B Integration of a quantity when calculating Work

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While integrating work we write dw = INT. F.ds. But why can't we write dw = INT. dF.s ?
 
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The definition of work is ##work = force \times distance## and while the force can change over position and over time as we move along some path a distance s, we can generalize it as an integral over the path with ds being a very small distance to handle non-linear paths.

However dF isn't a force its a change in force and if used breaks the definition of work which is ##work = force \times distance## not ##work = change in force \times distance ##.

http://hyperphysics.phy-astr.gsu.edu/hbase/wint.html
 
First what do you mean by dF multiplied by s...give the physical interpretation...
 
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Isn't by definition ##\displaystyle w = \int_C f\cdot ds## ?
 
Yes, it is so...
 
Gurasees said:
While integrating work we write dw = INT. F.ds. But why can't we write dw = INT. dF.s ?
Check integration by parts. You will see that f.ds is not the same as df.s but there is a relation between them. That is math. then you will have to see if that has physical sense.
 
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Gurasees said:
While integrating work we write dw = INT. F.ds. But why can't we write dw = INT. dF.s ?
nasu said:
The same question was recently asked in the General Physics section.
https://www.physicsforums.com/threads/derivation-of-work-done.914895/
That thread was closed yesterday. Is this an attempt to re-open the same discussion?
Thread closed. @Gurasees, please take a look at the thread in the link that @nasu posted.
 
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