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Engineering Mechanics:
 Statics in SI Units, 12e

    2               Force Vectors




        Copyright © 2010 Pearson Education South Asia Pte Ltd
Chapter Objectives

  • Parallelogram Law
  • Cartesian vector form
  • Dot product and angle between 2 vectors




           Copyright © 2010 Pearson Education South Asia Pte Ltd
Chapter Outline

  1.   Scalars and Vectors
  2.   Vector Operations
  3.   Vector Addition of Forces
  4.   Addition of a System of Coplanar Forces
  5.   Cartesian Vectors
  6.   Addition and Subtraction of Cartesian Vectors
  7.   Position Vectors
  8.   Force Vector Directed along a Line
  9.   Dot Product


             Copyright © 2010 Pearson Education South Asia Pte Ltd
2.1 Scalars and Vectors

  • Scalar
    – A quantity characterized by a positive or negative
    number
     – Indicated by letters in italic such as A
    e.g. Mass, volume and length




           Copyright © 2010 Pearson Education South Asia Pte Ltd
2.1 Scalars and Vectors

  • Vector
     – A quantity that has magnitude and direction
       e.g. Position, force and moment
                                                    
     – Represent by a letter with an arrow over it, A
                                      
    – Magnitude is designated as A
    – In this subject, vector is presented as A and its
      magnitude (positive quantity) as A




           Copyright © 2010 Pearson Education South Asia Pte Ltd
2.2 Vector Operations

  • Multiplication and Division of a Vector by a Scalar
    - Product of vector A and scalar a = aA
    - Magnitude = aA
    - Law of multiplication applies e.g. A/a = ( 1/a ) A, a≠0




           Copyright © 2010 Pearson Education South Asia Pte Ltd
2.2 Vector Operations

  • Vector Addition
    - Addition of two vectors A and B gives a resultant
      vector R by the parallelogram law
    - Result R can be found by triangle construction
    - Communicative e.g. R = A + B = B + A
    - Special case: Vectors A and B are collinear (both
      have the same line of action)




           Copyright © 2010 Pearson Education South Asia Pte Ltd
2.2 Vector Operations

  • Vector Subtraction
    - Special case of addition
    e.g. R’ = A – B = A + ( - B )
    - Rules of Vector Addition Applies




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2.3 Vector Addition of Forces

  Finding a Resultant Force
  • Parallelogram law is carried out to find the resultant
    force




  • Resultant,
    FR = ( F1 + F2 )


            Copyright © 2010 Pearson Education South Asia Pte Ltd
2.3 Vector Addition of Forces

  Procedure for Analysis
  • Parallelogram Law
    – Make a sketch using the parallelogram law
    – 2 components forces add to form the resultant force
    – Resultant force is shown by the diagonal of the
      parallelogram
    – The components is shown by the sides of the
      parallelogram




          Copyright © 2010 Pearson Education South Asia Pte Ltd
2.3 Vector Addition of Forces

  Procedure for Analysis
  • Trigonometry
    – Redraw half portion of the parallelogram
    – Magnitude of the resultant force can be determined
      by the law of cosines
    – Direction if the resultant force can be determined by
      the law of sines
    – Magnitude of the two components can be determined by
      the law of sines



          Copyright © 2010 Pearson Education South Asia Pte Ltd
Example 2.1

  The screw eye is subjected to two forces, F1 and F2.
  Determine the magnitude and direction of the resultant
  force.




           Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution

  Parallelogram Law
  Unknown: magnitude of FR and angle θ




           Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution

  Trigonometry
  Law of Cosines
  FR =   (100 N ) 2 + (150 N ) 2 − 2(100 N )(150 N ) cos115
  =   10000 + 22500 − 30000( − 0.4226) = 212.6 N = 213 N

  Law of Sines
  150 N 212.6 N
         =
   sin θ sin 115
           150 N
  sin θ =         ( 0.9063)
          212.6 N
  θ = 39.8
               Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution

  Trigonometry
  Direction Φ of FR measured from the horizontal
   φ = 39.8 + 15
   = 54.8 ∠φ




                Copyright © 2010 Pearson Education South Asia Pte Ltd
2.4 Addition of a System of Coplanar Forces


   • Scalar Notation
     – x and y axes are designated positive and negative
     – Components of forces expressed as algebraic
       scalars

     F = Fx + Fy
     Fx = F cos θ and Fy = F sin θ




           Copyright © 2010 Pearson Education South Asia Pte Ltd
2.4 Addition of a System of Coplanar Forces


   • Cartesian Vector Notation
     – Cartesian unit vectors i and j are used to designate
       the x and y directions
     – Unit vectors i and j have dimensionless magnitude
       of unity ( = 1 )
     – Magnitude is always a positive quantity,
       represented by scalars Fx and Fy


              F = Fx i + Fy j


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2.4 Addition of a System of Coplanar Forces


   • Coplanar Force Resultants
     To determine resultant of several coplanar forces:
     – Resolve force into x and y components
     – Addition of the respective components using scalar
        algebra
     – Resultant force is found using the parallelogram
        law
     – Cartesian vector notation:
        F1 = F1x i + F1 y j
         F2 = − F2 xi + F2 y j
         F3 = F3 x i − F3 y j
            Copyright © 2010 Pearson Education South Asia Pte Ltd
2.4 Addition of a System of Coplanar Forces


   • Coplanar Force Resultants
     – Vector resultant is therefore
        FR = F1 + F2 + F3
           = ( FRx ) i + ( FRy ) j

     – If scalar notation are used
        FRx = F1x − F2 x + F3 x
        FRy = F1 y + F2 y − F3 y



           Copyright © 2010 Pearson Education South Asia Pte Ltd
2.4 Addition of a System of Coplanar Forces


   • Coplanar Force Resultants
     – In all cases we have
        FRx = ∑ Fx
        FRy = ∑ Fy        * Take note of sign conventions

     – Magnitude of FR can be found by Pythagorean Theorem


                                               FRy
     FR = F + F
             2
            Rx
                     2
                    Ry    and θ = tan     -1

                                               FRx


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Example 2.5

  Determine x and y components of F1 and F2 acting on the
  boom. Express each force as a Cartesian vector.




           Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution

  Scalar Notation
  F1x = −200 sin 30 N = −100 N = 100 N ←
  F1 y = 200 cos 30 N = 173N = 173N ↑

  Hence, from the slope triangle, we have
             5
  θ = tan −1  
              12 




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Solution

  By similar triangles we have
             12 
  F2 x = 260  = 240 N
             13 
            5
  F2 y = 260  = 100 N
             13 
  Scalar Notation: F = 240 N →
                    2x

                       F2 y = −100 N = 100 N ↓

  Cartesian Vector Notation: F1 = { − 100i + 173 j} N
                                        F2 = { 240i − 100 j} N

            Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution

  Scalar Notation
  F1x = −200 sin 30 N = −100 N = 100 N ←
  F1 y = 200 cos 30 N = 173N = 173N ↑

  Hence, from the slope triangle, we have:
                    5
                     −1
            θ = tan  
                     12 
   Cartesian Vector Notation
 F1 = { − 100i + 173 j} N
 F2 = { 240i − 100 j} N
            Copyright © 2010 Pearson Education South Asia Pte Ltd
Example 2.6

  The link is subjected to two forces F1 and F2. Determine
  the magnitude and orientation of the resultant force.




           Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution I

  Scalar Notation:
   FRx = ΣFx :
   FRx = 600 cos 30 N − 400 sin 45 N
   = 236.8 N →
   FRy = ΣFy :
   FRy = 600 sin 30 N + 400 cos 45 N
   = 582.8 N ↑




             Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution I

  Resultant Force
   FR =   ( 236.8 N ) 2 + ( 582.8 N ) 2
  = 629 N
  From vector addition, direction angle θ is
              582.8 N 
  θ = tan −1          
              236.8 N 
  = 67.9




              Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution II

  Cartesian Vector Notation
  F1 = { 600cos30°i + 600sin30°j } N
  F2 = { -400sin45°i + 400cos45°j } N


  Thus,
  FR = F1 + F2
    = (600cos30ºN - 400sin45ºN)i
       + (600sin30ºN + 400cos45ºN)j
    = {236.8i + 582.8j}N
  The magnitude and direction of FR are determined in the
  same manner as 2010 Pearson Education South Asia Pte Ltd
           Copyright ©
                       before.
2.5 Cartesian Vectors


  • Right-Handed Coordinate System
     A rectangular or Cartesian coordinate system is said
     to be right-handed provided:
     – Thumb of right hand points in the direction of the
        positive z axis
     – z-axis for the 2D problem would be perpendicular,
        directed out of the page.




           Copyright © 2010 Pearson Education South Asia Pte Ltd
2.5 Cartesian Vectors

  • Rectangular Components of a Vector
    – A vector A may have one, two or three rectangular
      components along the x, y and z axes, depending on
      orientation
    – By two successive application of the parallelogram law
      A = A’ + Az
        A’ = Ax + Ay
    – Combing the equations,
      A can be expressed as
      A = Ax + Ay + Az


           Copyright © 2010 Pearson Education South Asia Pte Ltd
2.5 Cartesian Vectors

  • Unit Vector
    – Direction of A can be specified using a unit vector
    – Unit vector has a magnitude of 1
    – If A is a vector having a magnitude of A ≠ 0, unit
      vector having the same direction as A is expressed
      by uA = A / A. So that

               A = A uA




          Copyright © 2010 Pearson Education South Asia Pte Ltd
2.5 Cartesian Vectors

  • Cartesian Vector Representations
    – 3 components of A act in the positive i, j and k
      directions

       A = Axi + Ayj + AZk

       *Note the magnitude and direction
       of each components are separated,
       easing vector algebraic operations.



          Copyright © 2010 Pearson Education South Asia Pte Ltd
2.5 Cartesian Vectors

  • Magnitude of a Cartesian Vector
    – From the colored triangle, A =               A'2 + Az2

    – From the shaded triangle, A' = Ax + Ay
                                      2    2




    – Combining the equations
      gives magnitude of A

         A = Ax + Ay + Az2
              2    2




          Copyright © 2010 Pearson Education South Asia Pte Ltd
2.5 Cartesian Vectors

  • Direction of a Cartesian Vector
    – Orientation of A is defined as the coordinate
      direction angles α, β and γ measured between the
      tail of A and the positive x, y and z axes
    – 0° ≤ α, β and γ ≤ 180 °
    – The direction cosines of A is
               Ax                    Az
       cos α =               cos γ =
               A                     A
                               Ay
                  cos β =
                               A

          Copyright © 2010 Pearson Education South Asia Pte Ltd
2.5 Cartesian Vectors

  • Direction of a Cartesian Vector
    – Angles α, β and γ can be determined by the
       inverse cosines
    Given
    A = Axi + Ayj + AZk


    then,
    uA = A /A = (Ax/A)i + (Ay/A)j + (AZ/A)k


    where A = Ax2 + Ay + Az2
                     2




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2.5 Cartesian Vectors

  • Direction of a Cartesian Vector
    – uA can also be expressed as
      uA = cosαi + cosβj + cosγk

