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Calculus and Vectors – How to get an A+

7.4 Dot Product of Algebraic Vectors A Dot Product for Standard Unit Vectors The dot product of the standard unit vectors is given by: r r r r r r i ⋅ i =1 j ⋅ j =1 k ⋅ k =1 r r r r r r i ⋅ j =0 j ⋅k =0 k ⋅i = 0 B Dot Product for two Algebraic Vectors The dot product of two algebraic vectors r r r r a = (a x , a y , a z ) = a x i + a y j + a z k and r r r r b = (b x , b y , b z ) = b x i + b y j + b z k is given by: r r a ⋅ b = a x bx + a y b y + a z bz Proof: r r r r r r r r a ⋅ b = (a x i + a y j + a z k ) ⋅ (bx i + b y j + bz k ) r r r r r r = (a x bx )(i ⋅ i ) + (a x b y (i ⋅ j ) + (a x bz )(i ⋅ k ) + r r r r r r + (a y bx )( j ⋅ i ) + (a y b y ( j ⋅ j ) + (a y bz )( j ⋅ k ) + r r r r r r + (a z bx )(k ⋅ i ) + (a z b y (k ⋅ j ) + (a z bz )(k ⋅ k )
= a x bx + a y b y + a z bz

Proof: r r r r i ⋅ i =|| i || || i || cos 0° = (1)(1)(1) = 1 r r r r i ⋅ j =|| i || || j || cos 90° = (1)(1)(0) = 0

r Ex 1. For each case, find the dot product of the vectors a r and b . r r a) a = (1,−2,0) , b = (0,−1,2) r r a ⋅ b = (1)(0) + (−2)(−1) + (0)(2) = 2 r r r r r r r b) a = −i + 2 j , b = i − 2 j − k r r a ⋅ b = (−1)(1) + (2)(−2) + (0)(−1) = −1 − 4 = −5 r r r r r c) a = (−1,1,−1) , b = −i + 2 j − 2k r r a ⋅ b = (−1)(−1) + (1)(2) + (−1)(−2) = 1 + 2 + 2 = 5

C Angle between two Vectors r r r The angle θ = ∠(a , b ) between two vectors a and r b (when positioned tail to tail) is given by: r r a x bx + a y b y + a z bz a ⋅b cosθ = r r = | a || b | a x 2 + a y 2 + a z 2 bx 2 + b y 2 + bz 2 Notes: r r 1. If cosθ = 1 then a ↑↑ b (vectors are parallel and have same direction). r r 2. If cosθ = −1 then a ↑↓ b (vectors are parallel but have opposite direction). r r 3. If cosθ = 0 then a ⊥ b (vectors are perpendicular to each other or orthogonal).

r Ex 2. For each case, find the angle between the vectors a r and b . r r a) a = (1,−2,−1) , b = (0,−1,2) r r a ⋅b (1)(0) + (−2)(−1) + (−1)(2) cosθ = r r = =0 2 | a || b | 1 + (−2) 2 + (−1) 2 0 2 + (−1) 2 + 2 2 r r ∴θ = cos −1 0 = 90° (a ⊥ b )

r r r r r r b) a = −i − 2k , b = −2 j + k r r a ⋅b (−1)(0) + (0)(−2) + (−2)(1) −2 = cosθ = r r = 5 | a || b | (−1) 2 + 0 2 + (−2) 2 0 2 + (−2) 2 + 12
∴θ = cos −1 (−2 / 5) = 113.58°

4. If cosθ > 0 then 0° < θ < 90° ( θ is an acute angle).

Ex 3. Find a non zero vector perpendicular to each of the r r vectors a = (1,5,−1) and b = (−3,1,2) . r r r Let v = ( x, y, z ) be a vector perpendicular to both a and b . So: r r a ⋅ v = 0 ⇒ x + 5 y − z = 0 (1) r r b ⋅ v = 0 ⇒ −3x + y + 2 z = 0 (2) (1) ⇒ z = x + 5 y (3) (2) ⇒ −3 x + y + 2( x + 5 y ) = 0 ⇒ 11 y = x (3) ⇒ z = 11y + 5 y = 16 y r v = ( x, y, z ) = (11y, y,16 y ) = y (11,1,16) r ∴ v = y (11,1,16), y ∈ R \ {0}

5. If cosθ < 0 then 90° < θ < 180° ( θ is an obtuse angle).

7.4 The Dot Product of Algebraic Vectors ©2010 Iulia & Teodoru Gugoiu - Page 1 of 2

Calculus and Vectors – How to get an A+

Ex 4. A triangle is defined by three points A(0,1,2) , B(1,0,2) , and C (−1,2,0) . Find the angles ∠A of this triangle.

