify skewness, show that the system of equations for t t t and s s s is inconsistent.
7. Angle Between Two Vectors
From the dot product formula:
cos θ = ◆ L B ◆ a ⋅ b ◆ R B ◆◆ L B ◆ ∣ a ∣ ∣ b ∣ ◆ R B ◆ \cos\theta = \frac◆LB◆\mathbf{a}\cdot\mathbf{b}◆RB◆◆LB◆|\mathbf{a}||\mathbf{b}|◆RB◆ cos θ = L ◆ B ◆ a ⋅ b ◆ R B ◆◆ L B ◆∣ a ∣∣ b ∣◆ R B ◆
The angle between two lines is found using the direction vectors.
8. Distance from a Point to a Line
To find the shortest distance from point P P P to line r = a + t b \mathbf{r} = \mathbf{a} + t\mathbf{b} r = a + t b :
Let Q Q Q be the closest point on the line to P P P .
P Q → \overrightarrow{PQ} P Q is perpendicular to b \mathbf{b} b , so
P Q → ⋅ b = 0 \overrightarrow{PQ}\cdot\mathbf{b} = 0 P Q ⋅ b = 0 .
If P P P has position vector p \mathbf{p} p , then
P Q → = a + t b − p \overrightarrow{PQ} = \mathbf{a} + t\mathbf{b} - \mathbf{p} P Q = a + t b − p .
( a + t b − p ) ⋅ b = 0 (\mathbf{a} + t\mathbf{b} - \mathbf{p})\cdot\mathbf{b} = 0 ( a + t b − p ) ⋅ b = 0 gives t t t .
Substitute back to find Q Q Q and compute ∣ P Q → ∣ |\overrightarrow{PQ}| ∣ P Q ∣ .
The above procedure yields the general formula. For a line through A A A with direction d \mathbf{d} d ,
and a point P P P with position vector p \mathbf{p} p :
d = ◆ L B ◆ ∣ ( p − a ) × d ∣ ◆ R B ◆◆ L B ◆ ∣ d ∣ ◆ R B ◆ d = \frac◆LB◆|(\mathbf{p} - \mathbf{a}) \times \mathbf{d}|◆RB◆◆LB◆|\mathbf{d}|◆RB◆ d = L ◆ B ◆∣ ( p − a ) × d ∣◆ R B ◆◆ L B ◆∣ d ∣◆ R B ◆
This uses the cross product (vector product), which gives a vector perpendicular to both
A P → \overrightarrow{AP} A P and d \mathbf{d} d whose magnitude equals the area of the parallelogram they
span. Dividing by ∣ d ∣ |\mathbf{d}| ∣ d ∣ (the base) gives the perpendicular height, i.e. the shortest
distance.
When the cross product is not on your syllabus, use the dot-product method from Section 8.
The cross-product formula is listed here for reference and is examined on CIE P3 and some OCR
papers.
Example using the dot-product method. Find the distance from P ( 4 , 1 , − 1 ) P(4, 1, -1) P ( 4 , 1 , − 1 ) to the line
r = ( 1 0 2 ) + t ( 2 1 − 1 ) \mathbf{r} = \begin{pmatrix}1\\0\\2\end{pmatrix} + t\begin{pmatrix}2\\1\\-1\end{pmatrix} r = 1 0 2 + t 2 1 − 1 .
P Q → = ( 1 + 2 t t 2 − t ) − ( 4 1 − 1 ) = ( 2 t − 3 t − 1 3 − t ) \overrightarrow{PQ} = \begin{pmatrix}1+2t\\t\\2-t\end{pmatrix} - \begin{pmatrix}4\\1\\-1\end{pmatrix}
= \begin{pmatrix}2t-3\\t-1\\3-t\end{pmatrix} P Q = 1 + 2 t t 2 − t − 4 1 − 1 = 2 t − 3 t − 1 3 − t .
Set P Q → ⋅ ( 2 1 − 1 ) = 0 \overrightarrow{PQ}\cdot\begin{pmatrix}2\\1\\-1\end{pmatrix} = 0 P Q ⋅ 2 1 − 1 = 0 :
2 ( 2 t − 3 ) + ( t − 1 ) − ( 3 − t ) = 0 ⟹ 4 t − 6 + t − 1 − 3 + t = 0 ⟹ 6 t = 10 ⟹ t = 5 3 2(2t-3) + (t-1) - (3-t) = 0 \implies 4t - 6 + t - 1 - 3 + t = 0 \implies 6t = 10 \implies t = \dfrac{5}{3} 2 ( 2 t − 3 ) + ( t − 1 ) − ( 3 − t ) = 0 ⟹ 4 t − 6 + t − 1 − 3 + t = 0 ⟹ 6 t = 10 ⟹ t = 3 5 .
Q = ( 1 + 10 / 3 5 / 3 2 − 5 / 3 ) = ( 13 / 3 5 / 3 1 / 3 ) Q = \begin{pmatrix}1+10/3\\5/3\\2-5/3\end{pmatrix} = \begin{pmatrix}13/3\\5/3\\1/3\end{pmatrix} Q = 1 + 10/3 5/3 2 − 5/3 = 13/3 5/3 1/3 .
d = ∣ ( 1 / 3 2 / 3 − 2 / 3 ) ∣ = ◆ L B ◆ 1 9 + 4 9 + 4 9 ◆ R B ◆ = ◆ L B ◆ 9 9 ◆ R B ◆ = 1 d = \left|\begin{pmatrix}1/3\\2/3\\-2/3\end{pmatrix}\right| = \sqrt◆LB◆\dfrac{1}{9} + \dfrac{4}{9} + \dfrac{4}{9}◆RB◆ = \sqrt◆LB◆\dfrac{9}{9}◆RB◆ = 1 d = 1/3 2/3 − 2/3 = ◆ L B ◆ 9 1 + 9 4 + 9 4 ◆ R B ◆ = ◆ L B ◆ 9 9 ◆ R B ◆ = 1 .
9. Scalar Triple Product
9.1 Definition
Definition. The scalar triple product of three vectors a \mathbf{a} a , b \mathbf{b} b ,
c \mathbf{c} c is
[ a , b , c ] = a ⋅ ( b × c ) [\mathbf{a},\, \mathbf{b},\, \mathbf{c}] = \mathbf{a}\cdot(\mathbf{b}\times\mathbf{c}) [ a , b , c ] = a ⋅ ( b × c )
In component form, this equals the determinant:
[ a , b , c ] = ∣ a 1 a 2 a 3 b 1 b 2 b 3 c 1 c 2 c 3 ∣ [\mathbf{a},\, \mathbf{b},\, \mathbf{c}] = \begin{vmatrix} a_1 & a_2 & a_3 \\ b_1 & b_2 & b_3 \\ c_1 & c_2 & c_3 \end{vmatrix} [ a , b , c ] = a 1 b 1 c 1 a 2 b 2 c 2 a 3 b 3 c 3
9.2 Geometric interpretation: volume of a parallelepiped
Theorem. The absolute value of the scalar triple product equals the volume of the parallelepiped
with edges defined by a \mathbf{a} a , b \mathbf{b} b , and c \mathbf{c} c .
