Question #197817

Find the total work done in moving a particle in a force field given by 𝐹 = 3𝑥𝑦𝑖 − 5𝑧𝑗 + 10𝑥𝑘 along the curve x = 𝑡 2 + 1, 𝑦 = 2𝑡2 , 𝑧 = 𝑡 3 𝑓𝑟𝑜𝑚 𝑡 = 1 𝑡𝑜 𝑡 = 2.


Expert's answer

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:


r⃗=(t2+1,2t2,t3)\vec{r} = \begin{pmatrix} t^2+1, &2t^2, & t^3 \end{pmatrix} (between t=1 and t=2) which givesdr⃗dt=(2t,4t,3t2)\frac{d\vec{r}}{dt} = \begin{pmatrix} 2t, &4t, & 3t^2 \end{pmatrix}


F⃗=(3xy,−5z,10x)\vec{F} = \begin{pmatrix} 3xy, &-5z, & 10x \end{pmatrix} which we have to substitute in terms of the 't' variable:


F⃗=(3(t2+1)(2t2),−5(t3),10(t2+1))\vec{F} =\begin{pmatrix} 3(t^2+1)(2t^2), &-5(t^3), & 10(t^2+1) \end{pmatrix}


F⃗=(6t4+6t2,−5t3,10+10t2)\vec{F} = \begin{pmatrix} 6t^4+6t^2, &-5t^3, & 10+10t^2 \end{pmatrix}


Then we substitute and calculate the total work:


W=∫CF⃗⋅ds⃗=∫CF⃗(dr⃗dt)dtW=\int_{C}^{} \vec{F}\cdot d\vec{s} =\int_{C}^{} \vec{F}(\frac{\mathrm{d} \vec{r}}{\mathrm{d} t}) dt


W=∫12(6t4+6t2,−5t3,10+10t2)⋅(2t,4t,3t2)dtW = \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


=∫12(12t5+12t3−20t4+30t2+30t4)dt=\int_{1}^{2} (12t^{5}+12t^{3}-20t^{4}+30t^{2}+30t^{4})dt


W=∫12(12t5+10t4+12t3+30t2)dt=[2t6+2t5+3t4+10t3]12=(2(26)+2(25)+3(24)+10(23))−(2(16)+2(15)+3(14)+10(13))=(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=(128+64+48+80)−(2+2+3+10)=320−17W = (128+64+48+80)-(2+2+3+10) =320-17


W=303 uW = 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.
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