2.9 Dot Product
Dot product of vectors A and B is written
as A·B (Read A dot B)
Define the magnitudes of A and B and the
angle between their tails
    A·B = AB cosθ       where 0°≤ θ ≤180°
Referred to as scalar
product of vectors as
result is a scalar
2.9 Dot Product

   Laws of Operation
1. Commutative law
    A·B = B·A
2. Multiplication by a scalar
    a(A·B) = (aA)·B = A·(aB) = (A·B)a
3. Distribution law
    A·(B + D) = (A·B) + (A·D)
2.9 Dot Product

Cartesian Vector Formulation
- Dot product of Cartesian unit vectors
Eg: i·i = (1)(1)cos0° = 1 and
i·j = (1)(1)cos90° = 0
- Similarly
    i·i = 1   j·j = 1   k·k = 1
    i·j = 0   i·k = 1 j·k = 1
2.9 Dot Product
  Cartesian Vector Formulation
  - Dot product of 2 vectors A and B
  A·B = (Axi + Ayj + Azk)· (Bxi + Byj + Bzk)
      = AxBx(i·i) + AxBy(i·j) + AxBz(i·k)
            + AyBx(j·i) + AyBy(j·j) + AyBz(j·k)
            + AzBx(k·i) + AzBy(k·j) + AzBz(k·k)
      = AxBx + AyBy + AzBz
Note: since result is a scalar, be careful of including
  any unit vectors in the result
2.9 Dot Product

 Applications
  - The angle formed between two vectors or
  intersecting lines
      θ = cos-1 [(A·B)/(AB)]   0°≤ θ ≤180°
Note: if A·B = 0, cos-10= 90°, A is
perpendicular to B
2.9 Dot Product
Applications
- The components of a vector parallel and
perpendicular to a line
- Component of A parallel or collinear with line aa’ is
defined by A║ (projection of A onto the line)
     A║ = A cos θ
- If direction of line is specified by unit vector u (u =
1),
      A║ = A cos θ = A·u
2.9 Dot Product

Applications
- If A║ is positive, A║ has a directional
sense same as u
- If A║ is negative, A║ has a directional
sense opposite to u
- A║ expressed as a vector
     A║ = A cos θ u
         = (A·u)u
2.9 Dot Product
Applications
For component of A perpendicular to line aa’
1. Since A = A║ + A┴,
    then A┴ = A - A║
2. θ = cos-1 [(A·u)/(A)]
    then A┴ = Asinθ
3. If A║ is known, by Pythagorean Theorem
     A⊥ = A2 + A||2
2.9 Dot Product
For angle θ between the
rope and the beam A,
- Unit vectors along the
beams, uA = rA/rA
- Unit vectors along the
ropes, ur=rr/rr
- Angle θ = cos-1
(rA.rr/rArr)
           = cos-1 (uA· ur)
2.9 Dot Product
For projection of the force
along the beam A
- Define direction of the beam
     uA = rA/rA
- Force as a Cartesian vector
    F = F(rr/rr) = Fur
- Dot product
     F║ = F║·uA
2.9 Dot Product
Example 2.16
The frame is subjected to a horizontal force
F = {300j} N. Determine the components of
this force parallel and perpendicular to the
member AB.
2.9 Dot Product
Solution
Since          r     r    r
      r
r     r       2i + 6 j + 3k
u B = rB =
      rB    (2)2 + (6)2 + (3)2
        r        r          r
= 0.286i + 0.857 j + 0.429k
Then
 r       r
FAB = F cosθ
   rr           r           r         r        r
= F .u B = (300 j ) ⋅ (0.286i + 0.857 j + 0.429k )
= (0)(0.286) + (300)(0.857) + (0)(0.429)
= 257.1N
2.9 Dot Product
Solution
Since result is a positive scalar,
FAB has the same sense of
direction as uB. Express in
Cartesian form
r     r r
FAB = FAB u AB
                  r        r        r
= (257.1N )(0.286i + 0.857 j + 0.429k )
       r       r      r
= {73.5i + 220 j + 110k }N
Perpendicular component
r    r r           r        r       r      r           r      r      r
F⊥ = F − FAB = 300 j − (73.5i + 220 j + 110k ) = {−73.5i + 80 j − 110k }N
2.9 Dot Product
Solution
Magnitude can be determined
From F┴ or from Pythagorean
Theorem
r         r2 r      2
F⊥ =      F − FAB