V = ∣ a ⋅ ( b × c ) ∣ V = |\mathbf{a}\cdot(\mathbf{b}\times\mathbf{c})| V = ∣ a ⋅ ( b × c ) ∣
Proof. The vector b × c \mathbf{b}\times\mathbf{c} b × c has magnitude
∣ b ∣ ∣ c ∣ sin θ |\mathbf{b}||\mathbf{c}|\sin\theta ∣ b ∣∣ c ∣ sin θ equal to the area of the parallelogram with sides b \mathbf{b} b
and c \mathbf{c} c , and direction perpendicular to both. The height of the parallelepiped is the
projection of a \mathbf{a} a onto b × c \mathbf{b}\times\mathbf{c} b × c , which is ∣ a ∣ cos ϕ |\mathbf{a}|\cos\phi ∣ a ∣ cos ϕ where
ϕ \phi ϕ is the angle between a \mathbf{a} a and b × c \mathbf{b}\times\mathbf{c} b × c .
V = b a s e a r e a × h e i g h t = ∣ b × c ∣ ⋅ ∣ a ∣ cos ϕ = ∣ a ⋅ ( b × c ) ∣ ■ V = \mathrm{base area} \times \mathrm{height} = |\mathbf{b}\times\mathbf{c}| \cdot |\mathbf{a}|\cos\phi = |\mathbf{a}\cdot(\mathbf{b}\times\mathbf{c})| \quad \blacksquare V = basearea × height = ∣ b × c ∣ ⋅ ∣ a ∣ cos ϕ = ∣ a ⋅ ( b × c ) ∣ ■
9.3 Properties of the scalar triple product
Cyclic permutation:
[ a , b , c ] = [ b , c , a ] = [ c , a , b ] [\mathbf{a},\, \mathbf{b},\, \mathbf{c}] = [\mathbf{b},\, \mathbf{c},\, \mathbf{a}] = [\mathbf{c},\, \mathbf{a},\, \mathbf{b}] [ a , b , c ] = [ b , c , a ] = [ c , a , b ]
Anti-symmetry: Swapping any two vectors changes the sign:
[ a , c , b ] = − [ a , b , c ] [\mathbf{a},\, \mathbf{c},\, \mathbf{b}] = -[\mathbf{a},\, \mathbf{b},\, \mathbf{c}] [ a , c , b ] = − [ a , b , c ]
Coplanarity test: a \mathbf{a} a , b \mathbf{b} b , c \mathbf{c} c are coplanar if and only if
[ a , b , c ] = 0 [\mathbf{a},\, \mathbf{b},\, \mathbf{c}] = 0 [ a , b , c ] = 0 (the parallelepiped has zero volume).
Volume of a tetrahedron:
V t e t = 1 6 ∣ a ⋅ ( b × c ) ∣ V_{\mathrm{tet}} = \dfrac{1}{6}|\mathbf{a}\cdot(\mathbf{b}\times\mathbf{c})| V tet = 6 1 ∣ a ⋅ ( b × c ) ∣ , since a
tetrahedron is 1 6 \dfrac{1}{6} 6 1 of a parallelepiped.
Example. Find the volume of the parallelepiped with edges
a = ( 2 0 1 ) \mathbf{a} = \begin{pmatrix}2\\0\\1\end{pmatrix} a = 2 0 1 ,
b = ( 1 3 − 1 ) \mathbf{b} = \begin{pmatrix}1\\3\\-1\end{pmatrix} b = 1 3 − 1 ,
c = ( 0 2 4 ) \mathbf{c} = \begin{pmatrix}0\\2\\4\end{pmatrix} c = 0 2 4 .
[ a , b , c ] = ∣ 2 0 1 1 3 − 1 0 2 4 ∣ [\mathbf{a},\, \mathbf{b},\, \mathbf{c}] = \begin{vmatrix} 2 & 0 & 1 \\ 1 & 3 & -1 \\ 0 & 2 & 4 \end{vmatrix} [ a , b , c ] = 2 1 0 0 3 2 1 − 1 4
= 2 ∣ 3 − 1 2 4 ∣ − 0 ∣ 1 − 1 0 4 ∣ + 1 ∣ 1 3 0 2 ∣ = 2\begin{vmatrix}3 & -1\\2 & 4\end{vmatrix} - 0\begin{vmatrix}1 & -1\\0 & 4\end{vmatrix} + 1\begin{vmatrix}1 & 3\\0 & 2\end{vmatrix} = 2 3 2 − 1 4 − 0 1 0 − 1 4 + 1 1 0 3 2
= 2 ( 12 + 2 ) + 0 + 1 ( 2 ) = 28 + 2 = 30 = 2(12+2) + 0 + 1(2) = 28 + 2 = 30 = 2 ( 12 + 2 ) + 0 + 1 ( 2 ) = 28 + 2 = 30 .
Volume = ∣ 30 ∣ = 30 = |30| = 30 = ∣30∣ = 30 cubic units.
10. Vector Proof Techniques
10.1 Proving collinear points
Points A A A , B B B , C C C are collinear if and only if A B → \overrightarrow{AB} A B is parallel to
B C → \overrightarrow{BC} B C , i.e. A B → = k B C → \overrightarrow{AB} = k\,\overrightarrow{BC} A B = k B C for some scalar k k k .
Equivalently, A B → × B C → = 0 \overrightarrow{AB} \times \overrightarrow{BC} = \mathbf{0} A B × B C = 0 (zero vector).
Method:
Compute A B → = b − a \overrightarrow{AB} = \mathbf{b} - \mathbf{a} A B = b − a and
B C → = c − b \overrightarrow{BC} = \mathbf{c} - \mathbf{b} B C = c − b .
Check if one is a scalar multiple of the other.
Alternatively, check if A C → \overrightarrow{AC} A C is parallel to A B → \overrightarrow{AB} A B .
Example. Show that A ( 1 , 2 , 3 ) A(1, 2, 3) A ( 1 , 2 , 3 ) , B ( 3 , 4 , 5 ) B(3, 4, 5) B ( 3 , 4 , 5 ) , C ( 5 , 6 , 7 ) C(5, 6, 7) C ( 5 , 6 , 7 ) are collinear.
A B → = ( 2 2 2 ) \overrightarrow{AB} = \begin{pmatrix}2\\2\\2\end{pmatrix} A B = 2 2 2 ,
B C → = ( 2 2 2 ) \overrightarrow{BC} = \begin{pmatrix}2\\2\\2\end{pmatrix} B C = 2 2 2 .
