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Vectors in Two and Three Dimensions, Summaries of Algebra

The concept of vectors in two and three dimensions. It covers the terminology, notation, and conversion between magnitude-direction form and component form. It also introduces the use of unit vectors and position vectors in three dimensions. Examples are provided throughout the document to illustrate the concepts.

Typology: Summaries

2021/2022

Available from 02/27/2023

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Vector
8
5
30°
P1
8
Vectors
We drove into the future looking into a rear view mirror.
Herbert Marshall McLuhan
?
What
information
do
you
need
to decide how close the aircraft
which left these vapour trails
passed to each other?
A quantity which has both size and direction is called a vector. The velocity of
an aircraft through the sky is an example of a vector, having size (e.g. 600 mph)
and direction (on a course of 254°). By contrast the mass of the aircraft (100
tonnes) is completely described by its size and no direction is associated with it;
such a quantity is called a scalar.
Vectors are used extensively in mechanics to represent quantities such as force,
velocity and momentum, and in geometry to represent displacements. They
are an essential tool in three-dimensional co-ordinate geometry and it is this
application of vectors which is the subject of this chapter. However, before
coming on to this, you need to be familiar with the associated vocabulary and
notation, in two and three dimensions.
Vectors in two dimensions
Terminology
In two dimensions, it is common to represent a vector by a drawing of a straight
line with an arrowhead. The length represents the size, or magnitude, of the
vector and the direction is indicated by the line and the arrowhead. Direction is
usually given as the angle the vector makes with the positive x axis, with the
anticlockwise direction taken to be positive.
The vector in figure 8.1 has magnitude 5,
direction 30°. This is written (5, 30°) and
254
said to be in magnitudedirection form or
in
polar form. The general form of a vector
written in this way is (r, θ) where r is its
magnitude and θ its direction.
+
Figure 8.1
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pfa
pfd
pfe
pff
pf12
pf13
pf14
pf15
pf16
pf17
pf18
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pf1a
pf1b
pf1c
pf1d
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Vector

5 30°

P

Vectors We drove into the future looking into a rear view mirror. Herbert Marshall McLuhan

●?^ What^ information^ do^ you^ need

to decide how close the aircraft which left these vapour trails passed to each other? A quantity which has both size and direction is called a vector. The velocity of an aircraft through the sky is an example of a vector, having size (e.g. 600 mph) and direction (on a course of 254°). By contrast the mass of the aircraft ( tonnes) is completely described by its size and no direction is associated with it; such a quantity is called a scalar. Vectors are used extensively in mechanics to represent quantities such as force, velocity and momentum, and in geometry to represent displacements. They are an essential tool in three-dimensional co-ordinate geometry and it is this application of vectors which is the subject of this chapter. However, before coming on to this, you need to be familiar with the associated vocabulary and notation, in two and three dimensions.

Vectors in two dimensions

Terminology In two dimensions, it is common to represent a vector by a drawing of a straight line with an arrowhead. The length represents the size, or magnitude, of the vector and the direction is indicated by the line and the arrowhead. Direction is usually given as the angle the vector makes with the positive x axis, with the anticlockwise direction taken to be positive. The vector in figure 8.1 has magnitude 5, direction 30°. This is written (5, 30°) and 254 said to be in magnitudedirection form or in polar form. The general form of a vector written in this way is ( r , θ ) where r is its magnitude and θ its direction.

Figure 8.

4

2 )

or 4 i + 2 j

a

θ

Note

In the special case when the vector is representing real travel, as in the case of

the velocity of an aircraft, the direction may be described by a compass bearing

with the angle measured from north, clockwise. However, this is not

done in this chapter, where directions are all taken to be measured

anticlockwise from the positive x direction.

An alternative way of describing a vector is in terms of components in given

directions. The vector in figure 8.2 is 4 units in the x direction, and 2 in the

y direction, and this is denoted by

2

4

Figure 8.

This may also be written as 4 i  2 j , where i is a vector of magnitude 1, a unit

vector , in the x direction and j is a unit vector in the y direction (figure 8.3).

j

i

Figure 8.

In a book, a vector may be printed in bold, for example p or OP , or as a line  between two points with an arrow above it to indicate its direction, such as

OP.

