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P1 Chapter 11 :: Vectors [email protected] www.drfrostmaths.com @DrFrostMaths Last modified: 21 st August 2017

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Page 1: P1 Chapter 11 :: Vectors

P1 Chapter 11 :: Vectors

[email protected]

@DrFrostMaths

Last modified: 21st August 2017

Page 2: P1 Chapter 11 :: Vectors

Use of DrFrostMaths for practice

Register for free at:www.drfrostmaths.com/homework

Practise questions by chapter, including past paper Edexcel questions and extension questions (e.g. MAT).

Teachers: you can create student accounts (or students can register themselves).

Page 3: P1 Chapter 11 :: Vectors

Chapter Overview

1:: Add/scale factors and show vectors are parallel.

4:: Solve both geometric problems.

An orienteer leaves position 𝑂 and walks 15km at a bearing of 120Β° to

the position A. Determine 𝑂𝐴.

2:: Calculate magnitude and direction of a vector.

Vectors used to be a Year 2 A Level topic. However, the more difficult content has been moved to Further Maths. This chapter is now more intended as providing the β€˜fundamentals’ of vectors (most of which you learned at GCSE), supporting Mechanics and FM.

If 𝒂 = 3π’Š + 4𝒋, determine |𝒂|.

3:: Understand and use position vectors.

A donut has position vector 4π’Š + 3𝒋…

5:: Understand speed vs velocity

If a ship moves at a velocity of 12𝑖 + 5𝑗 π‘˜π‘š/β„Ž, what is its speed?

Page 4: P1 Chapter 11 :: Vectors

Vector Basics

Whereas a coordinate represents a position in space, a vectorrepresents a displacement in space.

A

A vector has 2 properties:β€’ Directionβ€’ Magnitude (i.e. length)

B

If 𝑃 and 𝑄 are points then 𝑃𝑄 is the vector between them.

𝑃

𝑄

If two vectors 𝑃𝑄 and 𝑅𝑆 have the same magnitude and direction, they’re the same vector and are parallel.

𝑃

𝑄

𝑅

𝑆

This might seem obvious, but students sometimes think the vector is different because the movement occurred at a different point in space. Nope!

D Triangle Law for vector addition:

𝐴𝐡 + 𝐡𝐢 = 𝐴𝐢

The vector of multiple vectors is known as the resultant vector. (you will encounter this term in Mechanics)

𝒂𝒃

𝒂 + 𝒃𝐴

𝐡

𝐢

C 𝐴𝐡 = βˆ’π΅π΄ and the two vectors are parallel, equal in magnitude but in opposite directions.

𝐴

𝐡

𝐴

𝐡𝒂

βˆ’π’‚

Page 5: P1 Chapter 11 :: Vectors

β€˜Multiplying’ two sets (known again as the cross product) finds each possible combination of members, one from each:

π‘Ž, 𝑏, 𝑐 Γ— 𝑑, 𝑒 = { π‘Ž, 𝑑 , π‘Ž, 𝑒 , {𝑏, 𝑑},𝑏, 𝑒 , 𝑐, 𝑑 , 𝑐, 𝑒 }

It has the nice property that 𝑛 𝐴 Γ— 𝐡 = 𝑛 𝐴 Γ— 𝑛(𝐡), where 𝑛 𝐴 gives the size of the set 𝐴. Also, 𝐴 Γ— 𝐡 = 𝐡 Γ— 𝐴.

Just for your interest…

Have you ever wondered what happens if you β€˜multiply’ two vectors or two sets?

ME-WOW!

Erm…

In KS2/3 you probably only experienced variables holding numerical values. You since saw that variables can represent other mathematical types, such as sets or vectors:

π‘₯ = 3

𝒂 =1βˆ’2

𝑇 = {2,5,9,10}

But when we do we need to define explicitly what operators like β€˜+’ and β€˜Γ—β€™ mean.

1 + 3 = 43βˆ’2

+10

=4βˆ’2

32βˆ’1

Γ—101

=? π‘Ž, 𝑏, 𝑐 Γ— 𝑑, 𝑒 =?

Often these operators are defined to give it properties that are consistent with its usage elsewhere, e.g. β€˜commutativity’: 𝒂 + 𝒃 = 𝒃 + 𝒂 for vector addition just as 2 + 4 = 4 + 2 for numbers.