Since A B → = B C → \overrightarrow{AB} = \overrightarrow{BC} A B = B C (i.e. k = 1 k = 1 k = 1 ), the points are collinear.
■ \blacksquare ■
10.2 Proving perpendicular lines
Two lines are perpendicular if and only if their direction vectors have dot product zero.
Method:
Identify the direction vectors d 1 \mathbf{d}_1 d 1 and d 2 \mathbf{d}_2 d 2 of the two lines.
Compute d 1 ⋅ d 2 \mathbf{d}_1\cdot\mathbf{d}_2 d 1 ⋅ d 2 .
If the result is zero (and neither direction vector is zero), the lines are perpendicular.
Example. Show that the lines
r 1 = ( 0 1 2 ) + t ( 1 2 − 2 ) \mathbf{r}_1 = \begin{pmatrix}0\\1\\2\end{pmatrix} + t\begin{pmatrix}1\\2\\-2\end{pmatrix} r 1 = 0 1 2 + t 1 2 − 2 and
r 2 = ( 3 0 − 1 ) + s ( 2 − 1 0 ) \mathbf{r}_2 = \begin{pmatrix}3\\0\\-1\end{pmatrix} + s\begin{pmatrix}2\\-1\\0\end{pmatrix} r 2 = 3 0 − 1 + s 2 − 1 0 are
perpendicular.
d 1 ⋅ d 2 = ( 1 ) ( 2 ) + ( 2 ) ( − 1 ) + ( − 2 ) ( 0 ) = 2 − 2 + 0 = 0 \mathbf{d}_1\cdot\mathbf{d}_2 = (1)(2) + (2)(-1) + (-2)(0) = 2 - 2 + 0 = 0 d 1 ⋅ d 2 = ( 1 ) ( 2 ) + ( 2 ) ( − 1 ) + ( − 2 ) ( 0 ) = 2 − 2 + 0 = 0 .
Since the dot product is zero, the lines are perpendicular. ■ \blacksquare ■
Points A A A , B B B , C C C , D D D form a parallelogram (in order) if and only if
A B → = D C → \overrightarrow{AB} = \overrightarrow{DC} A B = D C (or equivalently
A D → = B C → \overrightarrow{AD} = \overrightarrow{BC} A D = B C ).
Method:
Compute the relevant displacement vectors.
Show opposite sides are equal as vectors (same components).
To show a quadrilateral is a rhombus , additionally show that adjacent sides have equal
magnitude. To show a rectangle , show that adjacent sides are perpendicular. A square
requires both conditions.
10.4 Using vectors in geometric proofs
Many geometry problems can be solved elegantly using vectors. The general strategy is:
Assign position vectors to key points.
Express the relevant geometric conditions in vector form (parallelism via scalar multiples,
perpendicularity via dot products, midpoints via averages).
Compute and simplify algebraically.
Example. In triangle A B C ABC A B C , let M M M be the midpoint of A B AB A B . Prove that
C M → = 1 2 C A → + 1 2 C B → \overrightarrow{CM} = \dfrac{1}{2}\overrightarrow{CA} + \dfrac{1}{2}\overrightarrow{CB} C M = 2 1 C A + 2 1 C B .
m = ◆ L B ◆ a + b ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ \mathbf{m} = \dfrac◆LB◆\mathbf{a} + \mathbf{b}◆RB◆◆LB◆2◆RB◆ m = L ◆ B ◆ a + b ◆ R B ◆◆ L B ◆2◆ R B ◆ (midpoint formula).
C M → = m − c = ◆ L B ◆ a + b ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ − c = ◆ L B ◆ a − c ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ + ◆ L B ◆ b − c ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ = 1 2 C A → + 1 2 C B → \overrightarrow{CM} = \mathbf{m} - \mathbf{c} = \dfrac◆LB◆\mathbf{a} + \mathbf{b}◆RB◆◆LB◆2◆RB◆ - \mathbf{c}
= \dfrac◆LB◆\mathbf{a} - \mathbf{c}◆RB◆◆LB◆2◆RB◆ + \dfrac◆LB◆\mathbf{b} - \mathbf{c}◆RB◆◆LB◆2◆RB◆
= \dfrac{1}{2}\overrightarrow{CA} + \dfrac{1}{2}\overrightarrow{CB} C M = m − c = L ◆ B ◆ a + b ◆ R B ◆◆ L B ◆2◆ R B ◆ − c = L ◆ B ◆ a − c ◆ R B ◆◆ L B ◆2◆ R B ◆ + L ◆ B ◆ b − c ◆ R B ◆◆ L B ◆2◆ R B ◆ = 2 1 C A + 2 1 C B .
■ \blacksquare ■
Problem Set
Details
Problem 1
Given
a = 3 i − 2 j + k \mathbf{a} = 3\mathbf{i} - 2\mathbf{j} + \mathbf{k} a = 3 i − 2 j + k and
b = i + 4 j − 3 k \mathbf{b} = \mathbf{i} + 4\mathbf{j} - 3\mathbf{k} b = i + 4 j − 3 k , find
a + b \mathbf{a} + \mathbf{b} a + b ,
a − b \mathbf{a} - \mathbf{b} a − b ,
∣ a ∣ |\mathbf{a}| ∣ a ∣ , and a unit vector in the direction of
a \mathbf{a} a .
Details
Solution 1
a + b = 4 i + 2 j − 2 k = ( 4 2 − 2 ) \mathbf{a} + \mathbf{b} = 4\mathbf{i} + 2\mathbf{j} - 2\mathbf{k} = \begin{pmatrix}4\\2\\-2\end{pmatrix} a + b = 4 i + 2 j − 2 k = 4 2 − 2 .
a − b = 2 i − 6 j + 4 k = ( 2 − 6 4 ) \mathbf{a} - \mathbf{b} = 2\mathbf{i} - 6\mathbf{j} + 4\mathbf{k} = \begin{pmatrix}2\\-6\\4\end{pmatrix} a − b = 2 i − 6 j + 4 k = 2 − 6 4 .
∣ a ∣ = 9 + 4 + 1 = 14 |\mathbf{a}| = \sqrt{9+4+1} = \sqrt{14} ∣ a ∣ = 9 + 4 + 1 = 14 .
a ^ = ◆ L B ◆ 1 ◆ R B ◆◆ L B ◆ 14 ◆ R B ◆ ( 3 − 2 1 ) \hat{\mathbf{a}} = \dfrac◆LB◆1◆RB◆◆LB◆\sqrt{14}◆RB◆\begin{pmatrix}3\\-2\\1\end{pmatrix} a ^ = L ◆ B ◆1◆ R B ◆◆ L B ◆ 14 ◆ R B ◆ 3 − 2 1 .
If you get this wrong, revise:
Magnitude, Unit Vectors — Section 2.
