(a)
Let's use the [ ] instead of the < > such that e-t
𝐫 ( t ) = [ e − t t − t 3 l n ( t ) ] 𝐫 (t)=\begin{bmatrix}
e^{-t} \\
t-t^3\\
ln(t)
\end{bmatrix} r ( t ) = ⎣ ⎡ e − t t − t 3 l n ( t ) ⎦ ⎤ so that the derivative of r (t) will be;
𝐫 ′ ( t ) = d 𝐫 d t ( t ) = [ d d t e − t d d t t − t 3 d d t l n ( t ) ] 𝐫'(t)=\frac{d𝐫}{dt} (t) = \begin{bmatrix}
\frac{d}{dt} e^{-t} \\
\frac{d}{dt} t-t^3 \\
\frac{d}{dt}ln (t)
\end{bmatrix} r ′ ( t ) = d t d r ( t ) = ⎣ ⎡ d t d e − t d t d t − t 3 d t d l n ( t ) ⎦ ⎤
= [ − e − t 1 − 3 t 3 1 t ] =\begin{bmatrix}
-e^{-t} \\
1- 3t^3 \\
\frac{1}{t}
\end{bmatrix} = ⎣ ⎡ − e − t 1 − 3 t 3 t 1 ⎦ ⎤
(b)
𝐫 ( t ) = 1 1 + t i + t 1 + t j + t 2 1 + t k 𝐫(t)=\frac{1}{1+t}i + \frac{t}{1+t}j + \frac{t^2}{1+t}k r ( t ) = 1 + t 1 i + 1 + t t j + 1 + t t 2 k here, we apply the formula;
𝐫 ′ ( t ) = lim Δ t → 0 𝐫 ( t + Δ t ) − 𝐫 ( t ) Δ t 𝐫'(t)= \lim\limits_{Δt→0} \frac{𝐫(t + Δt) - 𝐫(t)}{Δt} r ′ ( t ) = Δ t → 0 lim Δ t r ( t + Δ t ) − r ( t )
= lim Δ t → 0 1 1 + t + Δ t i + t + Δ t 1 + t + Δ t j + ( t + Δ t ) 2 1 + t + Δ t k − ( 1 1 + t i + t 1 + t j + t 2 1 + t k ) Δ t =\lim\limits_{Δt→0} \frac{\frac{1}{1+t + Δt}i + \frac{t + Δt}{1+t + Δt}j + \frac{(t + Δt)^2}{1+t + Δt}k- (\frac{1}{1+t}i + \frac{t}{1+t}j + \frac{t^2}{1+t}k)} {Δt} = Δ t → 0 lim Δ t 1 + t + Δ t 1 i + 1 + t + Δ t t + Δ t j + 1 + t + Δ t ( t + Δ t ) 2 k − ( 1 + t 1 i + 1 + t t j + 1 + t t 2 k )
= lim Δ t → 0 1 1 + t + Δ t i + t + Δ t 1 + t + Δ t j + ( t 2 + 2 t Δ t + ( Δ t ) 2 1 + t + Δ t k − ( 1 1 + t i + t 1 + t j + t 2 1 + t k ) Δ t =\lim\limits_{Δt→0} \frac{\frac{1}{1+t + Δt}i + \frac{t + Δt}{1+t + Δt}j + \frac{(t^2 + 2tΔt +(Δt)^2}{1+t + Δt}k- (\frac{1}{1+t}i + \frac{t}{1+t}j + \frac{t^2}{1+t}k)} {Δt} = Δ t → 0 lim Δ t 1 + t + Δ t 1 i + 1 + t + Δ t t + Δ t j + 1 + t + Δ t ( t 2 + 2 t Δ t + ( Δ t ) 2 k − ( 1 + t 1 i + 1 + t t j + 1 + t t 2 k )
= lim Δ t → 0 [ 1 1 + t + Δ t − 1 1 + t ] i + [ t + Δ t 1 + t + Δ t − t 1 + t ] j + [ ( t 2 + 2 t Δ t + ( Δ t ) 2 1 + t + Δ t − t 2 1 + t ] k Δ t =\lim\limits_{Δt→0}\frac{[\frac{1}{1+t + Δt}- \frac{1}{1+t}] i + [\frac{t + Δt}{1+t + Δt}-\frac{t}{1+t}]j + [\frac{(t^2 + 2tΔt +(Δt)^2}{1+t + Δt}-\frac{t^2}{1+t}] k} {Δt} = Δ t → 0 lim Δ t [ 1 + t + Δ t 1 − 1 + t 1 ] i + [ 1 + t + Δ t t + Δ t − 1 + t t ] j + [ 1 + t + Δ t ( t 2 + 2 t Δ t + ( Δ t ) 2 − 1 + t t 2 ] k
