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A FIRST COURSEIN LINEAR ALGEBRAAn Open Text by Ken Kuttler
Rn: Vectors
Lecture Notes by Karen Seyffarth∗
Adapted byLYRYX SERVICE COURSE SOLUTION
∗Attribution-NonCommercial-ShareAlike (CC BY-NC-SA)This license lets others remix, tweak, and build upon your work
non-commercially, as long as they credit you and license their new creationsunder the identical terms.
Rn : Vectors Page 1/31
What is Rn?
Notation and Terminology
R denotes the set of real numbers.
R2 denotes the set of all column vectors with two entries.
R3 denotes the set of all column vectors with three entries.
In general, Rn denotes the set of all column vectors with n entries.
Rn : Vectors What is Rn? Page 2/31
Scalar quantities versus vector quantities
A scalar quantity has only magnitude; e.g. time, temperature.
A vector quantity has both magnitude and direction; e.g. displacement,force, wind velocity.
Whereas two scalar quantities are equal if they are represented by the same value,two vector quantities are equal if and only if they have the same magnitude anddirection.
Rn : Vectors What is Rn? Page 3/31
R2 and R3
Vectors in R2 and R3 have convenient geometric representations as positionvectors of points in the 2-dimensional (Cartesian) plane and in 3-dimensionalspace, respectively.
Rn : Vectors What is Rn? Page 4/31
R2
0 xa
y
b (a, b)
The vector
[ab
].
R3
0
x
y
z
(a, b, c)
a
b
c
The vector
abc
.
Rn : Vectors What is Rn? Page 5/31
Notation
If P is a point in Rn with coordinates (p1, p2, ..., pn) we denote this byP = (p1, p2, ..., pn).
If P = (p1, p2, . . . , pn) is a point in Rn, then
−→0P =
p1p2...pn
is often used to denote the position vector of the point.
Instead of using a capital letter to denote the vector (as we generally dowith matrices), we emphasize the importance of the geometry and thedirection with an arrow over the name of the vector.
Rn : Vectors What is Rn? Page 6/31
Notation and Terminology
The notation−→0P emphasizes that this vector goes from the origin 0 to the
point P. We can also use lower case letters for names of vectors. In this
case, we write−→0P = ~p.
Any vector
~x =
x1x2...xn
in Rn
is associated with the point (x1, x2, . . . , xn).
Often, there is no distinction made between the vector ~x and the point(x1, x2, . . . , xn), and we say that both (x1, x2, . . . , xn) ∈ Rn and
~x =
x1x2...xn
∈ Rn.
Rn : Vectors What is Rn? Page 7/31
Geometric Vectors in R2 and R3
Let A and B be two points in R2 or R3.
0 x
y
B
A
•−→AB is the geometric vector from A to B.
• A is the tail of−→AB.
• B is the tip of−→AB.
• the magnitude of−→AB is its length, and is
denoted ||−→AB||.
Rn : Vectors Geometric Vectors Page 8/31
Equality of geometric vectors
0 x
y
A
B
C
D
•−→AB is the vector from A = (1, 0).
to B = (2, 2).
•−→CD is the vector from C = (−1,−1)
to D = (0, 1).
•−→AB =
−→CD because the vectors have
the same length and direction.
The fact that the points A and B are different from the points C and D is notimportant. For geometric vectors, the location of the vector in the plane (or in3-dimensional space) is not important; the important properties are its length anddirection.
Rn : Vectors Geometric Vectors Page 9/31
Coordinatizing Vectors – Part 1
0 x
y
A
BP
−→0P is the position vector for P = (1, 2),
and−→0P =
[12
].
Since−→AB =
−→0P, it should be the case that
−→AB =
[12
]. This can be seen by
moving−→AB so that its tail is at the origin.
A geometric vector is coordinatized by putting it in standard position, meaningwith its tail at the origin, and then identifying the vector with its tip.
Rn : Vectors Geometric Vectors Page 10/31
Algebra in Rn
Addition in Rn
Since vectors in Rn are n × 1 matrices, addition in Rn is precisely matrix additionusing column matrices, i.e.,
If ~u and ~v are in Rn, then ~u + ~v is obtained by adding togethercorresponding entries of the vectors.
The zero vector in Rn is the n × 1 zero matrix, and is denoted ~0.
Example
Let ~u =
123
and ~v =
456
. Then,
~u + ~v =
123
+
456
=
579
Rn : Vectors Algebra in Rn Page 11/31
Properties of Vector Addition
Let ~u, ~v , and ~w be vectors in Rn. Then the following properties hold.
1 ~u + ~v = ~v + ~u (vector addition is commutative).
2 (~u + ~v) + ~w = ~u + (~v + ~w) (vector addition is associative).
3 ~u +~0 = ~u (existence of an additive identity).
4 ~u + (−~u) = ~0 (existence of an additive inverse).
Rn : Vectors Algebra in Rn Page 12/31
Scalar Multiplication
Since vectors in Rn are n × 1 matrices, scalar multiplication in Rn is preciselymatrix scalar multiplication using column matrices, i.e., If ~u is a vector in Rn andk ∈ R is a scalar, then k~u is obtained by multiplying every entry of ~u by k.