Details
Problem 2
Find the angle between
a = ( 2 1 − 1 ) \mathbf{a} = \begin{pmatrix}2\\1\\-1\end{pmatrix} a = 2 1 − 1 and
b = ( 1 − 3 2 ) \mathbf{b} = \begin{pmatrix}1\\-3\\2\end{pmatrix} b = 1 − 3 2 .
Details
Solution 2
a ⋅ b = 2 − 3 − 2 = − 3 \mathbf{a}\cdot\mathbf{b} = 2-3-2 = -3 a ⋅ b = 2 − 3 − 2 = − 3 .
∣ a ∣ = 4 + 1 + 1 = 6 |\mathbf{a}| = \sqrt{4+1+1} = \sqrt{6} ∣ a ∣ = 4 + 1 + 1 = 6 ,
∣ b ∣ = 1 + 9 + 4 = 14 |\mathbf{b}| = \sqrt{1+9+4} = \sqrt{14} ∣ b ∣ = 1 + 9 + 4 = 14 .
cos θ = ◆ L B ◆ − 3 ◆ R B ◆◆ L B ◆ 6 14 ◆ R B ◆ = ◆ L B ◆ − 3 ◆ R B ◆◆ L B ◆ 84 ◆ R B ◆ = ◆ L B ◆ − 3 ◆ R B ◆◆ L B ◆ 2 21 ◆ R B ◆ = ◆ L B ◆ − 21 ◆ R B ◆◆ L B ◆ 14 ◆ R B ◆ \cos\theta = \dfrac◆LB◆-3◆RB◆◆LB◆\sqrt{6}\sqrt{14}◆RB◆ = \dfrac◆LB◆-3◆RB◆◆LB◆\sqrt{84}◆RB◆ = \dfrac◆LB◆-3◆RB◆◆LB◆2\sqrt{21}◆RB◆ = \dfrac◆LB◆-\sqrt{21}◆RB◆◆LB◆14◆RB◆ cos θ = L ◆ B ◆ − 3◆ R B ◆◆ L B ◆ 6 14 ◆ R B ◆ = L ◆ B ◆ − 3◆ R B ◆◆ L B ◆ 84 ◆ R B ◆ = L ◆ B ◆ − 3◆ R B ◆◆ L B ◆2 21 ◆ R B ◆ = L ◆ B ◆ − 21 ◆ R B ◆◆ L B ◆14◆ R B ◆ .
θ = arccos ( ◆ L B ◆ − 21 ◆ R B ◆◆ L B ◆ 14 ◆ R B ◆ ) ≈ 109.1 ∘ \theta = \arccos\!\left(\dfrac◆LB◆-\sqrt{21}◆RB◆◆LB◆14◆RB◆\right) \approx 109.1^\circ θ = arccos ( L ◆ B ◆ − 21 ◆ R B ◆◆ L B ◆14◆ R B ◆ ) ≈ 109. 1 ∘ .
If you get this wrong, revise: The Scalar (Dot) Product —
Section 4.
Details
Problem 3
Find the vector equation of the line through
A ( 1 , 2 , − 1 ) A(1, 2, -1) A ( 1 , 2 , − 1 ) and
B ( 3 , 0 , 4 ) B(3, 0, 4) B ( 3 , 0 , 4 ) .
Details
Solution 3
Direction:
A B → = ( 3 − 1 0 − 2 4 − ( − 1 ) ) = ( 2 − 2 5 ) \overrightarrow{AB} = \begin{pmatrix}3-1\\0-2\\4-(-1)\end{pmatrix} = \begin{pmatrix}2\\-2\\5\end{pmatrix} A B = 3 − 1 0 − 2 4 − ( − 1 ) = 2 − 2 5 .
r = ( 1 2 − 1 ) + t ( 2 − 2 5 ) \mathbf{r} = \begin{pmatrix}1\\2\\-1\end{pmatrix} + t\begin{pmatrix}2\\-2\\5\end{pmatrix} r = 1 2 − 1 + t 2 − 2 5
If you get this wrong, revise: Vector Equation of a Line —
Section 5.
Details
Problem 4
Show that the lines
r = ( 1 0 2 ) + t ( 2 1 − 1 ) \mathbf{r} = \begin{pmatrix}1\\0\\2\end{pmatrix} + t\begin{pmatrix}2\\1\\-1\end{pmatrix} r = 1 0 2 + t 2 1 − 1 and
r = ( 3 1 1 ) + s ( 1 − 1 1 ) \mathbf{r} = \begin{pmatrix}3\\1\\1\end{pmatrix} + s\begin{pmatrix}1\\-1\\1\end{pmatrix} r = 3 1 1 + s 1 − 1 1 intersect, and find the point of intersection.
Details
Solution 4
Equating components:
1 + 2 t = 3 + s 1+2t = 3+s 1 + 2 t = 3 + s ,
t = 1 − s t = 1-s t = 1 − s ,
2 − t = 1 + s 2-t = 1+s 2 − t = 1 + s .
From t = 1 − s t = 1-s t = 1 − s and 2 − t = 1 + s 2-t = 1+s 2 − t = 1 + s : 2 − ( 1 − s ) = 1 + s ⟹ 1 + s = 1 + s 2-(1-s) = 1+s \implies 1+s = 1+s 2 − ( 1 − s ) = 1 + s ⟹ 1 + s = 1 + s ✓ (consistent).
Check first: 1 + 2 ( 1 − s ) = 3 + s ⟹ 3 − 2 s = 3 + s ⟹ s = 0 1+2(1-s) = 3+s \implies 3-2s = 3+s \implies s = 0 1 + 2 ( 1 − s ) = 3 + s ⟹ 3 − 2 s = 3 + s ⟹ s = 0 , t = 1 t = 1 t = 1 .
Point: ( 1 + 2 0 + 1 2 − 1 ) = ( 3 1 1 ) \begin{pmatrix}1+2\\0+1\\2-1\end{pmatrix} = \begin{pmatrix}3\\1\\1\end{pmatrix} 1 + 2 0 + 1 2 − 1 = 3 1 1 .
If you get this wrong, revise: Intersection of Lines — Section 6.
Details
Problem 5
Find
λ \lambda λ such that
( λ 3 − 1 ) \begin{pmatrix}\lambda\\3\\-1\end{pmatrix} λ 3 − 1 is perpendicular to
( 2 λ 4 ) \begin{pmatrix}2\\\lambda\\4\end{pmatrix} 2 λ 4 .
Details
Solution 5
Perpendicular
⟺ \iff ⟺ dot product
= 0 = 0 = 0 :
2 λ + 3 λ − 4 = 0 ⟹ 5 λ = 4 ⟹ λ = 4 5 2\lambda + 3\lambda - 4 = 0 \implies 5\lambda = 4 \implies \lambda = \frac{4}{5} 2 λ + 3 λ − 4 = 0 ⟹ 5 λ = 4 ⟹ λ = 5 4
If you get this wrong, revise: Perpendicularity test — Section 4.3.
