Work done along the curve in 3 dimensional space

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Homework Help Overview

The problem involves calculating the work done by a vector field along a parametrized curve in three-dimensional space. The vector field is given as ##\vec{F}(x,y,z)=(e^y+z^2\cos x,xe^y,2z\sin x)##, and the curve is parametrized by ##\vec{r(t)}=(\sin(3t),\cos(5+\sin(10t)),\sin(5+\sin(10t)))## for ##t\in [0, 2\pi]##.

Discussion Character

  • Exploratory, Assumption checking

Approaches and Questions Raised

  • Participants discuss whether the vector field is potential and explore the implications of the curve being closed or connected. There are attempts to verify the parametrization and its properties, including whether the endpoints match after one full traversal of the curve.

Discussion Status

Some participants have provided insights into the nature of the vector field and its potential, while others question the assumptions about the curve's connectivity and its implications for the work done. There is ongoing exploration of the relationship between the parametrization and the work calculation.

Contextual Notes

There is a mention of potential confusion regarding the parametrization of the curve and its implications for the work done. Participants are also considering the nature of the vector field and its exact differential properties.

brkomir
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Homework Statement


A vector field ##\vec{F}(x,y,z)=(e^y+z^2cosx,xe^y,2zsinx)## is given and a curve ##\Gamma## with parametrization ##\vec{r(t)}=(sin(3t),cost(5+sin(10t)),sint(5+sin(10t)))##. Calculate the work done along the curve ##\Gamma## for ##t\in \left [ 0,2\pi \right ]##

Homework Equations


The Attempt at a Solution



I first checked if ##\vec{F}## is potential:

##rot\vec{F}=\begin{pmatrix}
\frac{\partial }{\partial x} &\frac{\partial }{\partial y} & \frac{\partial }{\partial z}\\
e^y+z^2cosx& xe^y & 2zsinx
\end{pmatrix}=(0,2zcosx-2zcosx,e^y-e^y)=(0,0,0)##

So yes, ##\vec{F}## is potential!

Therefore the work done along the curve ##\Gamma## can be calculated ##\int \vec{F}d\vec{r}=\int grad(u)dr=u(b)-u(a)##

So I somehow have to get the equation of scalar field u...

Since we have a potential field I can say that ##u_x=e^y+z^2cosx##.

That gives me ##u=xe^y+z^2sinx +C(y,z)##

To determine ##C(y,z)## I derive the last equation: ##u_y=xe^y+C_y=xe^y##. The last equality comes from components of vector field ##\vec{F}##.

We can now see, that ##C(y,z)## is actually a function of z only! Let's check:

##u_z=2zsinx+C_z=2zsinx## now we can see that C is not a function of z either, there fore ##C=const## let's set C to 0.

Scala field is than given as ##u(x,y,z)=xe^y+z^2sinx## and the parametrization ##\vec{r(t)}=(sin(3t),cost(5+sin(10t)),sint(5+sin(10t)))## give us

##u(t)=sin(3t)e^{cost(5+sin(10t))}+sin^2(5+sin(10t))^2sin(sin(3t))## but because sin is a periodic function and equal to 0 for ##k2\pi ## where## k\in \mathbb{Z}## the final result is than also zero!
Which can only be explained IF the curve ##\Gamma## is connected.

Is everything written above ok? Is there a way I can check if ##\Gamma## is really connected?

I appreciate all the help!

Cheers
 
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brkomir said:
##\Gamma## with parametrization ##\vec{r(t)}=(sin(3t),cost(5+sin(10t)),sint(5+sin(10t)))##. Calculate the work done along the curve ##\Gamma## for ##t\in \left [ 0,2\pi \right ]##
the final result is than also zero!
Do you mean
##\vec{r(t)}=(\sin(3t),\cos (t(5+sin(10t))),\sin (t(5+sin(10t))))##?
If so, is it not clear that ##\vec{r(0)}=\vec{r(2\pi)}##?

Which can only be explained IF the curve ##\Gamma## is connected.
No. If ##\Gamma## is a closed loop then the work will be zero, but the work could happen to be zero even if ##\Gamma## is not a closed loop.
 
Try this: dr = (dx, dy, dz). Take the dot product F dot dr and see what you get. (It's going to be an exact differential).

Chet
 
haruspex said:
Do you mean
##\vec{r(t)}=(\sin(3t),\cos (t(5+sin(10t))),\sin (t(5+sin(10t))))##?
If so, is it not clear that ##\vec{r(0)}=\vec{r(2\pi)}##?No. If ##\Gamma## is a closed loop then the work will be zero, but the work could happen to be zero even if ##\Gamma## is not a closed loop.

No, the parametrization is ##\vec{r(t)}=(\sin(3t),(5+sin(10t))\cos t,(5+\sin (10t))\sin t)## .

Aha, ok, I forgot about that. So ##\Gamma## can be a closed loop or it can be anything else, but it just so happens that after ##2\pi## the function is at the same potential as in the beginning.

Chestermiller said:
Try this: dr = (dx, dy, dz). Take the dot product F dot dr and see what you get. (It's going to be an exact differential).

Chet

##\int \vec{F}d\vec{r}=\int (e^y+z^2\cos x)dx+\int xe^ydy+\int 2z\sin xdz=2xe^y+2z^2\sin x##

Sorry to ask you (i feel so stupid at the moment), but, why is this important?However, we all agree that work done along that curve is 0, right?
 
brkomir said:
##\int \vec{F}d\vec{r}=\int (e^y+z^2\cos x)dx+\int xe^ydy+\int 2z\sin xdz=2xe^y+2z^2\sin x##

Sorry to ask you (i feel so stupid at the moment), but, why is this important?


However, we all agree that work done along that curve is 0, right?
I didn't say to write it as an integral. I said to write it as
Fxdx+Fydy+Fzdz=(eydx+xeydy)+(z2cosxdx+2z sinx dz)=d(xey+z2sinx)
 
And because this is an exact differential, than F is potential?
 
brkomir said:
And because this is an exact differential, than F is potential?
Sure. More precisely, F is a force described by a potential.
 
Chestermiller said:
Sure. More precisely, F is a force described by a potential.
That's what brkomir showed in the first post.
 
brkomir said:
No, the parametrization is ##\vec{r(t)}=(\sin(3t),(5+sin(10t))\cos t,(5+\sin (10t))\sin t)## .
OK, but the question still applies: is it not clear that r(t+2π) = r(t)?
 

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