Letf(t)=cbe a constant vector. Thenf(t+h)=c, and so from the above definition
df
dt
=lim
h→ 0
(
f(t+h)−f(t)
h
)
=lim
h→ 0
(
c−c
h
)
= 0
The properties of differentiation of a vector look very much like those of ordinary
differentiation, although the notation may be a bit unnerving at first. We have three types
of product to contend with of course – multiplication by a scalar, scalar product and vector
product. On the other hand we don’t have to worry about a quotient rule, since we have
not defined division of vectors. The rules are as follows.
Ifs(t)is a scalar function andf(t)a vector function, then
(i)
d
dt
(s(t)f(t))=
ds(t)
dt
f(t)+s(t)
df(t)
dt
Ifg(t)is also a vector function, then
(ii)
d
dt
(f(t)+g(t))=
df(t)
dt
+
dg(t)
dt
(iii)
d
dt
(f·g)=f·
dg
dt
+
df
dt
·g
(iv)
d
dt
(f×g)=f×
dg
dt
+
df
dt
×g
where the order of vectors
must be preserved
(i) and (ii) show that differentiation of the component form is simple:
d
dt
(f 1 (t)i+f 2 (t)j+f 3 (t)k)=
df 1 (t)
dt
i+
df 2 (t)
dt
j+
df 3 (t)
dt
k
Problem 11.11
Differentiate the following vector functions with respect tot
(i) cos 4tiY3sin4tjYetk
(ii) tcostiYe−tsintjYt^2 k
(i)
d
dt
(cos 4ti+3sin4tj+etk)
=
d
dt
(cos 4t)i+
d
dt
(3sin4t)j+
d
dt
(et)k
=−4sin4ti+12 cos 4tj+etk
(ii)
d
dt
(tcosti+e−tsintj+t^2 k
=
d
dt
(tcost)i+
d
dt
(e−tsint)j+
d
dt
(t^2 )k
=(cost−tsint)i+(e−tcost−e−tsint)j+ 2 tk