8.3

Vectors in the Plane

Introduction

  • A directed line segment has magnitude and direction.
  • Equivalent directed line segments have the same magnitude and direction.
  • A vector vv in the plane is the set of all directed line segments equivalent to a directed line segment PQ⃗\vec{PQ}, written as v=PQ⃗v = \vec{PQ}.
  • A vector in standard position has its initial point at the origin and is called a position vector.

Component Form of a Vector

  • A vector with initial point at the origin can be uniquely represented by the coordinates of its terminal point (v<em>1,v</em>2)(v<em>1, v</em>2).
  • The component form of a vector is written as v=⟨v<em>1,v</em>2⟩v = \langle v<em>1, v</em>2 \rangle, where v<em>1v<em>1 and v</em>2v</em>2 are the components of vv.
  • The component form of the vector with initial point P(p<em>1,p</em>2)P(p<em>1, p</em>2) and terminal point Q(q<em>1,q</em>2)Q(q<em>1, q</em>2) is PQ⃗=⟨q<em>1−p</em>1,q<em>2−p</em>2⟩\vec{PQ} = \langle q<em>1 - p</em>1, q<em>2 - p</em>2 \rangle.
  • The magnitude (or length) of vv is calculated by: ∣∣v∣∣=v<em>12+v</em>22||v|| = \sqrt{v<em>1^2 + v</em>2^2}.
  • If ∣∣v∣∣=1||v|| = 1, then vv is a unit vector.
  • ∣∣v∣∣=0||v|| = 0 if and only if vv is the zero vector, 00.

Vector Operations

  • Sum of vectors u=⟨u<em>1,u</em>2⟩u = \langle u<em>1, u</em>2 \rangle and v=⟨v<em>1,v</em>2⟩v = \langle v<em>1, v</em>2 \rangle is: u+v=⟨u<em>1+v</em>1,u<em>2+v</em>2⟩u + v = \langle u<em>1 + v</em>1, u<em>2 + v</em>2 \rangle.
  • Numbers in vector operations are called scalars.
  • Scalar multiple of kk times u=⟨u<em>1,u</em>2⟩u = \langle u<em>1, u</em>2 \rangle is: ku=⟨ku<em>1,ku</em>2⟩ku = \langle ku<em>1, ku</em>2 \rangle.
  • If kk is positive, kvkv has the same direction as vv, and if kk is negative, kvkv has the opposite direction.

Properties of Vector Addition and Scalar Multiplication

  • u+v=v+uu + v = v + u
  • (u+v)+w=u+(v+w)(u + v) + w = u + (v + w)
  • u+0=uu + 0 = u
  • u+(−u)=0u + (-u) = 0
  • c(du)=(cd)uc(du) = (cd)u
  • (c+d)u=cu+du(c + d)u = cu + du
  • c(u+v)=cu+cvc(u + v) = cu + cv
  • 1(u)=u1(u) = u
  • 0(u)=00(u) = 0
  • ∣∣cv∣∣=∣c∣∣∣v∣∣||cv|| = |c|||v||

Unit Vectors

  • To find a unit vector uu that has the same direction as a given nonzero vector vv, use u=v∣∣v∣∣u = \frac{v}{||v||}. This is called a unit vector.
  • Standard unit vectors: i=⟨1,0⟩i = \langle 1, 0 \rangle and j=⟨0,1⟩j = \langle 0, 1 \rangle.
  • v=⟨v<em>1,v</em>2⟩v = \langle v<em>1, v</em>2 \rangle can be represented as v=v<em>1i+v</em>2jv = v<em>1i + v</em>2j, where v<em>1v<em>1 is the horizontal component and v</em>2v</em>2 is the vertical component.
  • The vector sum v<em>1i+v</em>2jv<em>1i + v</em>2j is a linear combination of the vectors ii and jj.

Direction Angles

  • If uu is a unit vector and θ\theta is its direction angle, then u=⟨x,y⟩=⟨cosθ,sinθ⟩u = \langle x, y \rangle = \langle cos \theta, sin \theta \rangle.
  • If vv is any vector with direction angle θ\theta, then v=⟨∣∣v∣∣cosθ,∣∣v∣∣sinθ⟩v = \langle ||v||cos \theta, ||v||sin \theta \rangle
  • If v=⟨a,b⟩v = \langle a, b \rangle, then the direction angle θ\theta for vv can be determined from tanθ=batan \theta = \frac{b}{a}.
  • θ\theta is the direction angle of vector vv where vv is in standard position and θ\theta is the angle (measured counterclockwise) from the positive x-axis to vv.

Applications

  • Vectors can be used to model and solve real-life problems involving forces, velocities, and directions.