Ex 5. Find the angles between the vector r r r r a = −2i + j + 3k and the coordinate axes. r r r r r a a ⋅i ∠(a , x − axis ) = ∠(a , i ) = cos −1 r r = cos −1 rx || a || || a || || i || r −2 ∴ ∠(a , x − axis ) = cos −1 ≅ 122.31° 14 r r ay r r r a⋅ j ∠(a , y − axis ) = ∠(a , j ) = cos −1 r r = cos −1 r || a || || a || || j || r 1 ∴ ∠(a , y − axis ) = cos −1 ≅ 74.5° 14 r r r r r a⋅k −1 −1 a z ∠(a , z − axis ) = ∠(a , k ) = cos r r r = cos || a || || a || || k || r 3 ∴ ∠(a , z − axis ) = cos −1 ≅ 36.7° 14

AB = (1,0,2) − (0,1,2) = (1,−1,0) AC = (−1,2,0) − (0,1,2) = (−1,1,−2) AB ⋅ AC −1 −1+ 0 −2 −1

cos A =

|| AB || || AC ||
−1

=

2 6

=

12

=

3

∴ ∠A = cos (−1 / 3 ) ≅ 125.26°

Ex 6. For what values of k are the vectors r r a = (k ,−2,3) and b = (2,2k − 6,6) a) perpendicular (orthogonal)? r r a ⋅ b = 0 ⇒ 2k − 2(2k − 6) + 18 = 0 ⇒ 2k − 4k + 12 + 18 = 0 ⇒ 30 = 2k ⇒∴ k = 15 b) parallel (collinear)? r r a = λb ⇒ (k ,−2,3) = λ (2,2k − 6,6) ⇒
⎧k = 2λ ⎪ ⎨− 2 = λ ( 2 k − 6) ⎪3 = 6λ ⇒ λ = 0.5 ⎩ k = 2(0.5) = 1 − 2 = 0.5(2 × 1 − 6) ⇒ −2 = −2 (true) ∴k = 1

c) in opposite direction? r r The vectors a and b are in opposite direction if r r there exists λ < 0 such that a = λb . But, according r r to part b) if a = λb then λ = 0.5 > 0 . r r Therefore the vectors a and b cannot be in opposite direction for any real value of the parameter k . Reading: Nelson Textbook, Pages 379-385 Homework: Nelson Textbook: Page #2c, 6d, 7a, 10, 13, 14, 18, 19

7.4 The Dot Product of Algebraic Vectors ©2010 Iulia & Teodoru Gugoiu - Page 2 of 2

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...Excerpt More information 1 Vector and tensor analysis Vectors and scalars Vector methods have become standard tools for the physicists. In this chapter we discuss the properties of the vectors and vector ®elds that occur in classical physics. We will do so in a way, and in a notation, that leads to the formation of abstract linear vector spaces in Chapter 5. A physical quantity that is completely speci®ed, in appropriate units, by a single number (called its magnitude) such as volume, mass, and temperature is called a scalar. Scalar quantities are treated as ordinary real numbers. They obey all the regular rules of algebraic addition, subtraction, multiplication, division, and so on. There are also physical quantities which require a magnitude and a direction for their complete speci®cation. These are called vectors if their combination with each other is commutative (that is the order of addition may be changed without a€ecting the result). Thus not all quantities possessing magnitude and direction are vectors. Angular displacement, for example, may be characterised by magnitude and direction but is not a vector, for the addition of two or more angular displacements is not, in general, commutative (Fig. 1.1). In print, we shall denote vectors by boldface letters (such as A) and use ordinary italic letters (such as A) for their magnitudes; in writing, vectors are usually ~ ~ represented by a letter with an arrow above it such as A. A given vector A (or A) can be written as ...

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