    – Since A = Ax2 + Ay + Az2
                       2
                                                and uA = 1, we have
             cos α + cos β + cos γ = 1
                   2              2             2



    – A as expressed in Cartesian vector form is
      A = AuA
       = Acosαi + Acosβj + Acosγk
       = Axi + Ayj + AZk
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2.6 Addition and Subtraction of Cartesian Vectors


   • Concurrent Force Systems
      – Force resultant is the vector sum of all the forces in
        the system

         FR = ∑F = ∑Fxi + ∑Fyj + ∑Fzk




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Example 2.8

  Express the force F as Cartesian vector.




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Solution

  Since two angles are specified, the third angle is found by
   cos 2 α + cos 2 β + cos 2 γ = 1
   cos 2 α + cos 2 60  + cos 2 45 = 1
   cos α = 1 − (0.5) − (0.707 ) = ±0.5
                    2          2




  Two possibilities exit, namely
  α = cos −1 (0.5) = 60 
  α = cos −1 ( − 0.5) = 120



               Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution

  By inspection, α = 60º since Fx is in the +x direction
  Given F = 200N
        F = Fcosαi + Fcosβj + Fcosγk
          = (200cos60ºN)i + (200cos60ºN)j
            + (200cos45ºN)k
          = {100.0i + 100.0j + 141.4k}N
  Checking:
         F = Fx2 + Fy2 + Fz2

         =    (100.0)    2
                             + (100.0 ) + (141.4 ) = 200 N
                                         2               2



             Copyright © 2010 Pearson Education South Asia Pte Ltd
2.7 Position Vectors

  • x,y,z Coordinates
     – Right-handed coordinate system
     – Positive z axis points upwards, measuring the height of
       an object or the altitude of a point
     – Points are measured relative
       to the origin, O.




           Copyright © 2010 Pearson Education South Asia Pte Ltd
2.7 Position Vectors

  Position Vector
     – Position vector r is defined as a fixed vector which
         locates a point in space relative to another point.
     – E.g. r = xi + yj + zk




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2.7 Position Vectors

  Position Vector
     – Vector addition gives rA + r = rB
     – Solving
       r = rB – rA = (xB – xA)i + (yB – yA)j + (zB –zA)k
       or r = (xB – xA)i + (yB – yA)j + (zB –zA)k




            Copyright © 2010 Pearson Education South Asia Pte Ltd
2.7 Position Vectors

  •   Length and direction of cable AB can be found by
      measuring A and B using the x, y, z axes
  •   Position vector r can be established
  •   Magnitude r represent the length of cable
  •   Angles, α, β and γ represent the direction of the cable
  •   Unit vector, u = r/r




            Copyright © 2010 Pearson Education South Asia Pte Ltd
Example 2.12

  An elastic rubber band is attached to points A and B.
  Determine its length and its direction measured from A
  towards B.




           Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution

  Position vector
         r = [-2m – 1m]i + [2m – 0]j + [3m – (-3m)]k
           = {-3i + 2j + 6k}m

  Magnitude = length of the rubber band
        r=    ( − 3)   2
                           + ( 2) + ( 6) = 7m
                               2      2



  Unit vector in the director of r
  u = r /r
    = -3/7i + 2/7j + 6/7k

             Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution



  α = cos-1(-3/7) = 115°
  β = cos-1(2/7) = 73.4°
  γ = cos-1(6/7) = 31.0°




            Copyright © 2010 Pearson Education South Asia Pte Ltd
2.8 Force Vector Directed along a Line


   •   In 3D problems, direction of F is specified by 2 points,
       through which its line of action lies
   •   F can be formulated as a Cartesian vector
           F = F u = F (r/r)

   •   Note that F has units of forces (N)
       unlike r, with units of length (m)




             Copyright © 2010 Pearson Education South Asia Pte Ltd
2.8 Force Vector Directed along a Line

  •   Force F acting along the chain can be presented as a
      Cartesian vector by
      - Establish x, y, z axes
      - Form a position vector r along length of chain
  •   Unit vector, u = r/r that defines the direction of both
      the chain and the force
  •   We get F = Fu




            Copyright © 2010 Pearson Education South Asia Pte Ltd
Example 2.13

  The man pulls on the cord with a force of 350N.
  Represent this force acting on the support A, as a
  Cartesian vector and determine its direction.




           Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution

  End points of the cord are A (0m, 0m, 7.5m) and
  B (3m, -2m, 1.5m)
  r = (3m – 0m)i + (-2m – 0m)j + (1.5m – 7.5m)k
    = {3i – 2j – 6k}m

  Magnitude = length of cord AB

  r=   ( 3m ) 2 + ( − 2m ) 2 + ( − 6m ) 2   = 7m


  Unit vector,
  u = r /r
    = 3/7i - 2/7j - 6/7k

                 Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution

  Force F has a magnitude of 350N, direction specified by
  u.
  F = Fu
    = 350N(3/7i - 2/7j - 6/7k)
    = {150i - 100j - 300k} N

  α = cos-1(3/7) = 64.6°
  β = cos-1(-2/7) = 107°
  γ = cos-1(-6/7) = 149°



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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




            Copyright © 2010 Pearson Education South Asia Pte Ltd
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)