Details
Problem 6
Find the distance from
P ( 1 , 2 , 3 ) P(1, 2, 3) P ( 1 , 2 , 3 ) to the line
r = ( 0 1 − 1 ) + t ( 1 1 1 ) \mathbf{r} = \begin{pmatrix}0\\1\\-1\end{pmatrix} + t\begin{pmatrix}1\\1\\1\end{pmatrix} r = 0 1 − 1 + t 1 1 1 .
Details
Solution 6
P Q → = ( t 1 + t − 1 + t ) − ( 1 2 3 ) = ( t − 1 t − 1 t − 4 ) \overrightarrow{PQ} = \begin{pmatrix}t\\1+t\\-1+t\end{pmatrix} - \begin{pmatrix}1\\2\\3\end{pmatrix} = \begin{pmatrix}t-1\\t-1\\t-4\end{pmatrix} P Q = t 1 + t − 1 + t − 1 2 3 = t − 1 t − 1 t − 4 .
P Q → ⋅ ( 1 1 1 ) = 0 \overrightarrow{PQ} \cdot \begin{pmatrix}1\\1\\1\end{pmatrix} = 0 P Q ⋅ 1 1 1 = 0 :
( t − 1 ) + ( t − 1 ) + ( t − 4 ) = 0 ⟹ 3 t = 6 ⟹ t = 2 (t-1)+(t-1)+(t-4) = 0 \implies 3t = 6 \implies t = 2 ( t − 1 ) + ( t − 1 ) + ( t − 4 ) = 0 ⟹ 3 t = 6 ⟹ t = 2 .
Q = ( 2 3 1 ) Q = \begin{pmatrix}2\\3\\1\end{pmatrix} Q = 2 3 1 ,
P Q → = ( 1 1 − 2 ) \overrightarrow{PQ} = \begin{pmatrix}1\\1\\-2\end{pmatrix} P Q = 1 1 − 2 ,
∣ P Q → ∣ = 1 + 1 + 4 = 6 |\overrightarrow{PQ}| = \sqrt{1+1+4} = \sqrt{6} ∣ P Q ∣ = 1 + 1 + 4 = 6 .
If you get this wrong, revise:
Distance from a Point to a Line — Section 8.
Details
Problem 7
Prove that the direction cosines satisfy
cos 2 α + cos 2 β + cos 2 γ = 1 \cos^2\alpha + \cos^2\beta + \cos^2\gamma = 1 cos 2 α + cos 2 β + cos 2 γ = 1 .
Details
Solution 7
For
a = ( a 1 a 2 a 3 ) \mathbf{a} = \begin{pmatrix}a_1\\a_2\\a_3\end{pmatrix} a = a 1 a 2 a 3 with
∣ a ∣ = m |\mathbf{a}| = m ∣ a ∣ = m :
cos α = a 1 / m \cos\alpha = a_1/m cos α = a 1 / m , cos β = a 2 / m \cos\beta = a_2/m cos β = a 2 / m , cos γ = a 3 / m \cos\gamma = a_3/m cos γ = a 3 / m .
cos 2 α + cos 2 β + cos 2 γ = a 1 2 + a 2 2 + a 3 2 m 2 = m 2 m 2 = 1 ■ \cos^2\alpha + \cos^2\beta + \cos^2\gamma = \frac{a_1^2+a_2^2+a_3^2}{m^2} = \frac{m^2}{m^2} = 1 \quad \blacksquare cos 2 α + cos 2 β + cos 2 γ = m 2 a 1 2 + a 2 2 + a 3 2 = m 2 m 2 = 1 ■
If you get this wrong, revise: Direction Cosines — Section 2.3.
Details
Problem 8
Points
A A A ,
B B B ,
C C C have position vectors
a = ( 1 − 1 2 ) \mathbf{a} = \begin{pmatrix}1\\-1\\2\end{pmatrix} a = 1 − 1 2 ,
b = ( 3 1 0 ) \mathbf{b} = \begin{pmatrix}3\\1\\0\end{pmatrix} b = 3 1 0 ,
c = ( 4 0 3 ) \mathbf{c} = \begin{pmatrix}4\\0\\3\end{pmatrix} c = 4 0 3 . Determine whether
△ A B C \triangle ABC △ A B C is right-angled.
Details
Solution 8
A B → = ( 2 2 − 2 ) \overrightarrow{AB} = \begin{pmatrix}2\\2\\-2\end{pmatrix} A B = 2 2 − 2 ,
A C → = ( 3 1 1 ) \overrightarrow{AC} = \begin{pmatrix}3\\1\\1\end{pmatrix} A C = 3 1 1 ,
B C → = ( 1 − 1 3 ) \overrightarrow{BC} = \begin{pmatrix}1\\-1\\3\end{pmatrix} B C = 1 − 1 3 .
A B → ⋅ A C → = 6 + 2 − 2 = 6 ≠ 0 \overrightarrow{AB}\cdot\overrightarrow{AC} = 6+2-2 = 6 \neq 0 A B ⋅ A C = 6 + 2 − 2 = 6 = 0 .
A B → ⋅ B C → = 2 − 2 − 6 = − 6 ≠ 0 \overrightarrow{AB}\cdot\overrightarrow{BC} = 2-2-6 = -6 \neq 0 A B ⋅ B C = 2 − 2 − 6 = − 6 = 0 .
A C → ⋅ B C → = 3 − 1 + 3 = 5 ≠ 0 \overrightarrow{AC}\cdot\overrightarrow{BC} = 3-1+3 = 5 \neq 0 A C ⋅ B C = 3 − 1 + 3 = 5 = 0 .
No pair is perpendicular, so △ A B C \triangle ABC △ A B C is not right-angled.
If you get this wrong, revise: Perpendicularity test — Section 4.3.
Details
Problem 9
Show that the lines
r = ( 0 0 1 ) + t ( 1 1 0 ) \mathbf{r} = \begin{pmatrix}0\\0\\1\end{pmatrix} + t\begin{pmatrix}1\\1\\0\end{pmatrix} r = 0 0 1 + t 1 1 0 and
r = ( 0 1 0 ) + s ( 1 0 1 ) \mathbf{r} = \begin{pmatrix}0\\1\\0\end{pmatrix} + s\begin{pmatrix}1\\0\\1\end{pmatrix} r = 0 1 0 + s 1 0 1 intersect, and find the point of intersection.
Details
Solution 9
Equating:
t = s t = s t = s ,
t = 1 t = 1 t = 1 ,
1 = s 1 = s 1 = s .
From t = 1 t = 1 t = 1 and t = s t = s t = s : s = 1 s = 1 s = 1 . Check third: 1 = s = 1 1 = s = 1 1 = s = 1 ✓.