When you write a vector by hand, it is usual to underline it, for example, p or OP ,



or to put an arrow above it, as in OP.

To convert a vector from component form to magnitudedirection form, or vice

versa, is just a matter of applying trigonometry to a right-angled triangle.

Write the vector a  4 i  2 j in magnitudedirection form.

SOLUTION

2

4

Figure

8

.

4

EXAMPLE 8.

Vectors

in

two

dimensions

P

4

P

5

60°

290°

10

The magnitude of a is given by the length a in figure 8.4.

a  (using Pythagoras’ theorem)

4.47 (to 3 significant figures)

The direction is given by the angle θ.

tan θ

2 0.

θ 26.6° (to 3 significant figures)

The vector a is (4.47, 26.6°).

The magnitude of a vector is also called its modulus and denoted by the

symbols

 . In the example a  4 i  2 j , the modulus of a , written  a , is 4.47. Another

convention for writing the magnitude of a vector is to use the same letter, but

in italics and not bold type; thus the magnitude of a may be written a.

Write the vector (5, 60°) in component form.

SOLUTION

In the right-angled triangle OPX

OX  5 cos 60° 2.

XP  5 sin 60° 4.33 j

(to 2 decimal places) O

i X

Figure 8.

OP is  

or 2.5 i 4.33 j.

This technique can be written as a general rule, for all values of θ.

r^ cos

( r , θ )  

r sin

( r cos θ ) i + ( r sin θ ) j

Write the vector (10, 290°) in component form.

SOLUTION

In this case r  10 and θ 290°.

 10 cos 290 

to 2 decimal places.

 10 sin 290 

This may also be written 3.42 i 9.40 j.

Figure 8.

256

EXAMPLE 8.

EXAMPLE 8.

Vector s

P

5

4 j length 4 r

j

αθ

  • 5 i length 5 O i

In Example 8.3 the signs looked after themselves. The component in the i

direction came out positive, that in the j direction negative, as must be the case for

a direction in the fourth quadrant (270° < θ < 360°). This will always be the case

when the conversion is from magnitudedirection form into component form.

The situation is not quite so straightforward when the conversion is carried out

the other way, from component form to magnitudedirection form. In that

case, it is best to draw a diagram and use it to see the approximate size of the

angle required. This is shown in the next example.

Write  5 i  4 j in magnitudedirection form.

SOLUTION

Figure 8.

In this case, the magnitude r

6.40 (to 2 decimal places).

The direction is given by the angle θ in figure 8.7, but first find the angle α.

tan α

4

 α 38.7° (to nearest 0.1°)

so θ  180  α 141.3°

The vector is (6.40, 141.3°) in magnitudedirection form.

257

EXAMPLE 8.

Vectors

in

two

dimensions

P

a

a

a

a

k

i (^) j

Equal vectors

The statement that two vectors a and b are equal means two things.

● The direction of a is the same as the direction of b.

● The magnitude of a is the same as the magnitude of b.

If the vectors are given in component form, each component of a equals the

corresponding component of b.

Position vectors

Saying the vector a is given by 3 i  4 jk tells you the components of the vector, or

equivalently its magnitude and direction. It does not tell you where the vector

is situated; indeed it could be anywhere.

All of the lines in figure 8.9 represent the vector a.

Figure 8.

There is, however, one special case which is an exception to the rule, that of a

vector which starts at the origin. This is called a position vector. Thus the line

joining the origin to the point P(3, 4, 1) is the position vector  4 or 3 i  4 jk.

Another way of expressing this is to say that the point P(3, 4, 1) has the position

^3 

vector  4 .

259

Vectors

in

three

dimensions

P

8

P

y 4 3 L 2 N 1

  • 2 – 1O 1 2 3 4 x

M – 1 Points L, M and N have co-ordinates (4, 3), (2, 1) and (2, 2).  (i) Write down, in component form, the position vector of L and the vector MN. (ii) What do your answers to part (i) tell you about the lines OL and MN? SOLUTIO N (i)  

^4 

.