           Copyright © 2010 Pearson Education South Asia Pte Ltd
2.9 Dot Product

  • Cartesian Vector Formulation
    - Dot product of Cartesian unit vectors
        i·i = (1)(1)cos0° = 1
        i·j = (1)(1)cos90° = 0
    - Similarly
        i·i = 1 j·j = 1 k·k = 1
        i·j = 0 i·k = 1j·k = 1




          Copyright © 2010 Pearson Education South Asia Pte Ltd
2.9 Dot Product

  • Cartesian Vector Formulation
    – Dot product of 2 vectors A and B
      A·B = AxBx + AyBy + AzBz
  • Applications
    – The angle formed between two vectors or
      intersecting lines.
       θ = cos-1 [(A·B)/(AB)] 0°≤ θ ≤180°
    – The components of a vector parallel and
      perpendicular to a line.
      Aa = A cos θ = A·u

          Copyright © 2010 Pearson Education South Asia Pte Ltd
Example 2.17

  The frame is subjected to a horizontal force F = {300j} N.
  Determine the components of this force parallel and
  perpendicular to the member AB.




            Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution

  Since                         
        
       r       2i + 6 j + 3k
  u B = B =
        rB    ( 2 ) 2 + ( 6 ) 2 + ( 3) 2
                                  
  = 0.286i + 0.857 j + 0.429k
  Thus
          
  FAB = F cosθ
                                              
  = F .u B = ( 300 j ) ⋅ ( 0.286i + 0.857 j + 0.429k )
  = (0)(0.286) + (300)(0.857) + (0)(0.429)
  = 257.1N


                Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution

  Since result is a positive scalar, FAB has the same sense
  of direction as uB. Express in Cartesian form
         
  FAB = FAB u AB
                                       
  = ( 257.1N ) ( 0.286i + 0.857 j + 0.429k )
                         
  = {73.5i + 220 j + 110k }N
  Perpendicular component
                                                                      
                                                               
  F⊥ = F − FAB    = 300 j − (73.5i + 220 j + 110k ) = {−73.5i + 80 j − 110k }N




               Copyright © 2010 Pearson Education South Asia Pte Ltd
Solution

  Magnitude can be determined from F┴ or from
  Pythagorean Theorem,
        2  2
  F⊥ = F − FAB

  =   ( 300 N ) 2 − ( 257.1N ) 2
  = 155 N




               Copyright © 2010 Pearson Education South Asia Pte Ltd
QUIZ

1. Which one of the following is a scalar quantity?
    A) Force B) Position C) Mass D) Velocity

2. For vector addition, you have to use ______ law.
  A) Newton’s Second
  B) the arithmetic
  C) Pascal’s
  D) the parallelogram




             Copyright © 2010 Pearson Education South Asia Pte Ltd
QUIZ

3. Can you resolve a 2-D vector along two directions,
   which are not at 90° to each other?
   A) Yes, but not uniquely.
   B) No.
   C) Yes, uniquely.

4. Can you resolve a 2-D vector along three directions
   (say at 0, 60, and 120°)?
   A) Yes, but not uniquely.
   B) No.
   C) Yes, uniquely.
            Copyright © 2010 Pearson Education South Asia Pte Ltd
QUIZ

5. Resolve F along x and y axes and write it in vector
   form. F = { ___________ } N                y
  A) 80 cos (30°) i – 80 sin (30°) j                          x
  B) 80 sin (30°) i + 80 cos (30°) j          30°
  C) 80 sin (30°) i – 80 cos (30°) j                   F = 80 N
  D) 80 cos (30°) i + 80 sin (30°) j
6. Determine the magnitude of the resultant (F1 + F2)
   force in N when F1={ 10i + 20j }N and F2={ 20i + 20j }
   N.
  A) 30 N            B) 40 N           C) 50 N
  D) 60 N            E) 70 N
             Copyright © 2010 Pearson Education South Asia Pte Ltd
QUIZ

7. Vector algebra, as we are going to use it, is based on

    a ___________ coordinate system.
  A) Euclidean B) Left-handed
  C) Greek     D) Right-handed       E) Egyptian

8. The symbols α, β, and γ designate the __________ of

    a 3-D Cartesian vector.
  A) Unit vectors      B) Coordinate direction angles
  C) Greek societies   D) X, Y and Z components
            Copyright © 2010 Pearson Education South Asia Pte Ltd
QUIZ

9. What is not true about an unit vector, uA ?
   A) It is dimensionless.
   B) Its magnitude is one.
   C) It always points in the direction of positive X- axis.
   D) It always points in the direction of vector A.

10. If F = {10 i + 10 j + 10 k} N and
     G = {20 i + 20 j + 20 k } N, then F + G = { ____ } N
    A) 10 i + 10 j + 10 k
    B) 30 i + 20 j + 30 k
    C) – 10 i – 10 j – 10 k
    D) 30 i + 30 j + 30 k
              Copyright © 2010 Pearson Education South Asia Pte Ltd
QUIZ

11. A position vector, rPQ, is obtained by
A)   Coordinates of Q minus coordinates of P
B)   Coordinates of P minus coordinates of Q
C)   Coordinates of Q minus coordinates of the origin
D)   Coordinates of the origin minus coordinates of P

12. A force of magnitude F, directed along a unit vector U, is given
by F = ______ .
A) F (U)
B) U / F
C) F / U
D) F + U
E) F – U
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QUIZ

13. P and Q are two points in a 3-D space. How are the
  position vectors rPQ and rQP related?
A) rPQ = rQP      B) rPQ = - rQP
C) rPQ = 1/rQP D) rPQ = 2 rQP


