Euclidean Spaces: Vectors, Operations, and Interpretations, Lecture notes of Calculus

An introduction to vectors in Euclidean spaces, including their definition, addition, scalar multiplication, and the inner product. It also covers geometric interpretations such as length, orthogonality, and projections. figures and theorems to illustrate the concepts.

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Vectors in Euclidean Spaces
Vectors.
Economists usually work in the vector space Rn. A point in this space is called
avector, and is typically defined by its rectangular coordinates.
For instance, let vRn. We define this vector by its ncoordinates, v1, v2, . . . , vn.
It is common to write v= (v1, v2, . . . , vn)or to display a vector as a column
matrix:
v=
v1
v2
.
.
.
vn
It is common to distinguish between locations and dispacements by writing a
location as a row vector and a displacement as a column vector. However, we
can use the same algebraic operations to work with each.
A vector can be also be defined by its origin and end points.
Suppose the vector vlinks the point P= (p1, . . . , pn)to the point Q= (q1, . . . , qn)
in Rn. Then v=QP, i.e. vi=piqi,i {1,2, . . . , n}.
-10 10
-5
5
v
P
Q
Figure 1: The displacement (5,3)
Addition.
Given two vectors uand v, with coordinates, we add them like so:
u+v=
u1
u2
.
.
.
un
+
v1
v2
.
.
.
vn
=
u1+v1
u2+v2
.
.
.
un+vn
.
pf3
pf4
pf5
pf8
pf9
pfa

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Vectors in Euclidean Spaces

Vectors.

  • Economists usually work in the vector space R n . A point in this space is called

a vector, and is typically defined by its rectangular coordinates.

  • For instance, let v ∈ R

n

. We define this vector by its n coordinates, v 1 , v 2 ,... , vn.

It is common to write v = (v 1 , v 2 ,... , vn) or to display a vector as a column

matrix:

v =

v 1

v 2

. . .

vn

  • It is common to distinguish between locations and dispacements by writing a

location as a row vector and a displacement as a column vector. However, we

can use the same algebraic operations to work with each.

  • A vector can be also be defined by its origin and end points.
  • Suppose the vector v links the point P = (p 1 ,... , pn) to the point Q = (q 1 ,... , qn)

in R n

. Then v = Q − P , i.e. vi = pi − qi, ∀i ∈ { 1 , 2 ,... , n}.

v

P

Q

Figure 1: The displacement (5, −3)

Addition.

  • Given two vectors u and v, with coordinates, we add them like so:

u + v =

u 1

u 2

. . .

un

v 1

v 2

. . .

vn

u 1 + v 1

u 2 + v 2

. . .

un + vn

v

v

u

u + v

v 1 u 1 u 1 +^ v 1

u 2

v 2

u 2 + v 2

Figure 2: Vector Addition

Scalar Multiplication.

  • We can also multiply vectors by scalars. Suppose λ ∈ R and v ∈ R

n

. Scalar

multiplication gives a vector λv ∈ R

n , defined by

λv =

λv 1

λv 2

. . .

λvn

     u

− 2 u

v

1 2

w v

3 w

Figure 3: Scalar multiplication

Subtraction.

  • The difference of two vectors, say u − v, is the sum of the vector u with the

vector −v = (−1)v.

u − v =

u 1

u 2

. . .

un

v 1

v 2

. . .

vn

u 1 − v 1

u 2 − v 2

. . .

un − vn

Laws of Vector Algebra.

  • Let λ, β ∈ R and u, v, w ∈ R

n

. Then the following algebraic properties of

vectors hold.

  • Commutativity:

u · v = v · u

  • Distributivity:

u · (v + w) = u · v + u · w

Length and Inner Product.

Definition. The norm or length of a vector u is the real number, denoted ‖u‖, given by

‖u‖ =

u

2 1 +^ u

2 2 +^ · · ·^ +^ u

2 n.^ N

  • Using our definition of the inner product we can also write this as

‖u‖ =

u.u

  • The norm of a vector is always positive unless the vector is the zero vector, in

which case the norm is zero.

  • The distance between two vectors u, v ∈ R n is calculated as

‖u − v‖ =

(u 1 − v 1 ) 2

  • · · · + (un − vn) 2 .
  • Note that for any λ ∈ R and u ∈ R

n :

‖λu‖ = |λ|‖u‖.

  • We can show that

u · v = ‖u‖‖v‖ cos θ

where θ is the angle between the vectors u and v.

  • Using the properties of the cosine we get the following result.

Theorem 1. The angle between vectors u and v in R n is

  1. acute, if u · v > 0 ,
  2. obtuse, if u · v < 0 ,
  3. right, if u · v = 0.