The position vector of L is

OL

  3  

 ^4  The vector MN is also   3

(see figure 8.10).   (ii) Since OL MN, lines OL and MN are parallel and equal in length. Figure 8. Note A line joining two points, like MN in figure 8.10, is often called a line segment , meaning that it is just that particular part of the infinite straight line that passes through those two points.  The vector MN is an example of a displacement vector. Its length represents the magnitude of the displacement when you move from M to N. The length of a vector In two dimensions, the use of Pythagoras’ theorem leads to the result that a vector a 1 ia 2 j has length  a given by  a  a 2  a 2 . 1 2 260 EXAMPLE 8. Vector s

8

P

a 2 a 4 Write, in component form, the vectors represented by the line segments joining the following points. (i) (2, 3) to (4, 1) (ii) (4, 0) to (6, 0) (iii) (0, 0) to (0, 4) (iv) (0, 4) to (0, 0) (v) (0, 0, 0) to (0, 0, 5) (vi) (0, 0, 0) to (1, 2, 3) (vii) (1,  2 , 3) to (0, 0, 0) (viii) (0, 2, 0) to (4, 0, 4) (ix) (1, 2, 3) to (3, 2, 1) (x) (4, 5, 0) to (4, 5, 1) 5 The points A, B and C have co-ordinates (2, 3), (0, 4) and (2, 1). (i) Write down the position vectors of A and C. (ii) Write down the vectors of the line segments joining AB and CB. (iii) What do your answers to parts (i) and (ii) tell you about (a) AB and OC (b) CB and OA? (iv) Describe the quadrilateral OABC.

Vector calculations

Multiplying a vector by a scalar When a vector is multiplied by a number (a scalar) its length is altered but its direction remains the same. The vector 2 a in figure 8.11 is twice as long as the vector a but in the same direction. Figure 8. When the vector is in component form, each component is multiplied by the number. For example: 2 (3 i  5 jk )  6 i  10 j  2 k

^3   6 

2 –5–10.   1     2  

262 The negative of a vector In figure 8.12 the vector  a has the same length as the vector a but the opposite direction. Vector s

aa

5 i + 2 j

2 i 3 i + 5 j 5 j

  • 3 j

2 i – 3 j

3 i

P

Figure 8.

When a is given in component form, the components of  a are the same as those

for a but with their signs reversed. So

^23  –23

Adding vectors

When vectors are given in component form, they can be added component

by component. This process can be seen geometrically by drawing them on

graph paper, as in the example below.

Add the vectors 2 i  3 j and 3 i + 5 j.

SOLUTION

2 i  3 j + 3 i + 5 j  5 i + 2 j

Figure 8.

The sum of two (or more) vectors is called the resultant and is usually

indicated by being marked with two arrowheads. 263

EXAMPLE 8.

calculations Vector

Q(3, 5)

1

4 )

P(2, 1)

T R

E

C

y

Q

When you find the vector y

represented by the line segment 6 joining two points, you are in

effect subtracting their position

5

vectors. If, for example,

P is the point (2, 1) and Q is the 4

 ^1 

point (3, 5), PQ is (^)   4

, as 3

figure 8.16 shows.

2

You find this by saying

  

PQ PO OQ  pq. (^1)

In this case, this gives

  2   3   1  0 1 2 3 4 5

x

PQ –

as expected.

This is an important result:



PQ  qp

Figure 8.

where p and q are the position vectors of P and Q.

Geometrical figures

It is often useful to be able to express lines in a geometrical figure in terms of

given vectors.

ACTIVITY 8.1 The diagram shows a cuboid OABCDEFG. P, Q, R, S and T are the mid-points of

the edges they lie on. The origin is at O and the axes lie along OA, OC and OD, as

shown in figure 8.17.



^6 

  0  

OA  0 , OC  5 , OD  0 

G S F

D

z B

O x P A

Figure 8.

calculations Vector

P

265

 C

 

CH = BG

  

FE = BC, EJ = BG, JI = AB

3 i + 5 j (^) This is the unit vector

3 i  5 j

3434

 

(iv) IJ DE

 AB

B

 p 8

 

(v) EF BC

 q

D

   

(vi) BE BC CD DE

q ( qp )  p

 2 q  2 p

E

  Figure 8.

Notice that BE 2CD.