14. If F and r are force vector and position vectors,
  respectively, in SI units, what are the units of the
  expression (r * (F / F)) ?
A) Newton               B) Dimensionless
C) Meter                D) Newton - Meter
E) The expression is algebraically illegal.
            Copyright © 2010 Pearson Education South Asia Pte Ltd
QUIZ

15. Two points in 3 – D space have coordinates of P (1,
2, 3) and Q (4, 5, 6) meters. The position vector rQP is
given by
A) {3 i + 3 j + 3 k} m
B) {– 3 i – 3 j – 3 k} m
C) {5 i + 7 j + 9 k} m
D) {– 3 i + 3 j + 3 k} m
E) {4 i + 5 j + 6 k} m

16. Force vector, F, directed along a line PQ is given by
A) (F/ F) rPQ       B) rPQ/rPQ
C) F(rPQ/rPQ)       D) F(rPQ/rPQ)
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QUIZ

17. The dot product of two vectors P and Q is defined as
  A) P Q cos θ       B) P Q sin θ                  P

  C) P Q tan θ       D) P Q sec θ              θ

                                                                    Q
18. The dot product of two vectors results in a _________
  quantity.
  A) Scalar       B) Vector
  C) Complex      D) Zero




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QUIZ

19. If a dot product of two non-zero vectors is 0, then the two vectors
must be _____________ to each other.
A) Parallel (pointing in the same direction)
B) Parallel (pointing in the opposite direction)
C) Perpendicular
D) Cannot be determined.

20. If a dot product of two non-zero vectors equals -1, then the
vectors must be ________ to each other.
A) Parallel (pointing in the same direction)
B) Parallel (pointing in the opposite direction)
C) Perpendicular
D) Cannot be determined.
               Copyright © 2010 Pearson Education South Asia Pte Ltd
QUIZ

1. The dot product can be used to find all of the following
except ____ .
A) sum of two vectors
B) angle between two vectors
C) component of a vector parallel to another line
D) component of a vector perpendicular to another line

2. Find the dot product of the two vectors P and Q.
   P = {5 i + 2 j + 3 k} m
  Q = {-2 i + 5 j + 4 k} m
  A) -12 m              B) 12 m           C) 12 m2
  D) -12 m2            E) 10 m2
             Copyright © 2010 Pearson Education South Asia Pte Ltd

