Interpreting the L2 Norm of Force on a Path

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maze
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The path integral of force is the work, something that has a clear physical meaning we can relate to. My question is, what is the physical interpretation for the L2 norm of the force along a path? (integral of the force squared, basically):

[tex]\left(\int_\Gamma F \cdot F \right)^{\frac{1}{2}}[/tex]

If a particle takes the path from point A to B which minimizes the work, then the least amount of external energy was expended moving it from point A to B. Can we analogously characterize the type of paths between 2 points that minimize the L2 norm of the force.

Thanks!
 
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maze said:
The path integral of force is the work, something that has a clear physical meaning we can relate to. My question is, what is the physical interpretation for the L2 norm of the force along a path? (integral of the force squared, basically):

[tex]\left(\int_\Gamma F \cdot F \right)^{\frac{1}{2}}[/tex]

Do you mean:

[tex]\left(\int_\Gamma (\mathbf{F} \cdot \mathbf{F})ds \right)^{\frac{1}{2}}[/tex]

?
 
Yes, of course. F:R3->R3, [itex]\Gamma:[0,1]->\textbf{R}^3[/itex]