In FM, you will see that β€˜multiplying’ two 3D vectors (known as the cross product) gives you a vector perpendicular to the two.Vector multiplication is not commutative, so 𝒂 Γ— 𝒃 β‰  𝒃 Γ— 𝒂 (however it is β€˜distributive’, so 𝒂 Γ— 𝒃 + 𝒄 = 𝒂 Γ— 𝒃 + 𝒂 Γ— 𝒄 )The Casio Classwiz can calculate this in Vector mode!

32βˆ’1

Γ—101

=2βˆ’42

𝒃

𝒂

𝒂 Γ— 𝒃

Page 6: P1 Chapter 11 :: Vectors

Vector Basics

E Vector subtraction is defined using vector addition and negation:

𝒂 βˆ’ 𝒃 = 𝒂 + βˆ’π’ƒ

𝒂 𝒃𝒂

βˆ’π’ƒ

𝒂 βˆ’ 𝒃

The zero vector 𝟎 (a bold 0), represents no movement.

𝑃𝑄 + 𝑄𝑃 = 𝟎

In 2D: 𝟎 =00

F

G A scalar is a normal number, which can be used to β€˜scale’ a vector.β€’ The direction will be the same.β€’ But the magnitude will be different

(unless the scalar is 1).

𝒂

2𝒂

Any vector parallel to the vector 𝒂 can be written as πœ†π’‚, where πœ† is a scalar.

H

The implication is that if we can write one vector as a multiple of another, then we can show they are parallel.

β€œShow 2𝒂 + 4𝒃 and 3𝒂 + 6𝒃 are parallel”.

3𝒂 + 6𝒃 =3

2𝒂 + 2𝒃 ∴ parallel

βˆ’1

2𝒂

If scalar is negative, opposite direction.

Page 7: P1 Chapter 11 :: Vectors

Example

Edexcel GCSE June 2013 1H Q27

𝑆𝑄 = βˆ’π’ƒ + 𝒂

For (b), there’s two possible paths to get from 𝑁 to 𝑅: via 𝑆 or via 𝑄. But which is best?In (a) we found 𝑺 to 𝑸 rather than 𝑸 to 𝑺, so it makes sense to go in this direction so that we can use our result in (a).

a

b 𝑁𝑅 =2

5𝑆𝑄 + 𝒃

=2

5βˆ’π’ƒ + 𝒂 + 𝒃

=2

5𝒂 +

3

5𝒃

Fro Tip: This ratio wasn’t in the original diagram. I like to add the ratio as a visual aid.

Fro Workings Tip: While you’re welcome to start your working with the second line, I recommend the first line so that your chosen route is clearer.

𝑄𝑅 is also 𝑏because it is exactly the same

movement as 𝑃𝑆.

Page 8: P1 Chapter 11 :: Vectors

Test Your Understanding

𝐴𝐡 = 𝐴𝑂 + 𝑂𝐡= βˆ’π’‚ + 𝒃

𝑂𝑃 = 𝒂 +3

4𝐴𝐡

= 𝒂 +3

4βˆ’π’‚ + 𝒃

=1

4𝒂 +

3

4𝒃

Edexcel GCSE June 2012

Page 9: P1 Chapter 11 :: Vectors

Exercise 11A

Pearson Pure Mathematics Year 1/ASPages 234-235

Page 10: P1 Chapter 11 :: Vectors

Representing Vectors

You should already be familiar that the value of a vector is the displacement in the π‘₯ and 𝑦 direction (if in 2D).

3βˆ’2 𝒂 =

3βˆ’2

, 𝒃 =0βˆ’1

𝒂 + 𝒃 =3βˆ’3

2𝒂 =6βˆ’4

! A unit vector is a vector of magnitude 1. π’Š and 𝒋 are unit vectors in the π‘₯-axis and 𝑦-axis respectively.

