Nice observation by @jasnyder610.
On the last line, the most general form of the RHS is actually (f⋅g)' = 𝑐⋅(f'g + g'f), for some constant 𝑐.
We can solve for 𝑐 by setting g(x) = 1, and we then see that we must have that 𝑐=1.
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This is really neat. When I see things like this, it makes me a little sad that by plunging myself deep down the mathematical rabbit hole, I seem to have let my basic physical intuition atrophy to the point that I forget to connect things back to reality.
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Thanks! it's how I think of things as a physicist.. we need all the cross checks we can get given how sloppy we are ;)
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Neat! I like it. There's also the matter of an overall scale factor, which you can see has to be 1 by (for example) setting g(x) = 1
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Ah good point!
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Do you have any other intuitive explanations of the product rule? Particularly in the complex case. This visualization explains very neatly the real case, but I've yet to see a good visual for the complex case.pic.twitter.com/ynOO1PyWd3
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this is cool! did you make it?
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I posed the problem of finding functions f,g satisfying the wrong product rule. (Also in relation to convolution, for what it's worth!)
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Nice, but it still doesn't help me memorizing the *quotient* rule.
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Yes but it's interesting to note that perhaps the lack of symmetry in the quotient rule is why it's more complicated
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