=   (300 N )2 − (257.1N )2
= 155 N
2.9 Dot Product
Example 2.17
The pipe is subjected to F = 800N. Determine the
angle θ between F and pipe segment BA, and the
magnitudes of the components of F, which are
parallel and perpendicular to BA.
2.9 Dot Product
Solution
For angle θ
rBA = {-2i - 2j + 1k}m
rBC = {- 3j + 1k}m
Thus,
            r r
            rBA ⋅ rBC (− 2 )(0 ) + (− 2 )(− 3) + (1)(1)
    cos θ = r r =
            rBA rBC                 3 10
    = 0.7379
    θ = 42.5o
2.9 Dot Product
Solution
Components ofr F
    r    r                        r
r        r       (−2i − 2 j + 1k )
u AB = rAB =
         rAB              3
                                r
    − 2 i +  − 2  r +  1  k
          r
=                j  
    3   3   3
 r         rr
FAB = F .u B
             r           r  2 r  2  r  1  r
= (− 758.9 j + 253.0k ) ⋅  − i +  −  j +  k
                              3   3   3
= 0 + 506.0 + 84.3
= 590 N
2.9 Dot Product
Solution
Checking from trigonometry,
r     r
FAB = F cos θ
= 800 cos 42.5o N
= 540 N
Magnitude can be determined
From F┴
r    r
F⊥ = F sin θ = 800 sin 42.5o = 540 N
2.9 Dot Product
Solution
Magnitude can be determined from F┴ or from
Pythagorean Theorem
r         r2 r 2
F⊥ =      F − FAB