= lim Δ t → 0 [ 1 + t − 1 − t − Δ t ( 1 + t ) ( 1 + t + Δ t ) ] i + [ ( 1 + t ) − t ( 1 + t + Δ t ) ( 1 + t ) ( 1 + t + Δ t ) ] j + [ ( t + 1 ) ( t 2 + 2 t Δ t + ( Δ t ) 2 ) − t 2 ( 1 + t + Δ t ) ( 1 + t ) ( 1 + t + Δ t ) ] k Δ t =\lim\limits_{Δt→0}\frac{[\frac{1+t-1-t-Δt} {(1+t) (1+t+ Δt)}] i + [\frac{(1+t)-t(1+t+Δt)}{(1+t)(1+t + Δt)} ]j + [\frac{(t+1)(t^2+2tΔt+(Δt)^2) -t^2(1+t+Δt)} {(1+t)(1+t + Δt)}] k} {Δt} = Δ t → 0 lim Δ t [ ( 1 + t ) ( 1 + t + Δ t ) 1 + t − 1 − t − Δ t ] i + [ ( 1 + t ) ( 1 + t + Δ t ) ( 1 + t ) − t ( 1 + t + Δ t ) ] j + [ ( 1 + t ) ( 1 + t + Δ t ) ( t + 1 ) ( t 2 + 2 t Δ t + ( Δ t ) 2 ) − t 2 ( 1 + t + Δ t ) ] k
= lim Δ t → 0 [ − Δ t ( 1 + t ) ( 1 + t + Δ t ) ] i + [ Δ t ( 1 + t ) ( 1 + t + Δ t ) ] j + [ Δ t ( 2 t Δ t + t 2 + 2 t ) ( 1 + t ) ( 1 + t + Δ t ) ] k Δ t =\lim\limits_{Δt→0}\frac{[\frac{-Δt} {(1+t) (1+t+ Δt)}] i + [\frac{Δt} {(1+t)(1+t + Δt)} ]j + [\frac{ Δt (2tΔt+t^2+2t)} {(1+t)(1+t + Δt)}] k} {Δt} = Δ t → 0 lim Δ t [ ( 1 + t ) ( 1 + t + Δ t ) − Δ t ] i + [ ( 1 + t ) ( 1 + t + Δ t ) Δ t ] j + [ ( 1 + t ) ( 1 + t + Δ t ) Δ t ( 2 t Δ t + t 2 + 2 t ) ] k
= lim Δ t → 0 [ Δ t ( − 1 ( 1 + t ) ( 1 + t + Δ t ) ) ] i + [ Δ t ( 1 ( 1 + t ) ( 1 + t + Δ t ) ) ] j + [ Δ t ( 2 t Δ t + t 2 + 2 t ( 1 + t ) ( 1 + t + Δ t ) ) ] k Δ t =\lim\limits_{Δt→0}\frac{[Δt (\frac{-1} {(1+t) (1+t+ Δt)}) ] i + [ Δt(\frac{1} {(1+t)(1+t + Δt)}) ]j + [ Δt(\frac{ 2tΔt+t^2+2t} {(1+t)(1+t + Δt)}) ] k} {Δt} = Δ t → 0 lim Δ t [ Δ t ( ( 1 + t ) ( 1 + t + Δ t ) − 1 )] i + [ Δ t ( ( 1 + t ) ( 1 + t + Δ t ) 1 )] j + [ Δ t ( ( 1 + t ) ( 1 + t + Δ t ) 2 t Δ t + t 2 + 2 t )] k Factorize Δt outside so that we have;
= lim Δ t → 0 Δ t [ − 1 ( 1 + t ) ( 1 + t + Δ t ) i + 1 ( 1 + t ) ( 1 + t + Δ t ) j + 2 t Δ t + t 2 + 2 t ( 1 + t ) ( 1 + t + Δ t ) k ] Δ t = \lim\limits_{Δt→0}Δt\frac{ [ \frac{-1} {(1+t) (1+t+ Δt)} i + \frac{1} {(1+t)(1+t + Δt)} j + \frac{ 2tΔt+t^2+2t} {(1+t)(1+t + Δt)} k]} {Δt} = Δ t → 0 lim Δ t Δ t [ ( 1 + t ) ( 1 + t + Δ t ) − 1 i + ( 1 + t ) ( 1 + t + Δ t ) 1 j + ( 1 + t ) ( 1 + t + Δ t ) 2 t Δ t + t 2 + 2 t k ] and it cancels out, remaining with;
= lim Δ t → 0 − 1 ( 1 + t ) ( 1 + t + Δ t ) i + 1 ( 1 + t ) ( 1 + t + Δ t ) j + 2 t Δ t + t 2 + 2 t ( 1 + t ) ( 1 + t + Δ t ) k = \lim\limits_{Δt→0}{ \frac{-1} {(1+t) (1+t+ Δt)} i + \frac{1} {(1+t)(1+t + Δt)} j + \frac{ 2tΔt+t^2+2t} {(1+t)(1+t + Δt)} k} = Δ t → 0 lim ( 1 + t ) ( 1 + t + Δ t ) − 1 i + ( 1 + t ) ( 1 + t + Δ t ) 1 j + ( 1 + t ) ( 1 + t + Δ t ) 2 t Δ t + t 2 + 2 t k Now substitute the value of Δt
S o , t h e r e f o r e , 𝐫 ′ ( t ) = − 1 ( 1 + 2 t + t 2 ) i + 1 ( 1 + 2 t + t 2 ) j + t 2 + 2 t ( 1 + 2 t + t 2 ) k So, therefore, 𝐫'(t)= {\frac{-1} {(1+2t+t^2)} i + \frac{1} {(1+2t+t^2)} j + \frac{ t^2+2t} {(1+2t+t^2)} k} S o , t h ere f ore , r ′ ( t ) = ( 1 + 2 t + t 2 ) − 1 i + ( 1 + 2 t + t 2 ) 1 j + ( 1 + 2 t + t 2 ) t 2 + 2 t k