π’Š =10

𝒋 =01

e.g. 43

= 410

+ 301

= 4π’Š + 3𝒋

π’Š

𝒋

Fro Side Notes: This allows us to write any vector algebraically without using vector notation. Any point in 2D space, as a vector from the

origin, can be obtained using a linear combination of π’Š and 𝒋, e.g. if 𝑃 5,βˆ’1 , 𝑂𝑃 = 5π’Š βˆ’ 𝒋. For this reason, π’Š and 𝒋 are known as basis

vectors of 2D coordinate space. In fact, any two non-parallel/non-zero vectors can be used as basis vectors, e.g. if 𝒂 =52

and 𝒃 =30

, it’s

possible to get any vector π‘₯𝑦 using a linear combination of these, i.e. we can always find scalars 𝑝 and π‘ž such that

π‘₯𝑦 = 𝑝

52

+ π‘ž30

.

Page 11: P1 Chapter 11 :: Vectors

Examples

If 𝒂 = 3π’Š, 𝒃 = π’Š + 𝒋, 𝒄 = π’Š βˆ’ 2𝒋 then:1) Write 𝒂 in vector form.2) Find 𝒃 + 2𝒄 in π’Š, 𝒋 form.

𝒂 =30

𝒃 + 2𝒄 = π’Š + 𝒋 + 2 π’Š βˆ’ 2𝒋= π’Š + 𝒋 + 2π’Š βˆ’ 4𝒋= 3π’Š βˆ’ 3𝒋

1

2

Page 12: P1 Chapter 11 :: Vectors

Exercise 11B

Pearson Pure Mathematics Year 1/ASPages 237-238

Page 13: P1 Chapter 11 :: Vectors

Magnitude of a Vector

! The magnitude |π‘Ž| of a vector π‘Ž is its length.

34

𝐴

𝐡

𝐴𝐡 = 32 + 42 = 5

3

4

1βˆ’1

= 2 βˆ’5βˆ’12

= 13

𝒂 =4βˆ’1

𝒂 = 42 + 12 = 17

𝒃 =20

𝒃 = 22 + 02 = 2

! If 𝒂 =π‘₯𝑦 𝒂 = π‘₯2 + 𝑦2

Page 14: P1 Chapter 11 :: Vectors

Unit Vectors

! A unit vector is a vector whose magnitude is 1

There’s certain operations on vectors that require the vectors to be β€˜unit’ vectors. We just scale the vector so that its magnitude is now 1.

𝒂 =34

𝒂 = 32 + 42 = 5

ෝ𝒂 =3/54/5

Test Your Understanding: Convert the following vectors to unit vectors.

𝒂 =12βˆ’5

𝒂 = 𝟏𝟐𝟐 + πŸ“πŸ = πŸπŸ‘

∴ ෝ𝒂 =

𝟏𝟐

πŸπŸ‘

βˆ’πŸ“

πŸπŸ‘

If 𝒂 is a vector, then the unit vector ෝ𝒂 in the same direction is

ෝ𝒂 =𝒂

𝒂

𝒃 =11

𝒃 = 𝟏𝟐 + 𝟏𝟐 = 𝟐

∴ 𝒃 =

𝟏

𝟐𝟏

𝟐

Page 15: P1 Chapter 11 :: Vectors

Exercise 11C

Pearson Pure Mathematics Year 1/ASPages 240-242

Page 16: P1 Chapter 11 :: Vectors

Position Vectors

Suppose we started at a point 3,2

and translated by the vector 40

:

𝐴 3,2

40

You might think we can do something like:

3,2 +40

= 7,2

But only vectors can be added to other vectors.If we treated the point πŸ‘, 𝟐 as a vector, then this solves the problem:

32

+40

=72

?

𝐴 3,2𝒂 =

32

𝑂

! The position vector of a

point 𝐴 is the vector 𝑂𝐴,

where 𝑂 is the origin. 𝑂𝐴is usually written as 𝒂.

π‘₯

𝑦

A vector used to represent a position is unsurprisingly known as a position vector.A position can be thought of as a translation from the origin, as per above. It enables us to use positions in all sorts of vector (and matrix!) calculations.