Wait — all three are consistent! Let me re-check. Line 1: ( t , t , 1 ) (t, t, 1) ( t , t , 1 ) . Line 2: ( s , 1 , s ) (s, 1, s) ( s , 1 , s ) .
t = s t = s t = s , t = 1 t = 1 t = 1 , 1 = s 1 = s 1 = s . So t = s = 1 t = s = 1 t = s = 1 . Point: ( 1 , 1 , 1 ) (1, 1, 1) ( 1 , 1 , 1 ) .
Actually the lines intersect at ( 1 , 1 , 1 ) (1,1,1) ( 1 , 1 , 1 ) , they are not skew.
If you get this wrong, revise: Skew Lines — Section 6.2.
Details
Problem 10
Given
a = 2 i + j \mathbf{a} = 2\mathbf{i} + \mathbf{j} a = 2 i + j and
b = i − 3 j \mathbf{b} = \mathbf{i} - 3\mathbf{j} b = i − 3 j , find the vector projection of
b \mathbf{b} b onto
a \mathbf{a} a .
Details
Solution 10
The projection of
b \mathbf{b} b onto
a \mathbf{a} a is
p r o j a b = ◆ L B ◆ a ⋅ b ◆ R B ◆◆ L B ◆ ∣ a ∣ 2 ◆ R B ◆ a \mathrm{proj}_{\mathbf{a}}\mathbf{b} = \dfrac◆LB◆\mathbf{a}\cdot\mathbf{b}◆RB◆◆LB◆|\mathbf{a}|^2◆RB◆\,\mathbf{a} proj a b = L ◆ B ◆ a ⋅ b ◆ R B ◆◆ L B ◆∣ a ∣ 2 ◆ R B ◆ a .
a ⋅ b = 2 − 3 = − 1 \mathbf{a}\cdot\mathbf{b} = 2-3 = -1 a ⋅ b = 2 − 3 = − 1 . ∣ a ∣ 2 = 4 + 1 = 5 |\mathbf{a}|^2 = 4+1 = 5 ∣ a ∣ 2 = 4 + 1 = 5 .
p r o j a b = − 1 5 ( 2 i + j ) = − 2 5 i − 1 5 j \mathrm{proj}_{\mathbf{a}}\mathbf{b} = \frac{-1}{5}(2\mathbf{i}+\mathbf{j}) = -\frac{2}{5}\mathbf{i} - \frac{1}{5}\mathbf{j} proj a b = 5 − 1 ( 2 i + j ) = − 5 2 i − 5 1 j
If you get this wrong, revise: Geometric Interpretation —
Section 4.2.
Details
Problem 11
Find the angle between the line
r = ( 1 2 − 1 ) + t ( 3 − 1 2 ) \mathbf{r} = \begin{pmatrix}1\\2\\-1\end{pmatrix} + t\begin{pmatrix}3\\-1\\2\end{pmatrix} r = 1 2 − 1 + t 3 − 1 2 and the plane
2 x − y + z = 5 2x - y + z = 5 2 x − y + z = 5 .
Details
Solution 11
The normal to the plane is
n = ( 2 − 1 1 ) \mathbf{n} = \begin{pmatrix}2\\-1\\1\end{pmatrix} n = 2 − 1 1 , and the direction of the line is
d = ( 3 − 1 2 ) \mathbf{d} = \begin{pmatrix}3\\-1\\2\end{pmatrix} d = 3 − 1 2 .
The angle between the line and the plane equals 90 ∘ 90^\circ 9 0 ∘ minus the angle between d \mathbf{d} d and
n \mathbf{n} n .
cos ϕ = ◆ L B ◆ d ⋅ n ◆ R B ◆◆ L B ◆ ∣ d ∣ ∣ n ∣ ◆ R B ◆ = ◆ L B ◆ 6 + 1 + 2 ◆ R B ◆◆ L B ◆ 14 6 ◆ R B ◆ = ◆ L B ◆ 9 ◆ R B ◆◆ L B ◆ 2 21 ◆ R B ◆ \cos\phi = \dfrac◆LB◆\mathbf{d}\cdot\mathbf{n}◆RB◆◆LB◆|\mathbf{d}||\mathbf{n}|◆RB◆ = \dfrac◆LB◆6+1+2◆RB◆◆LB◆\sqrt{14}\sqrt{6}◆RB◆ = \dfrac◆LB◆9◆RB◆◆LB◆2\sqrt{21}◆RB◆ cos ϕ = L ◆ B ◆ d ⋅ n ◆ R B ◆◆ L B ◆∣ d ∣∣ n ∣◆ R B ◆ = L ◆ B ◆6 + 1 + 2◆ R B ◆◆ L B ◆ 14 6 ◆ R B ◆ = L ◆ B ◆9◆ R B ◆◆ L B ◆2 21 ◆ R B ◆ .
Angle between line and normal: ϕ = arccos ( ◆ L B ◆ 9 ◆ R B ◆◆ L B ◆ 2 21 ◆ R B ◆ ) \phi = \arccos\!\left(\dfrac◆LB◆9◆RB◆◆LB◆2\sqrt{21}◆RB◆\right) ϕ = arccos ( L ◆ B ◆9◆ R B ◆◆ L B ◆2 21 ◆ R B ◆ ) .
Angle between line and plane: 90 ° − ϕ 90° - \phi 90° − ϕ .
If you get this wrong, revise: Angle Between Two Vectors —
Section 7.
Details
Problem 12
Find the direction cosines of the vector
v = ( 1 − 2 2 ) \mathbf{v} = \begin{pmatrix}1\\-2\\2\end{pmatrix} v = 1 − 2 2 , and verify that they satisfy
cos 2 α + cos 2 β + cos 2 γ = 1 \cos^2\alpha + \cos^2\beta + \cos^2\gamma = 1 cos 2 α + cos 2 β + cos 2 γ = 1 .
Details
Solution 12
∣ v ∣ = 1 + 4 + 4 = 9 = 3 |\mathbf{v}| = \sqrt{1 + 4 + 4} = \sqrt{9} = 3 ∣ v ∣ = 1 + 4 + 4 = 9 = 3 .
cos α = 1 3 \cos\alpha = \dfrac{1}{3} cos α = 3 1 , cos β = − 2 3 \quad \cos\beta = \dfrac{-2}{3} cos β = 3 − 2 , cos γ = 2 3 \quad \cos\gamma = \dfrac{2}{3} cos γ = 3 2 .
Check:
cos 2 α + cos 2 β + cos 2 γ = 1 9 + 4 9 + 4 9 = 9 9 = 1 \cos^2\alpha + \cos^2\beta + \cos^2\gamma = \dfrac{1}{9} + \dfrac{4}{9} + \dfrac{4}{9} = \dfrac{9}{9} = 1 cos 2 α + cos 2 β + cos 2 γ = 9 1 + 9 4 + 9 4 = 9 9 = 1 .