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Bab2

  • 1. Engineering Mechanics: Statics in SI Units, 12e 2 Force Vectors Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 2. Chapter Objectives • Parallelogram Law • Cartesian vector form • Dot product and angle between 2 vectors Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 3. Chapter Outline 1. Scalars and Vectors 2. Vector Operations 3. Vector Addition of Forces 4. Addition of a System of Coplanar Forces 5. Cartesian Vectors 6. Addition and Subtraction of Cartesian Vectors 7. Position Vectors 8. Force Vector Directed along a Line 9. Dot Product Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 4. 2.1 Scalars and Vectors • Scalar – A quantity characterized by a positive or negative number – Indicated by letters in italic such as A e.g. Mass, volume and length Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 5. 2.1 Scalars and Vectors • Vector – A quantity that has magnitude and direction e.g. Position, force and moment  – Represent by a letter with an arrow over it, A  – Magnitude is designated as A – In this subject, vector is presented as A and its magnitude (positive quantity) as A Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 6. 2.2 Vector Operations • Multiplication and Division of a Vector by a Scalar - Product of vector A and scalar a = aA - Magnitude = aA - Law of multiplication applies e.g. A/a = ( 1/a ) A, a≠0 Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 7. 2.2 Vector Operations • Vector Addition - Addition of two vectors A and B gives a resultant vector R by the parallelogram law - Result R can be found by triangle construction - Communicative e.g. R = A + B = B + A - Special case: Vectors A and B are collinear (both have the same line of action) Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 8. 2.2 Vector Operations • Vector Subtraction - Special case of addition e.g. R’ = A – B = A + ( - B ) - Rules of Vector Addition Applies Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 9. 2.3 Vector Addition of Forces Finding a Resultant Force • Parallelogram law is carried out to find the resultant force • Resultant, FR = ( F1 + F2 ) Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 10. 2.3 Vector Addition of Forces Procedure for Analysis • Parallelogram Law – Make a sketch using the parallelogram law – 2 components forces add to form the resultant force – Resultant force is shown by the diagonal of the parallelogram – The components is shown by the sides of the parallelogram Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 11. 2.3 Vector Addition of Forces Procedure for Analysis • Trigonometry – Redraw half portion of the parallelogram – Magnitude of the resultant force can be determined by the law of cosines – Direction if the resultant force can be determined by the law of sines – Magnitude of the two components can be determined by the law of sines Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 12. Example 2.1 The screw eye is subjected to two forces, F1 and F2. Determine the magnitude and direction of the resultant force. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 13. Solution Parallelogram Law Unknown: magnitude of FR and angle θ Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 14. Solution Trigonometry Law of Cosines FR = (100 N ) 2 + (150 N ) 2 − 2(100 N )(150 N ) cos115 = 10000 + 22500 − 30000( − 0.4226) = 212.6 N = 213 N Law of Sines 150 N 212.6 N = sin θ sin 115 150 N sin θ = ( 0.9063) 212.6 N θ = 39.8 Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 15. Solution Trigonometry Direction Φ of FR measured from the horizontal φ = 39.8 + 15 = 54.8 ∠φ Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 16. 2.4 Addition of a System of Coplanar Forces • Scalar Notation – x and y axes are designated positive and negative – Components of forces expressed as algebraic scalars F = Fx + Fy Fx = F cos θ and Fy = F sin θ Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 17. 2.4 Addition of a System of Coplanar Forces • Cartesian Vector Notation – Cartesian unit vectors i and j are used to designate the x and y directions – Unit vectors i and j have dimensionless magnitude of unity ( = 1 ) – Magnitude is always a positive quantity, represented by scalars Fx and Fy F = Fx i + Fy j Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 18. 2.4 Addition of a System of Coplanar Forces • Coplanar Force Resultants To determine resultant of several coplanar forces: – Resolve force into x and y components – Addition of the respective components using scalar algebra – Resultant force is found using the parallelogram law – Cartesian vector notation: F1 = F1x i + F1 y j F2 = − F2 xi + F2 y j F3 = F3 x i − F3 y j Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 19. 2.4 Addition of a System of Coplanar Forces • Coplanar Force Resultants – Vector resultant is therefore FR = F1 + F2 + F3 = ( FRx ) i + ( FRy ) j – If scalar notation are used FRx = F1x − F2 x + F3 x FRy = F1 y + F2 y − F3 y Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 20. 2.4 Addition of a System of Coplanar Forces • Coplanar Force Resultants – In all cases we have FRx = ∑ Fx FRy = ∑ Fy * Take note of sign conventions – Magnitude of FR can be found by Pythagorean Theorem FRy FR = F + F 2 Rx 2 Ry and θ = tan -1 FRx Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 21. Example 2.5 Determine x and y components of F1 and F2 acting on the boom. Express each force as a Cartesian vector. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 22. Solution Scalar Notation F1x = −200 sin 30 N = −100 N = 100 N ← F1 y = 200 cos 30 N = 173N = 173N ↑ Hence, from the slope triangle, we have 5 θ = tan −1    12  Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 23. Solution By similar triangles we have  12  F2 x = 260  = 240 N  13  5 F2 y = 260  = 100 N  13  Scalar Notation: F = 240 N → 2x F2 y = −100 N = 100 N ↓ Cartesian Vector Notation: F1 = { − 100i + 173 j} N F2 = { 240i − 100 j} N Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 24. Solution Scalar Notation F1x = −200 sin 30 N = −100 N = 100 N ← F1 y = 200 cos 30 N = 173N = 173N ↑ Hence, from the slope triangle, we have: 5 −1 θ = tan    12  Cartesian Vector Notation F1 = { − 100i + 173 j} N F2 = { 240i − 100 j} N Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 25. Example 2.6 The link is subjected to two forces F1 and F2. Determine the magnitude and orientation of the resultant force. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 26. Solution I Scalar Notation: FRx = ΣFx : FRx = 600 cos 30 N − 400 sin 45 N = 236.8 N → FRy = ΣFy : FRy = 600 sin 30 N + 400 cos 45 N = 582.8 N ↑ Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 27. Solution I Resultant Force FR = ( 236.8 N ) 2 + ( 582.8 N ) 2 = 629 N From vector addition, direction angle θ is  582.8 N  θ = tan −1    236.8 N  = 67.9 Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 28. Solution II Cartesian Vector Notation F1 = { 600cos30°i + 600sin30°j } N F2 = { -400sin45°i + 400cos45°j } N Thus, FR = F1 + F2 = (600cos30ºN - 400sin45ºN)i + (600sin30ºN + 400cos45ºN)j = {236.8i + 582.8j}N The magnitude and direction of FR are determined in the same manner as 2010 Pearson Education South Asia Pte Ltd Copyright © before.