Definition. Let v be a vector. The vector w which points in the same direction as v,

but has length 1 is called the unit vector in the direction of v (or simply the direction

of v). It is given by

w =

v

‖v‖

. N

u

v

‖u‖ cos θ

θ

Figure 5: The angle between two vectors u and v.

Definition. Two vectors u, v ∈ R n are orthogonal if u · v = 0. N

  • This definition implies the zero vector is orthogonal to any vector.

Definition. Two vectors u, v ∈ R are orthonormal if they are orthogonal and are unit

vectors. N

Theorem 2 (Triangle Inequality). For any two vectors u, v ∈ R

n ,

‖u + v‖ ≤ ‖u‖ + ‖v‖.

Theorem 3 (Triangle Inequality Variant). For any two vectors u, v ∈ R

n ,

|‖u‖ − ‖v‖| ≤ ‖u − v‖.

  • There are three basic properties of Euclidean length for any vectors u and v and

scalar λ:

  1. ‖u‖ ≥ 0 and ‖u‖ = 0 only when u = 0,
  2. ‖λu‖ = |λ|‖u‖,
  3. ‖u + v‖ ≤ ‖u‖ + ‖v‖.

Any assignment of a real number to a vector satisfying these properties is called

a norm (see sections 29.4 and 27 of S&B if interested).

Projections.

  • Let u, v ∈ R

n

. We want to find the vector projection of the vector u in the

direction of v.

  • Denote the projection of u on v by Pv (u). We can see from the diagram that the

length of Pv (u) (called the scalar projection of vector u on v) is given by

‖Pv (u)‖ = ‖u‖ cos θ.

p + tv v

p

Figure 7: Parametric line ` in R 2

Two-dimensional Planes.

  • We saw that a line – a one-dimensional object – can be described using only one

parameter.

  • A plane is two-dimensional, so we need two parameters.
  • Consider a plane P in R

3 and let u and v be two vectors in P that point in

different directions:

x 1

x 2

x 3

u

v

Figure 8: A plane P through the origin in R 3

  • We can move from the origin in direction u, v or any combination of the two.

So, for any scalars s and t, the vector su + tv also lies in the plane P.

  • Thus any plane P through the origin, in a vector space R n (n > 2 ), can be

defined in its parametric form as

P = {x ∈ R

n | x = su + tv, s, t ∈ R}

  • But what if the plane does not pass through the origin?
  • Suppose the plane does not pass throught the origin.
  • We can move from point p in the plane in direction u, v or any combination of

the two. Thus the vector p + su + tv also lies in the plane P.

x 1

x 2

x 3

p

u v

Figure 9: A plane P not through the origin in R 3

  • So any plane P through the point p, in a vector space R n (n > 2 ), can be defined

in its parametric form as

P = {x ∈ R

n | x = p + su + tv, s, t ∈ R}

  • A point x ∈ R n belongs to the plane P iff there exist two scalars s and t such

that x = p + su + tv. Equivalently, the vector x − p must be a linear combination

of the vectors u and v.

  • As two points uniquely determine a line, three distinct (non-collinear) points P ,

Q and R uniquely determine a plane.

  • Let u = Q − P and v = R − P. We can picture these as displacement

vectors from P :

x 1

x 2

x 3

P

u

Q

v

R

Figure 10: A plane P not through the origin in R 3

  • Remember, we need u and v to be nonparallel to for them to uniquely determine

a plane.

Hyperplanes.

  • We saw a line in R

2 can be written as

a 1 x 1 + a 2 x 2 = d

and a plane in R

3 can be written in point-normal form as

a 1 x 1 + a 2 x 2 + a 3 x 3 = d.

  • Generalizing, a hyperplane in R n can be written in point-normal form as

a 1 x 1 + a 2 x 2 + · · · + anxn = d,

where (a 1 , a 2 ,... , an) is a normal.

  • The set of vectors in the hyperplane have tail at (0,... , 0 , d/an) and are

perpindicular to the normal vector to the hyperplane.

Example 1.

  1. An economic application you have probably seen deals with commodity spaces.
    • The vector

x = (x 1 , x 2 ,... , xn)

of nonnegative quantities of n commodities is called a commodity bundle.

The set of all commodity bundles is the set

{(x 1 ,... , xn) | x 1 ≥ 0 ,... , xn ≥ 0 }

and is called a commodity space.

  • Let pi > 0 be the price of commodity i. The cost of buying bundle x is

p 1 x 1 + p 2 x 2 + · · · + pnxn = p · x.

A consumer with income I can purchase only bundles x for which p·x ≤ I.

This subset of the commodity space is the consumer’s budget set.

  1. • The budget set is bounded above by the hyperplane p·x = I, whose normal

vector is the price vector p.

x 1

x 2

p = (p 1 , p 2 )

p 1 x 1 + p 2 x 2 = I

Figure 12: A consumer’s budget set, p · x ≤ I, in commodity space.