✓
The angles are α = arccos ( 1 / 3 ) ≈ 70.5 ∘ \alpha = \arccos(1/3) \approx 70.5^\circ α = arccos ( 1/3 ) ≈ 70. 5 ∘ ,
β = arccos ( − 2 / 3 ) ≈ 131.8 ∘ \beta = \arccos(-2/3) \approx 131.8^\circ β = arccos ( − 2/3 ) ≈ 131. 8 ∘ , γ = arccos ( 2 / 3 ) ≈ 48.2 ∘ \gamma = \arccos(2/3) \approx 48.2^\circ γ = arccos ( 2/3 ) ≈ 48. 2 ∘ .
If you get this wrong, revise: Direction Cosines — Section 2.3.
Details
Problem 13
Find the vector equation of the line through
A ( 2 , − 3 , 1 ) A(2, -3, 1) A ( 2 , − 3 , 1 ) that is parallel to the line
r = ( 0 1 − 2 ) + t ( 4 − 1 3 ) \mathbf{r} = \begin{pmatrix}0\\1\\-2\end{pmatrix} + t\begin{pmatrix}4\\-1\\3\end{pmatrix} r = 0 1 − 2 + t 4 − 1 3 .
Details
Solution 13
Since the line is parallel, it has the same direction vector
( 4 − 1 3 ) \begin{pmatrix}4\\-1\\3\end{pmatrix} 4 − 1 3 .
Using point A ( 2 , − 3 , 1 ) A(2, -3, 1) A ( 2 , − 3 , 1 ) :
r = ( 2 − 3 1 ) + t ( 4 − 1 3 ) \mathbf{r} = \begin{pmatrix}2\\-3\\1\end{pmatrix} + t\begin{pmatrix}4\\-1\\3\end{pmatrix} r = 2 − 3 1 + t 4 − 1 3
If you get this wrong, revise:
Vector Equation of a Line in 3D — Section 5.4.
Details
Problem 14
Find the volume of the parallelepiped with edges
a = ( 1 0 2 ) \mathbf{a} = \begin{pmatrix}1\\0\\2\end{pmatrix} a = 1 0 2 ,
b = ( 3 1 − 1 ) \mathbf{b} = \begin{pmatrix}3\\1\\-1\end{pmatrix} b = 3 1 − 1 ,
c = ( − 1 2 1 ) \mathbf{c} = \begin{pmatrix}-1\\2\\1\end{pmatrix} c = − 1 2 1 .
Details
Solution 14
[ a , b , c ] = ∣ 1 0 2 3 1 − 1 − 1 2 1 ∣ [\mathbf{a},\, \mathbf{b},\, \mathbf{c}] = \begin{vmatrix} 1 & 0 & 2 \\ 3 & 1 & -1 \\ -1 & 2 & 1 \end{vmatrix} [ a , b , c ] = 1 3 − 1 0 1 2 2 − 1 1
= 1 ∣ 1 − 1 2 1 ∣ − 0 ∣ 3 − 1 − 1 1 ∣ + 2 ∣ 3 1 − 1 2 ∣ = 1\begin{vmatrix}1 & -1\\2 & 1\end{vmatrix} - 0\begin{vmatrix}3 & -1\\-1 & 1\end{vmatrix} + 2\begin{vmatrix}3 & 1\\-1 & 2\end{vmatrix} = 1 1 2 − 1 1 − 0 3 − 1 − 1 1 + 2 3 − 1 1 2
= 1 ( 1 + 2 ) + 0 + 2 ( 6 + 1 ) = 3 + 14 = 17 = 1(1+2) + 0 + 2(6+1) = 3 + 14 = 17 = 1 ( 1 + 2 ) + 0 + 2 ( 6 + 1 ) = 3 + 14 = 17 .
Volume = ∣ 17 ∣ = 17 = |17| = 17 = ∣17∣ = 17 cubic units.
Volume of the tetrahedron = 17 6 = \dfrac{17}{6} = 6 17 cubic units.
If you get this wrong, revise: Scalar Triple Product — Section 9.
Details
Problem 15
Determine whether the points
P ( 1 , 2 , 3 ) P(1, 2, 3) P ( 1 , 2 , 3 ) ,
Q ( 4 , 5 , 6 ) Q(4, 5, 6) Q ( 4 , 5 , 6 ) ,
R ( 7 , 8 , 9 ) R(7, 8, 9) R ( 7 , 8 , 9 ) are collinear. If they are, find the ratio
P Q : Q R PQ : QR P Q : QR .
Details
Solution 15
P Q → = ( 3 3 3 ) \overrightarrow{PQ} = \begin{pmatrix}3\\3\\3\end{pmatrix} P Q = 3 3 3 ,
Q R → = ( 3 3 3 ) \overrightarrow{QR} = \begin{pmatrix}3\\3\\3\end{pmatrix} QR = 3 3 3 .
Since P Q → = Q R → \overrightarrow{PQ} = \overrightarrow{QR} P Q = QR , the points are collinear. The ratio is
P Q : Q R = 1 : 1 PQ : QR = 1 : 1 P Q : QR = 1 : 1 .
If you get this wrong, revise: Proving Collinear Points —
Section 10.1.
Details
Problem 16
Show that the lines
r 1 = ( 1 0 0 ) + t ( 1 2 3 ) \mathbf{r}_1 = \begin{pmatrix}1\\0\\0\end{pmatrix} + t\begin{pmatrix}1\\2\\3\end{pmatrix} r 1 = 1 0 0 + t 1 2 3 and
r 2 = ( 0 1 − 1 ) + s ( 2 − 1 1 ) \mathbf{r}_2 = \begin{pmatrix}0\\1\\-1\end{pmatrix} + s\begin{pmatrix}2\\-1\\1\end{pmatrix} r 2 = 0 1 − 1 + s 2 − 1 1 are skew.
Details
Solution 16
Equating components:
1 + t = 2 s 1+t = 2s 1 + t = 2 s ,
2 t = 1 − s 2t = 1-s 2 t = 1 − s ,
3 t = − 1 + s 3t = -1+s 3 t = − 1 + s .
From equation 2: s = 1 − 2 t s = 1 - 2t s = 1 − 2 t . Substitute into equation 1:
1 + t = 2 ( 1 − 2 t ) = 2 − 4 t ⟹ 5 t = 1 ⟹ t = 1 / 5 1+t = 2(1-2t) = 2-4t \implies 5t = 1 \implies t = 1/5 1 + t = 2 ( 1 − 2 t ) = 2 − 4 t ⟹ 5 t = 1 ⟹ t = 1/5 .
Then s = 1 − 2 / 5 = 3 / 5 s = 1 - 2/5 = 3/5 s = 1 − 2/5 = 3/5 .
