Fundamental Theorem of Line Integral question

In summary, the question is asking to find the work done by an inverse square force field in moving an object from one point to another along a path, given the distances of these points from the origin. The field is conservative, meaning the work is path-independent and only depends on the distances from the origin. To solve this problem, one must prove the field is conservative and then use the argument that the work is only dependent on the distances from the origin to find the total work done.
  • #1
nfljets
3
0
The question is suppose that F is an inverse square force field, that is,

F(r)=cr/|r^3|

where c is some constant. r = xi + yj + zk. Find the work done by F in moving an object from a point P1 along a path to a point P2 in terms of the distances d1 and d2 from those points to the origin.

I'm not exactly sure how to do this or even where to start?

Usually F denotes a vector field, but in case it doesn't...?

Any help would be greatly appreciated!
 
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  • #2
nfljets said:
The question is suppose that F is an inverse square force field, that is,

F(r)=cr/|r^3|

where c is some constant. r = xi + yj + zk. Find the work done by F in moving an object from a point P1 along a path to a point P2 in terms of the distances d1 and d2 from those points to the origin.

I'm not exactly sure how to do this or even where to start?

Usually F denotes a vector field, but in case it doesn't...?

Your || signs should be around just the r, but Why do you say it isn't a vector field? You are given r = <x, y, z> and

[tex]\vec F = \frac {c}{|\vec r|^3}\ \vec r =
\langle \frac{cx}{(x^2+y^2+z^2)^{\frac 3 2}},\frac{cy}{(x^2+y^2+z^2)^{\frac 3 2}},\frac{cz}{(x^2+y^2+z^2)^{\frac 3 2}}\rangle[/tex]

What does the fund. theroem of line integrals have to say about this?
 
  • #3
I am a bit rusty on vector fields, but I bielive the situation is as follows:
(1) Notice that in every point r=(x,y,z) in space the field F(r) is a vector along the ray coming from the center of coordinate through this point. So you can picture the entire field like a blast from singe central point 0.
(1) Think of two points A, B located at the same distance from 0 - that is, on a sphere with radius |A| - and a path, also on this sphere, connecting them. To move a particle along this path would cost you no energy since you are always orthogonal to force direction.

(2) Conclude that for all it matters, the points P1 and P2 can be located on the same ray coming from the origin (while preserving only their distances from it), and the work accounted for is the work along the path from distance |P2| to distance |P1| along this ray.

To do this formally, look for the term "conservative field", for which the work between two points is path-independent. Prove that your field is conservative, and apply the argument above.
 
  • #4
jshtok said:
I am a bit rusty on vector fields, but I bielive the situation is as follows:
(1) Notice that in every point r=(x,y,z) in space the field F(r) is a vector along the ray coming from the center of coordinate through this point. So you can picture the entire field like a blast from singe central point 0.
(1) Think of two points A, B located at the same distance from 0 - that is, on a sphere with radius |A| - and a path, also on this sphere, connecting them. To move a particle along this path would cost you no energy since you are always orthogonal to force direction.

(2) Conclude that for all it matters, the points P1 and P2 can be located on the same ray coming from the origin (while preserving only their distances from it), and the work accounted for is the work along the path from distance |P2| to distance |P1| along this ray.

To do this formally, look for the term "conservative field", for which the work between two points is path-independent. Prove that your field is conservative, and apply the argument above.

So, what's your question? He has given you intuitive reasoning and told you what to do.
 

Related to Fundamental Theorem of Line Integral question

1. What is the Fundamental Theorem of Line Integrals?

The Fundamental Theorem of Line Integrals is a mathematical theorem that relates a line integral along a path to a double integral over a region bounded by that path. It states that if a function F is continuous on a simple, closed curve C and has an anti-derivative f, then the line integral of F along C is equal to the difference of f evaluated at the endpoints of C.

2. How is the Fundamental Theorem of Line Integrals used in mathematics?

The Fundamental Theorem of Line Integrals is used in various fields of mathematics, such as vector calculus, differential equations, and physics. It allows for the evaluation of line integrals using anti-derivatives, making calculations simpler and more efficient. It also has applications in the calculation of work, flux, and circulation.

3. What is the difference between the Fundamental Theorem of Line Integrals and the Fundamental Theorem of Calculus?

The Fundamental Theorem of Line Integrals and the Fundamental Theorem of Calculus are both fundamental theorems in calculus, but they apply to different types of integrals. The Fundamental Theorem of Calculus relates a definite integral to an anti-derivative of its integrand, while the Fundamental Theorem of Line Integrals relates a line integral to a double integral over a region.

4. Can the Fundamental Theorem of Line Integrals be extended to higher dimensions?

Yes, the Fundamental Theorem of Line Integrals can be extended to higher dimensions. In three dimensions, it becomes the Fundamental Theorem of Surface Integrals, and in even higher dimensions, it becomes the Fundamental Theorem of Volume Integrals. These theorems continue to relate higher-dimensional integrals to lower-dimensional integrals over a region.

5. Are there any limitations to the Fundamental Theorem of Line Integrals?

One limitation of the Fundamental Theorem of Line Integrals is that it only applies to simple, closed curves. It cannot be used for non-simple curves, such as self-intersecting curves. Additionally, the function F must be continuous on the curve C for the theorem to hold. If F is discontinuous at any point on C, the theorem does not apply.

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