Page 17: P1 Chapter 11 :: Vectors

Example

The points 𝐴 and 𝐡 have coordinates 3,4 and (11,2) respectively.Find, in terms of 𝑖 and 𝑗:a) The position vector of 𝐴b) The position vector of 𝐡

c) The vector 𝐴𝐡

𝑂𝐴 = 3π’Š + 4𝒋

𝑂𝐡 = 11π’Š + 2𝒋

𝐴𝐡 = 8π’Š βˆ’ 2𝒋

a

b

c

You can see this by inspection of the change in π‘₯ and the change in 𝑦:

𝐴 3,4 β†’ 𝐡(11,2)

More formally:

𝐴𝐡 = 𝑂𝐡 βˆ’ 𝑂𝐴

=112

βˆ’34

=8βˆ’2

+8 βˆ’2

Page 18: P1 Chapter 11 :: Vectors

Further Example

𝑂𝐴 = 5𝑖 βˆ’ 2𝑗 and 𝐴𝐡 = 3𝑖 + 4𝑗. Find:a) The position vector of 𝐡.

b) The exact value of 𝑂𝐡 in simplified surd form.

𝑂𝐡 = 𝑂𝐴 + 𝐴𝐡 =5βˆ’2

+34

=82

𝑂𝐡 = 82 + 22 = 2 17

a

b

Either a quick sketch will help you see this, or

thinking of 𝑂𝐴 as the

original position and 𝐴𝐡as the translation.

Page 19: P1 Chapter 11 :: Vectors

Exercise 11D

Pearson Pure Mathematics Year 1/ASPages 243-244

Page 20: P1 Chapter 11 :: Vectors

Solving Geometric Problems

𝒂𝑴

𝑢 𝑩

𝑿

𝒃

𝑨 π‘ͺ

𝑋 is a point on 𝐴𝐡 such that 𝐴𝑋: 𝑋𝐡 = 3: 1. 𝑀 is the midpoint of 𝐡𝐢.

Show that 𝑋𝑀 is parallel to 𝑂𝐢.

𝑂𝐢 = π‘Ž + 𝑏

𝑋𝑀 =1

4βˆ’π‘Ž + 𝑏 +

1

2π‘Ž =

1

4π‘Ž +

1

4𝑏

=1

4π‘Ž + 𝑏

𝑋𝑀 is a multiple of 𝑂𝐢 ∴ parallel.

The key is to factor out a scalar such that we see the same vector.

For any proof question always find the vectors

involved first, in this case 𝑋𝑀 and 𝑂𝐢.

The magic words here are β€œis a multiple of”.

Page 21: P1 Chapter 11 :: Vectors

Introducing Scalars and Comparing Coefficients

𝒂

𝒃

𝑂

𝐡

𝐴

𝐢

𝑋

Remember when we had identitieslike: π‘Žπ‘₯2 + 3π‘₯ ≑ 2π‘₯2 + 𝑏π‘₯we could compare coefficients, so that π‘Ž = 2 and 3 = 𝑏.We can do the same with (non-parallel) vectors!

𝑂𝐴𝐢𝐡 is a parallelogram, where 𝑂𝐴 = π‘Ž and 𝑂𝐡 = 𝑏. The diagonals 𝑂𝐢 and 𝐴𝐡 intersect at a point 𝑋. Prove that the diagonals bisect each other.

(Hint: Perhaps find 𝑂𝑋 in two different ways?)

By considering the route 𝑂 β†’ 𝐡 β†’ 𝑋:

𝑂𝑋 = 𝒃 + πœ† 𝐡𝐴= 𝒃 + πœ† βˆ’π’ƒ + 𝒂 = 𝒃 βˆ’ πœ†π’ƒ + πœ†π’‚= πœ†π’‚ + 1 βˆ’ πœ† 𝒃

Similarly, considering the line 𝑂𝐢:

𝑂𝑋 = πœ‡ 𝑂𝐢 = πœ‡ 𝒂 + 𝒃 = πœ‡π’‚ + πœ‡π’ƒβˆ΄ πœ‡π’‚ + πœ‡π’ƒ = πœ†π’‚ + 1 βˆ’ πœ† 𝒃

Comparing coefficients of 𝒂: πœ‡ = πœ†Comparing coefficients of 𝒃: πœ‡ = 1 βˆ’ πœ†

∴ πœ‡ = πœ† =1

2∴ 𝑋 is the midpoint of each of the diagonals.

We don’t know what fraction of the way across 𝐡𝐴the point 𝑋 is, so let πœ† be the fraction of the way

across. We’re hoping that πœ† =1

2, so that 𝑋 is exactly

halfway across and therefore bisects 𝐡𝐴.