  • 29. 2.5 Cartesian Vectors • Right-Handed Coordinate System A rectangular or Cartesian coordinate system is said to be right-handed provided: – Thumb of right hand points in the direction of the positive z axis – z-axis for the 2D problem would be perpendicular, directed out of the page. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 30. 2.5 Cartesian Vectors • Rectangular Components of a Vector – A vector A may have one, two or three rectangular components along the x, y and z axes, depending on orientation – By two successive application of the parallelogram law A = A’ + Az A’ = Ax + Ay – Combing the equations, A can be expressed as A = Ax + Ay + Az Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 31. 2.5 Cartesian Vectors • Unit Vector – Direction of A can be specified using a unit vector – Unit vector has a magnitude of 1 – If A is a vector having a magnitude of A ≠ 0, unit vector having the same direction as A is expressed by uA = A / A. So that A = A uA Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 32. 2.5 Cartesian Vectors • Cartesian Vector Representations – 3 components of A act in the positive i, j and k directions A = Axi + Ayj + AZk *Note the magnitude and direction of each components are separated, easing vector algebraic operations. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 33. 2.5 Cartesian Vectors • Magnitude of a Cartesian Vector – From the colored triangle, A = A'2 + Az2 – From the shaded triangle, A' = Ax + Ay 2 2 – Combining the equations gives magnitude of A A = Ax + Ay + Az2 2 2 Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 34. 2.5 Cartesian Vectors • Direction of a Cartesian Vector – Orientation of A is defined as the coordinate direction angles α, β and γ measured between the tail of A and the positive x, y and z axes – 0° ≤ α, β and γ ≤ 180 ° – The direction cosines of A is Ax Az cos α = cos γ = A A Ay cos β = A Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 35. 2.5 Cartesian Vectors • Direction of a Cartesian Vector – Angles α, β and γ can be determined by the inverse cosines Given A = Axi + Ayj + AZk then, uA = A /A = (Ax/A)i + (Ay/A)j + (AZ/A)k where A = Ax2 + Ay + Az2 2 Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 36. 2.5 Cartesian Vectors • Direction of a Cartesian Vector – uA can also be expressed as uA = cosαi + cosβj + cosγk – Since A = Ax2 + Ay + Az2 2 and uA = 1, we have cos α + cos β + cos γ = 1 2 2 2 – A as expressed in Cartesian vector form is A = AuA = Acosαi + Acosβj + Acosγk = Axi + Ayj + AZk Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 37. 2.6 Addition and Subtraction of Cartesian Vectors • Concurrent Force Systems – Force resultant is the vector sum of all the forces in the system FR = ∑F = ∑Fxi + ∑Fyj + ∑Fzk Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 38. Example 2.8 Express the force F as Cartesian vector. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 39. Solution Since two angles are specified, the third angle is found by cos 2 α + cos 2 β + cos 2 γ = 1 cos 2 α + cos 2 60  + cos 2 45 = 1 cos α = 1 − (0.5) − (0.707 ) = ±0.5 2 2 Two possibilities exit, namely α = cos −1 (0.5) = 60  α = cos −1 ( − 0.5) = 120 Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 40. Solution By inspection, α = 60º since Fx is in the +x direction Given F = 200N F = Fcosαi + Fcosβj + Fcosγk = (200cos60ºN)i + (200cos60ºN)j + (200cos45ºN)k = {100.0i + 100.0j + 141.4k}N Checking: F = Fx2 + Fy2 + Fz2 = (100.0) 2 + (100.0 ) + (141.4 ) = 200 N 2 2 Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 41. 2.7 Position Vectors • x,y,z Coordinates – Right-handed coordinate system – Positive z axis points upwards, measuring the height of an object or the altitude of a point – Points are measured relative to the origin, O. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 42. 2.7 Position Vectors Position Vector – Position vector r is defined as a fixed vector which locates a point in space relative to another point. – E.g. r = xi + yj + zk Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 43. 2.7 Position Vectors Position Vector – Vector addition gives rA + r = rB – Solving r = rB – rA = (xB – xA)i + (yB – yA)j + (zB –zA)k or r = (xB – xA)i + (yB – yA)j + (zB –zA)k Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 44. 2.7 Position Vectors • Length and direction of cable AB can be found by measuring A and B using the x, y, z axes • Position vector r can be established • Magnitude r represent the length of cable • Angles, α, β and γ represent the direction of the cable • Unit vector, u = r/r Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 45. Example 2.12 An elastic rubber band is attached to points A and B. Determine its length and its direction measured from A towards B. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 46. Solution Position vector r = [-2m – 1m]i + [2m – 0]j + [3m – (-3m)]k = {-3i + 2j + 6k}m Magnitude = length of the rubber band r= ( − 3) 2 + ( 2) + ( 6) = 7m 2 2 Unit vector in the director of r u = r /r = -3/7i + 2/7j + 6/7k Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 47. Solution α = cos-1(-3/7) = 115° β = cos-1(2/7) = 73.4° γ = cos-1(6/7) = 31.0° Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 48. 2.8 Force Vector Directed along a Line • In 3D problems, direction of F is specified by 2 points, through which its line of action lies • F can be formulated as a Cartesian vector F = F u = F (r/r) • Note that F has units of forces (N) unlike r, with units of length (m) Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 49. 2.8 Force Vector Directed along a Line • Force F acting along the chain can be presented as a Cartesian vector by - Establish x, y, z axes - Form a position vector r along length of chain • Unit vector, u = r/r that defines the direction of both the chain and the force • We get F = Fu Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 50. Example 2.13 The man pulls on the cord with a force of 350N. Represent this force acting on the support A, as a Cartesian vector and determine its direction. