Higher Engineering Mathematics

(Greg DeLong) #1
SCALAR AND VECTOR PRODUCTS 245

D


  1. (a) 2p× 3 r(b) (p+r)×q
    [
    (a)− 36 i− 30 j− 54 k
    (b) 11i+ 4 j−k


]


  1. (a)p×(r×q) (b) (3p× 2 r)×q
    [
    (a)− 22 i−j+ 33 k
    (b) 18i+ 162 j+ 102 k


]


  1. For vectorsp= 4 i−j+ 2 kand
    q=− 2 i+ 3 j− 2 kdetermine: (i)p•q
    (ii)p×q(iii)|p×q|(iv)q×pand (v) the
    angle between the vectors.



(i)−15 (ii)− 4 i+ 4 j+ 10 k
(iii) 11.49 (iv) 4i− 4 j− 10 k
(v) 142. 55 ◦




  1. For vectorsa=− 7 i+ 4 j+^12 kandb= 6 i−
    5 j−k find (i) a•b (ii) a×b (iii)|a×b|
    (iv) b×aand (v) the angle between the
    vectors. ⎡




(i)− 6212 (ii)− 112 i− 4 j+ 11 k
(iii) 11.80 (iv) 1^12 i+ 4 j− 11 k
(v) 169. 31 ◦





  1. Forces of (i+ 3 j), (− 2 i−j), (i− 2 j) newtons
    act at three points having position vectors of
    (2i+ 5 j), 4jand (−i+j) metres respectively.
    Calculate the magnitude of the moment.
    [10 Nm]

  2. A force of (2i−j+k) newtons acts on a line
    through pointPhaving co-ordinates (0, 3, 1)
    metres. Determine the moment vector and its
    magnitude about pointQhaving co-ordinates
    (4, 0,−1) metres.
    [
    M=(5i+ 8 j− 2 k)Nm,
    |M|= 9 .64 Nm


]


  1. A sphere is rotating with angular velocityω
    about thez-axis of a system, the axis coincid-
    ing with the axis of the sphere. Determine the
    velocity vector and its magnitude at position
    (− 5 i+ 2 j− 7 k) m, when the angular velocity
    is (i+ 2 j) rad/s. [
    υ=− 14 i+ 7 j+ 12 k,
    |υ|= 19 .72 m/s


]


  1. Calculate the velocity vector and its magni-
    tude for a particle rotating about thez-axis
    at an angular velocity of (3i−j+ 2 k) rad/s
    when the position vector of the particle is at
    (i− 5 j+ 4 k)m.
    [6i− 10 j− 14 k, 18.22 m/s]


22.4 Vector equation of a line


The equation of a straight line may be determined,
given that it passes through the pointAwith position
vectorarelative toO, and is parallel to vectorb. Let
rbe the position vector of a pointPon the line, as
shown in Fig. 22.10.

b

a

r

A

P

O

Figure 22.10

By vector addition,OP=OA+AP,
i.e.r=a+AP.
However, as the straight line throughAis parallel
to the free vectorb(free vectormeans one that
has the same magnitude, direction and sense), then
AP=λb, whereλis a scalar quantity. Hence, from
above,

r=a+λb (8)

If, say,r=xi+yj+zk,a=a 1 i+a 2 j+a 3 kand
b=b 1 i+b 2 j+b 3 k, then from equation (8),

xi+yj+zk=(a 1 i+a 2 j+a 3 k)

+λ(b 1 i+b 2 j+b 3 k)

Hencex=a 1 +λb 1 ,y=a 2 +λb 2 andz=a 3 +λb 3.
Solving forλgives:

x−a 1
b 1

=

y−a 2
b 2

=

z−a 3
b 3

=λ (9)

Equation (9) is the standard Cartesian form for the
vector equation of a straight line.

Problem 11. (a) Determine the vector equa-
tion of the line through the point with position
vector 2i+ 3 j−kwhich is parallel to the vector
i− 2 j+ 3 k.
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