450 Chapter 16Vectors
(iii) Scalar multiplication.The product caof the scalar cand the vector ais obtained
by multiplying each component of aby c,
ca 1 = 1 (ca
x
, ca
y
, ca
z
) (16.11)
EXAMPLE 16.3
(i) Find the vector whose initial point P isp 1 = 1 (2, 1, 0)and whose terminal
point Q isq 1 = 1 (1, 3, −2). (ii) What is the length of a? (iii) Find the unit vector parallel
to a.
(i) a 1 = 1 q 1 − 1 p 1 = 1 (1, 3, −2) 1 − 1 (2, 1, 0) 1 = 1 (−1, 2, −2)
(ii)
(iii)â 1 = 1 a 2 |a| 1 = 1 (− 12 3, 2 2 3, − 22 3)
0 Exercises 2–5
EXAMPLE 16.4Given a 1 = 1 (2, 3, 1), b 1 = 1 (1, −2, 0), and c 1 = 1 (5, 2, −1), find (a)
d 1 = 12 a 1 + 13 b 1 − 1 cand (b)|d|.
(a) Ifd 1 = 1 (d
x
, d
y
,d
z
)then
d
x
1 = 12 a
x
1 + 13 b
x
1 − 1 c
x
1 = 1 (2 1 × 121 + 131 × 111 − 1 5) 1 = 12
d
y
1 = 12 a
y
1 + 13 b
y
1 − 1 c
y
1 = 1 (2 1 × 131 + 131 × 1 (−2) 1 − 1 2) 1 = 1 − 2
d
z
1 = 12 a
z
1 + 13 b
z
1 − 1 c
z
1 = 1 (2 1 × 111 + 131 × 101 − 1 (−1)) 1 = 13
andd 1 = 1 (2, −2, 3).
(b)
0 Exercises 6–10
Equation (16.9) for the equality of vectors and Example 16.4 show that, for vectors
in three dimensions, a vector equation is equivalent to three simultaneous scalar
equations, one for each component. Conversely, the three scalar equations are expressed
by the single vector equation. Vector algebra then provides a powerful method for
the formulation and solution of physical problems that involve vector quantities. The
resolution into the component equations is often necessary only when the solution
of a problem needs to be completed by the insertion of numerical values for the
components.
||d=++=+−+=ddd
xyz
222 2 22
22317()
|| ( )a=− ++− =12 2 3( )
22 2
a=PQ