Derivative of a symetrical function

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If a function f(x) is symmetrical (even), then all odd derivatives of f vanish at x, meaning f^{(n)}(x) = 0 for n=1,3,5,... This can be proven by examining the Taylor expansion, where odd power terms disappear if the function is C^{\infty}. The discussion also highlights that odd derivatives of even functions result in odd functions, which have specific properties, such as f(0) = 0. Additionally, the concept of rotational symmetry is clarified, explaining that rotating the graph of an odd function 180 degrees about the origin yields the same graph. Understanding these properties is essential for analyzing symmetrical functions in calculus.
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If f(x) is symetrical, then

f^{(n)}(x) =0, \ \ \ n=1,3,5,...

What would be a proof of that?
 
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ummm, no that doesn't make sense, does it. How about

If f(x) is symetrical and C^{\infty}, then the terms of odd powers in the Taylor expansion vanish.

What would be a proof of that?
 
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Suppose that the coefficients of the odd terms are not all zero. Look at f(-x) and use the fact that (convergent) Taylor series are equal in an interval iff the coefficients are equal.
 
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Great, thank you Data.
 
So you meant "even" instead of "symmetric"...The function is "even",its graph is "symmetric" wrt the vertically chosen Oy axis...:wink:

Daniel.
 
One can also show that any odd derivative (1, 3, 5, etc.) of an even function is an odd function. Of course, for any odd function, f, f(0)= 0.
 
And odd functions are also symmetric, rotationally,
 
Yeah, what does rotational symmetry, or symmetry about the origin mean again? Thinking of graphs of odd functions I can remember (e.g. y = x3), the only thing I can think of is that it means rotating the graph of the function 180o about the origin, gives an image the same as the original.
 

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