Physical significance of integral of F cross dr

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SUMMARY

The integral of the form ##\int \vec F \times d\vec r## does not represent torque, as clarified in the discussion. Instead, torque is defined by the equation ##\vec \tau = -\int \vec F \times \vec r dV##, which involves a volume integral rather than a line integral. The cross-product is a crucial mathematical tool in mechanics, with applications in calculating torque and angular momentum. The discussion emphasizes the distinction between infinitesimal changes in position and the overall position vector in the context of these integrals.

PREREQUISITES
  • Understanding of vector calculus, specifically line integrals and cross-products.
  • Familiarity with Newtonian mechanics concepts such as torque and angular momentum.
  • Knowledge of the Biot-Savart Law and its applications in physics.
  • Basic grasp of volume integrals and their significance in mechanics.
NEXT STEPS
  • Study the derivation and applications of the Biot-Savart Law in electromagnetism.
  • Explore the mathematical foundations of torque using volume integrals in mechanics.
  • Learn about the physical significance of the cross-product in various mechanical systems.
  • Investigate practical examples of torque calculations in real-world engineering problems.
USEFUL FOR

Physics students, mechanical engineers, and anyone interested in the applications of vector calculus in mechanics will benefit from this discussion.

arpon
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In the vector calculus course, I calculated integrals like,
##\int \vec F \times \vec{dr} ##
Does this kind of integrals have physical significance or practical application other than Biot-Savart's Law?
 
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In Newtonian mechanics the integral represents torque or rate of change of angular momentum.

The cross-product as a mathematical tool was invented probably because of its practical application. Although its development as a mathematical tool was post-Newton, it is very useful in mechancs.

AM
 
Andrew Mason said:
In Newtonian mechanics the integral represents torque or rate of change of angular momentum.

The cross-product as a mathematical tool was invented probably because of its practical application. Although its development as a mathematical tool was post-Newton, it is very useful in mechancs.

AM
Isn't torque defined as ##\vec r \times \vec F## ?
 
arpon said:
Isn't torque defined as ##\vec r \times \vec F## ?

##\vec r \times \vec F = - \vec F \times \vec r##
 
Yes. That is just a convention. The difference is the sign or direction of the torque vector.

AM
 
PeroK said:
##\vec r \times \vec F = - \vec F \times \vec r##
That was not my point. ##d \vec r## represents infinitesimal change in position vector, while ##\vec r## represents position vector. Could you please give me a practical example where the net torque is calculated by ##\int \vec F \times d \vec r## ?
 
arpon said:
That was not my point. ##d \vec r## represents infinitesimal change in position vector, while ##\vec r## represents position vector. Could you please give me a practical example where the net torque is calculated by ##\int \vec F \times d \vec r## ?

The line integral doesn't represent the torque on a body. The total torque on a body would be a volume integral:

##\vec{\tau} = -\int \vec F \times \vec r dV##

I'm not sure when you would use the line integral.
 
arpon said:
That was not my point. ##d \vec r## represents infinitesimal change in position vector, while ##\vec r## represents position vector. Could you please give me a practical example where the net torque is calculated by ##\int \vec F \times d \vec r## ?
I see your point. PeroK is quite right that ##\int \vec F \times d \vec r## does not represent torque. I am not sure what it would represent. I also don't see how it applies even to the Biot-Savart Law.

AM
 

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