   

(vii) AH AB BC CH

pqr

   

(viii) FI FE EJ JI

qrp

Unit vectors

A unit vector is a vector with a magnitude of 1, like i and j. To find the unit

vector in the same direction as a given vector, divide that vector by its magnitude.

Thus the vector 3 i  5 j (in figure 8.20) has magnitude

the vector

i

j is a unit vector. It has magnitude

 34 , and so

The unit vector in the direction of vector a is written as â and read as ‘a hat’.

y

5 j

4 j

3 j

2 j

j

O i

Figure 8.

2 i 3 i 4 i x

267

calculations Vector

P

AB

3

AC
BC
AB

 

 

AB + AC
BC.
AC

9 This is themagnitude^ of^ AB.

Relative to an origin O, the position vectors of the points A, B and C are given by







OA  3 , OB  1 and OC  3 .



(i) Find the unit vector in the direction AB.

(ii) Find the perimeter of triangle ABC.

SOLUTION

  

For convenience call OA  a , OB  b and OC  c.



(i) AB  ba  1  3  2 

 

To find the unit vector in the direction AB, you need to divide AB by its

magnitude.

  



^2 

2 

3

So the unit vector in the direction AB is

1  2  

2

 

3

  1

3

(ii)

1



 







^2  ^2 
^0 

AC  ca  3  3  0 

^ ^ 



^2  
^2 

BC  cb  3  1  2 

^

  (^) 

Perimeter of ABC ^ ^ +

 

+ BC

EXAMPLE 8.

Vector s

The perimeter of the triangle is given +

P

   

Verify that AB BC

a

M

1 Simplify the following.

P

(i) ^2  

^4  (ii)

(iii)

^3 

(iv) 3

(v) 6(3 i  2 j ) 9(2 ij )

2 The vectors p , q and r are given by

p  3 i  2 jk q  2 i  2 j  2 k r  3 ij  2 k.

Find, in component form, the following vectors.

(i) p + q + r (ii) pq (iii) p + r

(iv) 3( pq ) + 2( p + r ) (v) 4 p − 3 q + 2 r

 

3 In the diagram, PQRS is a parallelogram and PQ  a , PS  b.

(i) Write, in terms of a and b , Q R the following vectors.

 

(a) QR (b) PR



(c) QS

(ii) The mid-point of PR is M. Find

 

(a) PM (b) QM. P (^) b S

(iii) Explain why this shows you that the

diagonals of a parallelogram bisect each other.

4 In the diagram, ABCD is a kite. B AC and BD meet at M.



AB  ij and



AD  i  2 j j

(i) Use the facts that the diagonals

of a kite meet at right angles

i

and that M is the mid-point of

AC to find, in terms of i and j , D  

(a) AM (b) AC

 

(ii)

(c) BC (d) CD.

  (^) 

   

AD CD.

269

EXERCISE 8B

8B Exercise

and

A C

NM

8

P

5 In the diagram, ABC is a triangle. A L, M and N are the mid-points of the sides BC, CA and AB.   AB  p and AC  q  (i) Find, in terms of p and q , BC,   MN, LM and LN. B L C (ii) Explain how your results from part (i) show you that the sides of triangle LMN are parallel to those of triangle ABC, and half their lengths. 6 Find unit vectors in the same directions as the following vectors. (i)

(ii) 3 i  4 j (iii)

(iv) 5 i  12 j 7 Find unit vectors in the same direction as the following vectors.

^1 

(i)  2 

(ii) 2 i – 2 j + k (iii) 3 i – 4 k

^4 

(iv)  4  (v) 5 i – 3 j + 2 k (vi)  0 

8 Relative to an origin O, the position vectors of the points A, B and C are given by 

 ^2  

^1 

OA  1 , OB  4 and OC  2 .

Find the perimeter of triangle ABC. 9 Relative to an origin O, the position vectors of the points P and Q are given   by OP  3 ij  4 k and OQ  ix j  2 k. Find the values of x for which the magnitude of PQ is 7. 10 Relative to an origin O, the position vectors of the points A and B are given by 

^4 



^3 

OA  1  and OB  2 .

  (i) Given that C  i  s the point such that AC = 2 AB, find the unit vector in the direction of OC. 

^1 

The position vector of the point D is given by OD =  4 , where k is a  k     Vector s