Check equation 3: 3 ( 1 / 5 ) = 3 / 5 3(1/5) = 3/5 3 ( 1/5 ) = 3/5 and − 1 + 3 / 5 = − 2 / 5 -1 + 3/5 = -2/5 − 1 + 3/5 = − 2/5 .
3 / 5 ≠ − 2 / 5 3/5 \neq -2/5 3/5 = − 2/5 , so the third equation is inconsistent . The lines are skew. ■ \blacksquare ■
If you get this wrong, revise: Skew Lines — Section 6.2.
Details
Problem 17
Find the shortest distance from the point
P ( 3 , − 1 , 2 ) P(3, -1, 2) P ( 3 , − 1 , 2 ) to the line
r = ( 1 2 − 1 ) + t ( 1 0 3 ) \mathbf{r} = \begin{pmatrix}1\\2\\-1\end{pmatrix} + t\begin{pmatrix}1\\0\\3\end{pmatrix} r = 1 2 − 1 + t 1 0 3 .
Details
Solution 17
Let
a = ( 1 2 − 1 ) \mathbf{a} = \begin{pmatrix}1\\2\\-1\end{pmatrix} a = 1 2 − 1 ,
d = ( 1 0 3 ) \mathbf{d} = \begin{pmatrix}1\\0\\3\end{pmatrix} d = 1 0 3 ,
p = ( 3 − 1 2 ) \mathbf{p} = \begin{pmatrix}3\\-1\\2\end{pmatrix} p = 3 − 1 2 .
A P → = p − a = ( 2 − 3 3 ) \overrightarrow{AP} = \mathbf{p} - \mathbf{a} = \begin{pmatrix}2\\-3\\3\end{pmatrix} A P = p − a = 2 − 3 3 .
P Q → = a + t d − p = ( t − 2 t + 2 − 1 + 3 t − 2 ) = ( t − 2 t + 2 3 t − 3 ) \overrightarrow{PQ} = \mathbf{a} + t\mathbf{d} - \mathbf{p} = \begin{pmatrix}t-2\\t+2\\-1+3t-2\end{pmatrix} = \begin{pmatrix}t-2\\t+2\\3t-3\end{pmatrix} P Q = a + t d − p = t − 2 t + 2 − 1 + 3 t − 2 = t − 2 t + 2 3 t − 3 .
Set P Q → ⋅ d = 0 \overrightarrow{PQ}\cdot\mathbf{d} = 0 P Q ⋅ d = 0 : ( t − 2 ) ( 1 ) + ( t + 2 ) ( 0 ) + ( 3 t − 3 ) ( 3 ) = 0 (t-2)(1) + (t+2)(0) + (3t-3)(3) = 0 ( t − 2 ) ( 1 ) + ( t + 2 ) ( 0 ) + ( 3 t − 3 ) ( 3 ) = 0
t − 2 + 9 t − 9 = 0 ⟹ 10 t = 11 ⟹ t = 11 / 10 t - 2 + 9t - 9 = 0 \implies 10t = 11 \implies t = 11/10 t − 2 + 9 t − 9 = 0 ⟹ 10 t = 11 ⟹ t = 11/10 .
Q = ( 1 + 11 / 10 2 − 1 + 33 / 10 ) = ( 21 / 10 2 23 / 10 ) Q = \begin{pmatrix}1+11/10\\2\\-1+33/10\end{pmatrix} = \begin{pmatrix}21/10\\2\\23/10\end{pmatrix} Q = 1 + 11/10 2 − 1 + 33/10 = 21/10 2 23/10 .
P Q → = ( 21 / 10 − 3 2 − ( − 1 ) 23 / 10 − 2 ) = ( − 9 / 10 3 3 / 10 ) \overrightarrow{PQ} = \begin{pmatrix}21/10-3\\2-(-1)\\23/10-2\end{pmatrix} = \begin{pmatrix}-9/10\\3\\3/10\end{pmatrix} P Q = 21/10 − 3 2 − ( − 1 ) 23/10 − 2 = − 9/10 3 3/10 .
d = 81 / 100 + 9 + 9 / 100 = 81 / 100 + 900 / 100 + 9 / 100 = 990 / 100 = ◆ L B ◆ 3 110 ◆ R B ◆◆ L B ◆ 10 ◆ R B ◆ d = \sqrt{81/100 + 9 + 9/100} = \sqrt{81/100 + 900/100 + 9/100} = \sqrt{990/100} = \dfrac◆LB◆3\sqrt{110}◆RB◆◆LB◆10◆RB◆ d = 81/100 + 9 + 9/100 = 81/100 + 900/100 + 9/100 = 990/100 = L ◆ B ◆3 110 ◆ R B ◆◆ L B ◆10◆ R B ◆ .
If you get this wrong, revise:
Distance from a Point to a Line — Section 8.
Details
Problem 18
Points
A A A ,
B B B ,
C C C ,
D D D have position vectors
a = ( 0 0 0 ) \mathbf{a} = \begin{pmatrix}0\\0\\0\end{pmatrix} a = 0 0 0 ,
b = ( 4 1 − 2 ) \mathbf{b} = \begin{pmatrix}4\\1\\-2\end{pmatrix} b = 4 1 − 2 ,
c = ( 6 3 1 ) \mathbf{c} = \begin{pmatrix}6\\3\\1\end{pmatrix} c = 6 3 1 ,
d = ( 2 2 3 ) \mathbf{d} = \begin{pmatrix}2\\2\\3\end{pmatrix} d = 2 2 3 . Show that
A B C D ABCD A B C D is a parallelogram, and determine whether it is a rectangle.
Details
Solution 18
A B → = ( 4 1 − 2 ) \overrightarrow{AB} = \begin{pmatrix}4\\1\\-2\end{pmatrix} A B = 4 1 − 2 ,
D C → = c − d = ( 4 1 − 2 ) \overrightarrow{DC} = \mathbf{c} - \mathbf{d} = \begin{pmatrix}4\\1\\-2\end{pmatrix} D C = c − d = 4 1 − 2 .
Since A B → = D C → \overrightarrow{AB} = \overrightarrow{DC} A B = D C , A B C D ABCD A B C D is a parallelogram. ✓
Check for rectangle:
A B → ⋅ A D → = ( 4 1 − 2 ) ⋅ ( 2 2 3 ) = 8 + 2 − 6 = 4 ≠ 0 \overrightarrow{AB}\cdot\overrightarrow{AD} = \begin{pmatrix}4\\1\\-2\end{pmatrix}\cdot\begin{pmatrix}2\\2\\3\end{pmatrix} = 8 + 2 - 6 = 4 \neq 0 A B ⋅ A D = 4 1 − 2 ⋅ 2 2 3 = 8 + 2 − 6 = 4 = 0 .
The adjacent sides are not perpendicular, so A B C D ABCD A B C D is not a rectangle.
If you get this wrong, revise:
Proving Points Form a Parallelogram — Section 10.3.
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tip
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