Example
Let ~u =
123
and k = 4. Then,
k~u = 4
123
=
48
12
Rn : Vectors Algebra in Rn Page 13/31
Properties of Scalar Multiplication
Let ~u, ~v ∈ Rn be vectors and k , p ∈ R be scalars. Then the following propertieshold.
1 k(~u + ~v) = k~u + k~v (scalar multiplication distributes over vector addition).
2 (k + p)~u = k~u + p~u (addition distributes over scalar multiplication).
3 k(p~u) = (kp)~u (scalar multiplication is associative).
4 1~u = ~u (existence of a multiplicative identity).
Rn : Vectors Algebra in Rn Page 14/31
The Geometry of Vector Addition
1 Vector Equality. The vectors have the same length and direction.
2 The zero vector, ~0 has length zero and no direction.
3 Addition. Let ~u, ~v be vectors. Then ~u + ~v is the diagonal of theparallelogram defined by ~u and ~v , and having the same tail as ~u and ~v .
~u
~u + ~v
~v
Rn : Vectors The Geometry of Vector Addition Page 15/31
Tip-to-Tail Method for Vector Addition
For points A, B and C , −→AB +
−→BC =
−→AC .
A
B
C
−→AB
−→BC
−→AC
−→AB
−→BC
Rn : Vectors The Geometry of Vector Addition Page 16/31
Example
The diagonals of any parallelogram bisect each other.
To see this, denote the parallelogram by its vertices, ABCD.
A
B C
D
M
• Let M denote the midpoint
of−→AC .
Then−−→AM =
−−→MC .
• It now suffices to show
that−−→BM =
−−→MD.
−−→BM =
−→BA +
−−→AM =
−→CD +
−−→MC =
−−→MC +
−→CD =
−−→MD.
Since−−→BM =
−−→MD, these vectors have the same magnitude and direction, implying
that M is the midpoint of−→BD.
Therefore, the diagonals of ABCD bisect each other.
Rn : Vectors The Geometry of Vector Addition Page 17/31
The Geometry of Vector Subtraction
Let ~u and ~v be vectors in R2 or R3. The vector ~u−~v = ~u + (−~v) is obtained fromthe parallelogram defined by ~u and ~v by taking the vector from the tip of ~v to thetip of ~u, i.e., the diagonal of the parallelogram, directed towards the tip of ~u.
~v
~u
~u
−~v~u − ~v
Rn : Vectors The Geometry of Vector Addition Page 18/31
Coordinatizing Vectors – Part 2
Let A = (x1, y1, z1) and B = (x2, y2, z2) be two points in R3.
0
x
y
z
A
B
We see from the figure that−→0A +
−→AB =
−→0B, and hence
−→AB =
−→0B −
−→0A =
x2y2z2
− x1
y1z1
=
x2 − x1y2 − y1z2 − z1
.
Rn : Vectors The Geometry of Vector Addition Page 19/31
Length of a Vector
The Distance Between Points
For A = (x1, y1, z1) and B = (x2, y2, z2) in R3, the distance between them iswritten d(A,B) and is given by
d(A,B) =√
(x2 − x1)2 + (y2 − y1)2 + (z2 − z1)2.
This is called the distance formulaIf P = (x2 − x1, y2 − y1, z2 − z1), then the distance between the origin and P isequal to the the distance between points A and B i.e.,
d(0,P) = d(A,B) =√
(x2 − x1)2 + (y2 − y1)2 + (z2 − z1)2.
Rn : Vectors Length of a Vector Page 20/31
Properties of Distance
Let P and Q be two points in Rn, and d(P,Q) the distance between them. Thenthe following properties hold.
1 The distance between P and Q is equal to the distance between Q and P,i.e., d(P,Q) = d(Q,P).
2 d(P,Q) ≥ 0 with equality if and only if P = Q.
Example
For P = (1,−1, 3) and Q = (3, 1, 0), the distance between P and Q isd(P,Q) =
√22 + 22 + (−3)2 =
√17.
Rn : Vectors Length of a Vector Page 21/31
Length of a Vector
More generally, if P = (p1, p2, . . . , pn) and Q = (q1, q2, . . . , qn) are points in Rn,
then the distance between P and Q is the length of the vector−→PQ, written ‖
−→PQ‖.
d(P,Q) = ‖−→PQ‖ =
√(q1 − p1)2 + (q2 − p2)2 + · · ·+ (qn − pn)2.
If ~x =
[x1x2
]∈ R2,
0x
yX = (x1, x2)
~x
then the length of the vector ~x is the distance from the origin 0 to the pointX = (x1, x2) given by d(0,X ).The length of ~x , denoted ‖~x‖, is given by:
d(0,X ) = ‖~x‖ =√x21 + x22 .