We need to use a different scalar constant, this time πœ‡.It is common to use the letters πœ† and πœ‡ for scalars.

Page 22: P1 Chapter 11 :: Vectors

Test Your Understanding

𝒂

𝒃

𝑂

𝐡

𝐴

𝐢

𝑋

𝑄

In the above diagram, 𝑂𝐴 = 𝒂,𝑂𝐡 = 𝒃 and 𝑂𝑄 =1

3𝒂. We wish to find the ratio 𝑂𝑋: 𝑋𝐢.

a) If 𝑂𝑋 = πœ† 𝑂𝐢, find an expression for 𝑂𝑋 in terms of 𝒂, 𝒃 and πœ†.

b) If 𝐡𝑋 = πœ‡ 𝐡𝑄, find an expression for 𝑂𝑋 in terms of 𝒂, 𝒃 and πœ‡.c) By comparing coefficients or otherwise, determine the value of πœ†, and hence the ratio 𝑂𝑋: 𝑋𝐢.

𝑂𝑋 = πœ† 𝑂𝐢 = πœ† 𝒂 + 𝒃 = πœ†π’‚ + πœ†π’ƒ

𝑂𝑋 = 𝒃 + πœ‡ 𝐡𝑄 = 𝒃 + πœ‡ βˆ’π’ƒ +1

3𝒂 =

1

3πœ‡π’‚ + 1 βˆ’ πœ‡ 𝒃

Comparing coefficients: πœ† =1

3πœ‡ and πœ† = 1 βˆ’ πœ‡, ∴ πœ† =

1

4

If 𝑂𝑋 =1

4𝑂𝐢, then 𝑂𝑋: 𝑋𝐢 = 1: 3.

a

b

c

Expand and collect 𝒂 terms and collect 𝒃 terms, so that we can compare coefficients later.

Page 23: P1 Chapter 11 :: Vectors

Area of a Triangle

𝐴𝐡 = 3π’Š βˆ’ 2𝒋 and 𝐴𝐢 = π’Š βˆ’ 5𝒋. Determine ∠𝐡𝐴𝐢.

Strategy: Find 3 lengths of triangle then use cosine rule to find angle.

𝐴

𝐢

𝐡

3βˆ’2

1βˆ’5

23

𝐴𝐡 = 13

𝐴𝐢 = 26𝐢𝐡 = 13

A clever student might at this point realise that we can divide all the lengths by 13 without changing ∠𝐡𝐴𝐢,

giving a 1: 1: 2 triangle (one of our β€˜special’ triangles!), and thus instantly getting ∠𝐡𝐴𝐢 = 45Β°.But let’s use a more general method of using the cosine rule:

π‘Ž = 13, 𝑏 = 13, 𝑐 = 26

13 = 13 + 26 βˆ’ 2 Γ— 13 Γ— 26 Γ— cos 𝐴

cos 𝐴 =1

2β†’ 𝐴 = 45Β°

Page 24: P1 Chapter 11 :: Vectors

Exercise 11E

Pearson Pure Mathematics Year 1/ASPages 246-247

[STEP 2010 Q7]Relative to a fixed origin 𝑂, the points 𝐴 and 𝐡 have position vectors 𝒂 and 𝒃, respectively. (The points 𝑂, 𝐴 and 𝐡 are not collinear.) The point 𝐢 has position vector 𝒄 given by

𝒄 = 𝛼𝒂 + 𝛽𝒃,where 𝛼 and 𝛽 are positive constants with 𝛼 + 𝛽 < 1. The lines 𝑂𝐴and 𝐡𝐢 meet at the point 𝑃 with position vector 𝒑 and the lines 𝑂𝐡and 𝐴𝐢 meet at the point 𝑄 with position vector 𝒒. Show that

𝒑 =π›Όπ‘Ž

1 βˆ’ 𝛽and write down π‘ž in terms of 𝛼, 𝛽 and 𝑏.Show further that the point 𝑅 with position vector π‘Ÿ given by

𝒓 =𝛼𝒂 + 𝛽𝒃

𝛼 + 𝛽,

lies on the lines 𝑂𝐢 and 𝐴𝐡.

The lines 𝑂𝐡 and 𝑃𝑅 intersect at the point 𝑆. Prove that 𝑂𝑄

𝐡𝑄=

𝑂𝑆

𝐡𝑆.

