Why do we need to imagine a varied path in the calculus of variations?

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SUMMARY

The discussion centers on the necessity of imagining varied paths in the calculus of variations to determine the shortest path between two points. The process involves differentiating the action with respect to paths, similar to differentiating a function of one variable. By considering nearby paths, one can identify where the derivative equals zero, indicating a minimum length. This method is essential for finding the correct path that minimizes the action integral, analogous to finding extrema in single-variable functions.

PREREQUISITES
  • Understanding of calculus, specifically differentiation
  • Familiarity with the concept of action integrals
  • Knowledge of the calculus of variations
  • Basic grasp of parametric equations and path parametrization
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  • Explore methods for parametrizing paths in mathematical analysis
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This discussion is beneficial for students and professionals in mathematics, physics, and engineering, particularly those interested in optimization problems and the calculus of variations.

NihalRi
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I'm very new to this. So in the context of finding the shortest path the idea is that you imagine another path that starts and ends at the same point. The shortest path is a minima so you differentiate and find for what values the differential is zero.
I don't understand why we need to imagine this varied path, why not differentiate the original path?
 
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Actually we're differentiating the action w.r.t. to paths. Its pretty much like differentiating a function of one variable. The definition is ## \displaystyle f'(x)=\lim_{\delta\to 0}\frac{f(x+\delta)-f(x)}{\delta} ##. The analogue of your question about the derivative of a function of one variable is that why are we considering ## f(x+\delta) ##? Why not only ##f(x)## appears in the definition?
The answer in both cases is that we need to find out in what point the derivative is equal to zero to lowest order, which means the function doesn't change when we move only a little bit. You just need to recognize that an action integral is a function of paths between two given endpoints so when we want to calculate its derivative, we have to consider two nearby paths between those two endpoints(like ##x+\delta## and ##x## above) and calculate the output of the action integral for both and demand that the difference vanishes to lowest order. This way we find out at what path this happens and that'll be the correct path. This is pretty much like setting the first derivative of a function of one variable to zero to find in what ##x##s the function has extrema.
 
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The IDEA is the following: you start with a family of continuous paths from the initial point ##A## to the final point ##B##, you can parametrize this family by a parameter ##t## so for each ##t## you have a path between ##A## and ##B##, and the corresponding length of the path from ##A## and ##B##. So you have a function ##\mathcal{L}(t)## that for each path ##t## give you the length. You minimize the quantity ##\mathcal{L}(t)## studying the derivative and you will find the minimum length, so the minimum path ...
 
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Relativistic Momentum, Mass, and Energy Momentum and mass (...), the classic equations for conserving momentum and energy are not adequate for the analysis of high-speed collisions. (...) The momentum of a particle moving with velocity ##v## is given by $$p=\cfrac{mv}{\sqrt{1-(v^2/c^2)}}\qquad{R-10}$$ ENERGY In relativistic mechanics, as in classic mechanics, the net force on a particle is equal to the time rate of change of the momentum of the particle. Considering one-dimensional...

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