Rn : Vectors Length of a Vector Page 22/31
The formula for calculating the length of a vector generalizes to Rn: if
~x =
x1x2...xn
∈ Rn,
then
‖~x‖ =√x21 + x22 + · · ·+ x2n ,
which represents the distance from the origin to the point (x1, x2, . . . , xn).
Rn : Vectors Length of a Vector Page 23/31
Example
Let ~p =
[−34
]and ~q =
3−1−2
. Then −2~q = (−2)~q =
−624
.
The lengths of these vectors are
‖~p‖ =√
(−3)2 + 42 =√
9 + 16 = 5,
‖~q‖ =√
(3)2 + (−1)2 + (−2)2 =√
9 + 1 + 4 =√
14,
and
‖ − 2~q‖ =√
(−6)2 + 22 + 42
=√
36 + 4 + 16
=√
56 =√
4× 14
= 2√
14 = 2‖~q‖.
Rn : Vectors Length of a Vector Page 24/31
Unit Vectors
DefinitionA unit vector is a vector of length one.
Example 100
,
010
,
001
,
√220√22
, are examples of unit vectors.
Example
If ~v 6= ~0, then1
‖~v‖~v
is a unit vector in the same direction as ~v .
Rn : Vectors Length of a Vector Page 25/31
Example
~v =
−132
is not a unit vector, since ‖~v‖ =√
14. However,
~u =1√14
~v =
−1√143√142√14
is a unit vector in the same direction as ~v , i.e.,
‖~u‖ =1√14‖~v‖ =
1√14
√14 = 1.
Example
If ~v and ~w are nonzero that have
the same direction, then ~v = ‖~v‖‖~w‖ ~w ;
opposite directions, then ~v = − ‖~v‖‖~w‖ ~w .
Rn : Vectors Length of a Vector Page 26/31
The Geometry of Scalar Multiplication
Scalar Multiplication. If ~v 6= ~0 and a ∈ R, a 6= 0, then a~v has length‖a~v‖ = |a| · ‖~v‖, and
I has the same direction as ~v if a > 0;I has direction opposite to ~v if a < 0.
Parallel Vectors. Two nonzero vectors are called parallel if they have thesame direction or opposite directions. It follows that nonzero vectors ~v and~w are parallel if and only if one is a scalar multiple of the other.
Rn : Vectors The Geometry of Scalar Multiplication Page 27/31
Problem
Let P = (1,−2, 1),Q = (−3, 0, 5), X = (2,−1, 5) and Y = (4,−2, 3) be points in
R3. Is−→PQ parallel to
−→XY ? Is
−→PX parallel to
−−→QY ?
Solution
−→PQ =
−424
,−→XY =
2−1−2
, and these vectors are parallel if−→PQ = k
−→XY for
some scalar k , i.e., −424
= k
2−1−2
or
−424
=
2k−k−2k
.
This gives a system of three equations in one variable, which is consistent, and
has unique solution k = −2. Therefore,−→PQ is parallel to
−→XY .
−→PX =
114
,−−→QY =
7−2−2
, and these vectors are parallel if−→PX = `
−−→QY for
some scalar `. You will find that no such ` exists, so−→PX is not parallel to
−−→QY .
Rn : Vectors The Geometry of Scalar Multiplication Page 28/31
Vector problems and examples
Problem
Find the point, M, that is midway between P1 = (−1,−4, 3) and P2 = (5, 0,−3).
Solution
0
P1 M
P2
−→0M =
−−→0P1 +
−−→P1M =
−−→0P1 +
1
2
−−−→P1P2 =
−1−4
3
+1
2
64−6
=
−1−4
3
+
32−3
=
2−2
0
.
Therefore M = (2,−2, 0).
Rn : Vectors Vector problems and examples Page 29/31
Problem
Find the two points trisecting the segment between P = (2, 3, 5) andQ = (8,−6, 2).
Solution
0
P A
B
Q
•−→0A =
−→0P + 1
3
−→PQ
•−→0B =
−→0P + 2
3
−→PQ
Since−→PQ =
6−9−3
,
−→0A =
235
+
2−3−1
=
404
and−→0B =
235
+
4−6−2
=
6−3
3
.
Therefore, the two points are A = (4, 0, 4) and B = (6,−3, 3).
Rn : Vectors Vector problems and examples Page 30/31
Example
If ABCD is an arbitrary quadrilateral, then the the midpoints of the four sides ofABCD are the vertices of a parallelogram.
A
B
C
D
Let M1 denote the midpoint of−→AB,
M1
M2 the midpoint of−→BC ,
M2
M3 the midpoint of−→CD, and
M3
M4 the midpoint of−→DA.
M4
It suffices to prove that−−−→M1M2 =
−−−→M4M3.
−−−→M1M2 =
−−→M1B +
−−→BM2
−−−→M4M3 =
−−→M4D +
−−→DM3
= 12
−→AB + 1
2
−→BC = 1
2
−→AD + 1
2
−→DC
= 12
−→AC = 1
2
−→AC
Since−−−→M1M2 =
−−−→M4M3, the points M1, M2, M3, M4 are the vertices of a
parallelogram.
Rn : Vectors Vector problems and examples Page 31/31