=   (800)2 − (590)2
= 540 N

6161103 2.9 dot product

  • 1.
    2.9 Dot Product Dotproduct of vectors A and B is written as A·B (Read A dot B) Define the magnitudes of A and B and the angle between their tails A·B = AB cosθ where 0°≤ θ ≤180° Referred to as scalar product of vectors as result is a scalar
  • 2.
    2.9 Dot Product Laws of Operation 1. Commutative law A·B = B·A 2. Multiplication by a scalar a(A·B) = (aA)·B = A·(aB) = (A·B)a 3. Distribution law A·(B + D) = (A·B) + (A·D)
  • 3.
    2.9 Dot Product CartesianVector Formulation - Dot product of Cartesian unit vectors Eg: i·i = (1)(1)cos0° = 1 and i·j = (1)(1)cos90° = 0 - Similarly i·i = 1 j·j = 1 k·k = 1 i·j = 0 i·k = 1 j·k = 1
  • 4.
    2.9 Dot Product Cartesian Vector Formulation - Dot product of 2 vectors A and B A·B = (Axi + Ayj + Azk)· (Bxi + Byj + Bzk) = AxBx(i·i) + AxBy(i·j) + AxBz(i·k) + AyBx(j·i) + AyBy(j·j) + AyBz(j·k) + AzBx(k·i) + AzBy(k·j) + AzBz(k·k) = AxBx + AyBy + AzBz Note: since result is a scalar, be careful of including any unit vectors in the result
  • 5.
    2.9 Dot Product Applications - The angle formed between two vectors or intersecting lines θ = cos-1 [(A·B)/(AB)] 0°≤ θ ≤180° Note: if A·B = 0, cos-10= 90°, A is perpendicular to B
  • 6.
    2.9 Dot Product Applications -The components of a vector parallel and perpendicular to a line - Component of A parallel or collinear with line aa’ is defined by A║ (projection of A onto the line) A║ = A cos θ - If direction of line is specified by unit vector u (u = 1), A║ = A cos θ = A·u
  • 7.
    2.9 Dot Product Applications -If A║ is positive, A║ has a directional sense same as u - If A║ is negative, A║ has a directional sense opposite to u - A║ expressed as a vector A║ = A cos θ u = (A·u)u
  • 8.
    2.9 Dot Product Applications Forcomponent of A perpendicular to line aa’ 1. Since A = A║ + A┴, then A┴ = A - A║ 2. θ = cos-1 [(A·u)/(A)] then A┴ = Asinθ 3. If A║ is known, by Pythagorean Theorem A⊥ = A2 + A||2
  • 9.
    2.9 Dot Product Forangle θ between the rope and the beam A, - Unit vectors along the beams, uA = rA/rA - Unit vectors along the ropes, ur=rr/rr - Angle θ = cos-1 (rA.rr/rArr) = cos-1 (uA· ur)
  • 10.
    2.9 Dot Product Forprojection of the force along the beam A - Define direction of the beam uA = rA/rA - Force as a Cartesian vector F = F(rr/rr) = Fur - Dot product F║ = F║·uA
  • 11.
    2.9 Dot Product Example2.16 The frame is subjected to a horizontal force F = {300j} N. Determine the components of this force parallel and perpendicular to the member AB.
  • 12.
    2.9 Dot Product Solution Since r r r r r r 2i + 6 j + 3k u B = rB = rB (2)2 + (6)2 + (3)2 r r r = 0.286i + 0.857 j + 0.429k Then r r FAB = F cosθ rr r r r r = F .u B = (300 j ) ⋅ (0.286i + 0.857 j + 0.429k ) = (0)(0.286) + (300)(0.857) + (0)(0.429) = 257.1N
  • 13.
    2.9 Dot Product Solution Sinceresult is a positive scalar, FAB has the same sense of direction as uB. Express in Cartesian form r r r FAB = FAB u AB r r r = (257.1N )(0.286i + 0.857 j + 0.429k ) r r r = {73.5i + 220 j + 110k }N Perpendicular component r r r r r r r r r r F⊥ = F − FAB = 300 j − (73.5i + 220 j + 110k ) = {−73.5i + 80 j − 110k }N
  • 14.
    2.9 Dot Product Solution Magnitudecan be determined From F┴ or from Pythagorean Theorem r r2 r 2 F⊥ = F − FAB = (300 N )2 − (257.1N )2 = 155 N
  • 15.
    2.9 Dot Product Example2.17 The pipe is subjected to F = 800N. Determine the angle θ between F and pipe segment BA, and the magnitudes of the components of F, which are parallel and perpendicular to BA.
  • 16.
    2.9 Dot Product Solution Forangle θ rBA = {-2i - 2j + 1k}m rBC = {- 3j + 1k}m Thus, r r rBA ⋅ rBC (− 2 )(0 ) + (− 2 )(− 3) + (1)(1) cos θ = r r = rBA rBC 3 10 = 0.7379 θ = 42.5o
  • 17.
    2.9 Dot Product Solution Componentsofr F r r r r r (−2i − 2 j + 1k ) u AB = rAB = rAB 3 r  − 2 i +  − 2  r +  1  k r =   j    3   3   3 r rr FAB = F .u B r r  2 r  2  r  1  r = (− 758.9 j + 253.0k ) ⋅  − i +  −  j +  k  3   3   3 = 0 + 506.0 + 84.3 = 590 N
  • 18.
    2.9 Dot Product Solution Checkingfrom trigonometry, r r FAB = F cos θ = 800 cos 42.5o N = 540 N Magnitude can be determined From F┴ r r F⊥ = F sin θ = 800 sin 42.5o = 540 N
  • 19.
    2.9 Dot Product Solution Magnitudecan be determined from F┴ or from Pythagorean Theorem r r2 r 2 F⊥ = F − FAB = (800)2 − (590)2 = 540 N