The total work done can be found as the integral of the scalar product between the force vector F and a certain displacement trajectory vector ds . We use the definition for the curve r as well to proceed:
r ⃗ = ( t 2 + 1 , 2 t 2 , t 3 ) \vec{r} = \begin{pmatrix}
t^2+1, &2t^2, & t^3
\end{pmatrix} r = ( t 2 + 1 , 2 t 2 , t 3 ) (between t=1 and t=2) which givesd r ⃗ d t = ( 2 t , 4 t , 3 t 2 ) \frac{d\vec{r}}{dt} = \begin{pmatrix}
2t, &4t, & 3t^2
\end{pmatrix} d t d r = ( 2 t , 4 t , 3 t 2 )
F ⃗ = ( 3 x y , − 5 z , 10 x ) \vec{F} = \begin{pmatrix}
3xy, &-5z, & 10x
\end{pmatrix} F = ( 3 x y , − 5 z , 10 x ) which we have to substitute in terms of the 't' variable:
F ⃗ = ( 3 ( t 2 + 1 ) ( 2 t 2 ) , − 5 ( t 3 ) , 10 ( t 2 + 1 ) ) \vec{F} =\begin{pmatrix}
3(t^2+1)(2t^2), &-5(t^3), & 10(t^2+1)
\end{pmatrix} F = ( 3 ( t 2 + 1 ) ( 2 t 2 ) , − 5 ( t 3 ) , 10 ( t 2 + 1 ) )
F ⃗ = ( 6 t 4 + 6 t 2 , − 5 t 3 , 10 + 10 t 2 ) \vec{F} = \begin{pmatrix}
6t^4+6t^2, &-5t^3, & 10+10t^2
\end{pmatrix} F = ( 6 t 4 + 6 t 2 , − 5 t 3 , 10 + 10 t 2 )
Then we substitute and calculate the total work:
W = ∫ C F ⃗ ⋅ d s ⃗ = ∫ C F ⃗ ( d r ⃗ d t ) d t W=\int_{C}^{} \vec{F}\cdot d\vec{s} =\int_{C}^{} \vec{F}(\frac{\mathrm{d} \vec{r}}{\mathrm{d} t}) dt W = ∫ C F ⋅ d s = ∫ C F ( d t d r ) d t
W = ∫ 1 2 ( 6 t 4 + 6 t 2 , − 5 t 3 , 10 + 10 t 2 ) ⋅ ( 2 t , 4 t , 3 t 2 ) d t W = \int_{1}^{2}
\begin{pmatrix}
6t^4+6t^2, &-5t^3, & 10+10t^2
\end{pmatrix}
\cdot
\begin{pmatrix}
2t, &4t, & 3t^2
\end{pmatrix}
dt W = ∫ 1 2 ( 6 t 4 + 6 t 2 , − 5 t 3 , 10 + 10 t 2 ) ⋅ ( 2 t , 4 t , 3 t 2 ) d t
= ∫ 1 2 ( 12 t 5 + 12 t 3 − 20 t 4 + 30 t 2 + 30 t 4 ) d t =\int_{1}^{2} (12t^{5}+12t^{3}-20t^{4}+30t^{2}+30t^{4})dt = ∫ 1 2 ( 12 t 5 + 12 t 3 − 20 t 4 + 30 t 2 + 30 t 4 ) d t
W = ∫ 1 2 ( 12 t 5 + 10 t 4 + 12 t 3 + 30 t 2 ) d t = [ 2 t 6 + 2 t 5 + 3 t 4 + 10 t 3 ] 1 2 = ( 2 ( 2 6 ) + 2 ( 2 5 ) + 3 ( 2 4 ) + 10 ( 2 3 ) ) − ( 2 ( 1 6 ) + 2 ( 1 5 ) + 3 ( 1 4 ) + 10 ( 1 3 ) ) = ( 128 + 64 + 48 + 80 ) − ( 2 + 2 ) + 3 + 10 ) W=\int_{1}^{2} (12t^{5}+10t^{4}+12t^{3}+30t^{2})dt=\left [ 2t^{6}+2t^{5} +3t^{4}+10t^{3}\right ]_{1}^{2}= (2(2^6)+2(2^5)+3(2^4)+10(2^3))-(2(1^6)+2(1^5)+3(1^4)+10(1^3))=(128+64+48+80)-(2+2)+3+10) W = ∫ 1 2 ( 12 t 5 + 10 t 4 + 12 t 3 + 30 t 2 ) d t = [ 2 t 6 + 2 t 5 + 3 t 4 + 10 t 3 ] 1 2 = ( 2 ( 2 6 ) + 2 ( 2 5 ) + 3 ( 2 4 ) + 10 ( 2 3 )) − ( 2 ( 1 6 ) + 2 ( 1 5 ) + 3 ( 1 4 ) + 10 ( 1 3 )) = ( 128 + 64 + 48 + 80 ) − ( 2 + 2 ) + 3 + 10 )
W = ( 128 + 64 + 48 + 80 ) − ( 2 + 2 + 3 + 10 ) = 320 − 17 W = (128+64+48+80)-(2+2+3+10) =320-17 W = ( 128 + 64 + 48 + 80 ) − ( 2 + 2 + 3 + 10 ) = 320 − 17
W = 303 u W = 303\,u W = 303 u
In conclusion, the total work done is 303 units.
Reference:
Young, H. D., Freedman, R. A., & Ford, A. L. (2006). Sears and Zemansky's university physics (Vol. 1). Pearson education.