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 51. Solution End points of the cord are A (0m, 0m, 7.5m) and B (3m, -2m, 1.5m) r = (3m – 0m)i + (-2m – 0m)j + (1.5m – 7.5m)k = {3i – 2j – 6k}m Magnitude = length of cord AB r= ( 3m ) 2 + ( − 2m ) 2 + ( − 6m ) 2 = 7m Unit vector, u = r /r = 3/7i - 2/7j - 6/7k Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 52. Solution Force F has a magnitude of 350N, direction specified by u. F = Fu = 350N(3/7i - 2/7j - 6/7k) = {150i - 100j - 300k} N α = cos-1(3/7) = 64.6° β = cos-1(-2/7) = 107° γ = cos-1(-6/7) = 149° Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 53. 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 Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 54. 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) Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 55. 2.9 Dot Product • Cartesian Vector Formulation - Dot product of Cartesian unit vectors i·i = (1)(1)cos0° = 1 i·j = (1)(1)cos90° = 0 - Similarly i·i = 1 j·j = 1 k·k = 1 i·j = 0 i·k = 1j·k = 1 Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 56. 2.9 Dot Product • Cartesian Vector Formulation – Dot product of 2 vectors A and B A·B = AxBx + AyBy + AzBz • Applications – The angle formed between two vectors or intersecting lines. θ = cos-1 [(A·B)/(AB)] 0°≤ θ ≤180° – The components of a vector parallel and perpendicular to a line. Aa = A cos θ = A·u Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 57. Example 2.17 The frame is subjected to a horizontal force F = {300j} N. Determine the components of this force parallel and perpendicular to the member AB. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 58. Solution Since      r 2i + 6 j + 3k u B = B = rB ( 2 ) 2 + ( 6 ) 2 + ( 3) 2    = 0.286i + 0.857 j + 0.429k Thus   FAB = F cosθ      = F .u B = ( 300 j ) ⋅ ( 0.286i + 0.857 j + 0.429k ) = (0)(0.286) + (300)(0.857) + (0)(0.429) = 257.1N Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 59. Solution Since result is a positive scalar, FAB has the same sense of direction as uB. Express in Cartesian form    FAB = FAB u AB    = ( 257.1N ) ( 0.286i + 0.857 j + 0.429k )    = {73.5i + 220 j + 110k }N Perpendicular component           F⊥ = F − FAB = 300 j − (73.5i + 220 j + 110k ) = {−73.5i + 80 j − 110k }N Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 60. Solution Magnitude can be determined from F┴ or from Pythagorean Theorem,  2  2 F⊥ = F − FAB = ( 300 N ) 2 − ( 257.1N ) 2 = 155 N Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 61. QUIZ 1. Which one of the following is a scalar quantity? A) Force B) Position C) Mass D) Velocity 2. For vector addition, you have to use ______ law. A) Newton’s Second B) the arithmetic C) Pascal’s D) the parallelogram Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 62. QUIZ 3. Can you resolve a 2-D vector along two directions, which are not at 90° to each other? A) Yes, but not uniquely. B) No. C) Yes, uniquely. 4. Can you resolve a 2-D vector along three directions (say at 0, 60, and 120°)? A) Yes, but not uniquely. B) No. C) Yes, uniquely. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 63. QUIZ 5. Resolve F along x and y axes and write it in vector form. F = { ___________ } N y A) 80 cos (30°) i – 80 sin (30°) j x B) 80 sin (30°) i + 80 cos (30°) j 30° C) 80 sin (30°) i – 80 cos (30°) j F = 80 N D) 80 cos (30°) i + 80 sin (30°) j 6. Determine the magnitude of the resultant (F1 + F2) force in N when F1={ 10i + 20j }N and F2={ 20i + 20j } N. A) 30 N B) 40 N C) 50 N D) 60 N E) 70 N Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 64. QUIZ 7. Vector algebra, as we are going to use it, is based on a ___________ coordinate system. A) Euclidean B) Left-handed C) Greek D) Right-handed E) Egyptian 8. The symbols α, β, and γ designate the __________ of a 3-D Cartesian vector. A) Unit vectors B) Coordinate direction angles C) Greek societies D) X, Y and Z components Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 65. QUIZ 9. What is not true about an unit vector, uA ? A) It is dimensionless. B) Its magnitude is one. C) It always points in the direction of positive X- axis. D) It always points in the direction of vector A. 10. If F = {10 i + 10 j + 10 k} N and G = {20 i + 20 j + 20 k } N, then F + G = { ____ } N A) 10 i + 10 j + 10 k B) 30 i + 20 j + 30 k C) – 10 i – 10 j – 10 k D) 30 i + 30 j + 30 k Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 66. QUIZ 11. A position vector, rPQ, is obtained by A) Coordinates of Q minus coordinates of P B) Coordinates of P minus coordinates of Q C) Coordinates of Q minus coordinates of the origin D) Coordinates of the origin minus coordinates of P 12. A force of magnitude F, directed along a unit vector U, is given by F = ______ . A) F (U) B) U / F C) F / U D) F + U E) F – U Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 67. QUIZ 13. P and Q are two points in a 3-D space. How are the position vectors rPQ and rQP related? A) rPQ = rQP B) rPQ = - rQP C) rPQ = 1/rQP D) rPQ = 2 rQP 14. If F and r are force vector and position vectors, respectively, in SI units, what are the units of the expression (r * (F / F)) ? A) Newton B) Dimensionless C) Meter D) Newton - Meter E) The expression is algebraically illegal. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 68. QUIZ 15. Two points in 3 – D space have coordinates of P (1, 2, 3) and Q (4, 5, 6) meters. The position vector rQP is given by A) {3 i + 3 j + 3 k} m B) {– 3 i – 3 j – 3 k} m C) {5 i + 7 j + 9 k} m D) {– 3 i + 3 j + 3 k} m E) {4 i + 5 j + 6 k} m 16. Force vector, F, directed along a line PQ is given by A) (F/ F) rPQ B) rPQ/rPQ C) F(rPQ/rPQ) D) F(rPQ/rPQ) Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 69. QUIZ 17. The dot product of two vectors P and Q is defined as A) P Q cos θ B) P Q sin θ P C) P Q tan θ D) P Q sec θ θ Q 18. The dot product of two vectors results in a _________ quantity. A) Scalar B) Vector C) Complex D) Zero Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 70. QUIZ 19. If a dot product of two non-zero vectors is 0, then the two vectors must be _____________ to each other. A) Parallel (pointing in the same direction) B) Parallel (pointing in the opposite direction) C) Perpendicular D) Cannot be determined. 20. If a dot product of two non-zero vectors equals -1, then the vectors must be ________ to each other. A) Parallel (pointing in the same direction) B) Parallel (pointing in the opposite direction) C) Perpendicular D) Cannot be determined. Copyright © 2010 Pearson Education South Asia Pte Ltd
  • 71. QUIZ 1. The dot product can be used to find all of the following except ____ . A) sum of two vectors B) angle between two vectors C) component of a vector parallel to another line D) component of a vector perpendicular to another line 2. Find the dot product of the two vectors P and Q. P = {5 i + 2 j + 3 k} m Q = {-2 i + 5 j + 4 k} m A) -12 m B) 12 m C) 12 m2 D) -12 m2 E) 10 m2 Copyright © 2010 Pearson Education South Asia Pte Ltd