Extension

1

Click here for the solution:http://www.mathshelper.co.uk/STEP%202010%20Solutions.pdf(go to Q7)

Page 25: P1 Chapter 11 :: Vectors

Modelling

Velocitye.g.

34

π‘˜π‘š/β„Ž

In Mechanics, you will see certain things can be represented as a simple number (without direction), or as a vector (with direction):

4

3

Vector Quantity Equivalent Scalar Quantity

Speed= 5 π‘˜π‘š/β„Ž

5

Remember a β€˜scalar’ just means a normal number (in the context of vectors). It can be obtained using the magnitude of the vector.

This means the position vector of the object changes

by 34

each hour.

…which is equivalent to moving 5km each hour.

Displacemente.g.

βˆ’512

π‘˜π‘š

Distance= 13 π‘˜π‘š

Page 26: P1 Chapter 11 :: Vectors

Example

[Textbook] A girl walks 2 km due east from a fixed point 𝑂 to 𝐴, and then 3 km due south from 𝐴 to 𝐡. Finda) the total distance travelledb) the position vector of 𝐡 relative to 𝑂

c) 𝑂𝐡

d) The bearing of 𝐡 from 𝑂.

2

3

N

𝑂𝐴

𝐡

πœƒ

2 + 3 = 5π‘˜π‘š

𝑂𝐡 =23

π‘˜π‘š

𝑂𝐡 = 22 + 32 = 13 = 3.61π‘˜π‘š (3sf)

90Β° + tanβˆ’13

2= 56.3Β°

a

b

c

d

Page 27: P1 Chapter 11 :: Vectors

Further Example

[Textbook] In an orienteering exercise, a cadet leaves the starting point 𝑂 and walks 15 km on a bearing of 120Β° to reach 𝐴, the first checkpoint. From 𝐴 he walks 9 km on a bearing of 240Β° to the second checkpoint, at 𝐡. From 𝐡 he returns directly to 𝑂.Find:a) the position vector of 𝐴 relative to 𝑂

b) 𝑂𝐡

c) the bearing of 𝐡 from 𝑂d) the position vector of 𝐡 relative 𝑂.

9 π‘˜π‘š

15 π‘˜π‘š

N

𝑂

𝐴

𝐡

πœƒ

N

240Β°

a 120Β°

30Β°

𝑂𝐴 =15 cos 30Β°15 sin 30Β°

=13.07.5

π‘˜π‘š

b

9 π‘˜π‘š

15 π‘˜π‘š

N

π΄πœƒ

N

240Β°

30Β°60Β°

60Β°

𝐡

𝑂

Using cosine rule on Δ𝑂𝐴𝐡,

𝑂𝐡 = 13.1π‘˜π‘š (3sf)

c Using sine rule on Δ𝑂𝐴𝐡:πœƒ = 36.6… Β°

∴ Bearing = 120 + 36.6° = 157° (3sf)

I have no specific advice to offer except:1. Draw a BIG diagram.2. Remember bearings are measured

clockwise from North.3. Don’t forget units (on vectors!)

Page 28: P1 Chapter 11 :: Vectors

Further Example

[Textbook] In an orienteering exercise, a cadet leaves the starting point 𝑂 and walks 15 km on a bearing of 120Β° to reach 𝐴, the first checkpoint. From 𝐴 he walks 9 km on a bearing of 240Β° to the second checkpoint, at 𝐡. From 𝐡 he returns directly to 𝑂.Find:a) the position vector of 𝐴 relative to 𝑂

b) 𝑂𝐡

c) the bearing of 𝐡 from 𝑂d) the position vector of 𝐡 relative 𝑂.

d

9 π‘˜π‘š

N

𝑂

𝐴

𝐡

πŸ‘πŸ”. πŸ“πŸ—Β°

N

120Β°

30Β°

23.41Β°

𝑂𝐡 =13.07 sin 23.41Β°βˆ’13.07 cos 23.41Β°

=5.19βˆ’12.0

π‘˜π‘š

(I think the textbook made a rounding error due to use of

rounded values. They put 5.1

βˆ’12.1)

Page 29: P1 Chapter 11 :: Vectors

Exercise 11F

Pearson Pure Mathematics Year 1/ASPages 250-251