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has a bounded derivative discontinuous at that is nevertheless Riemann integrable, and Newton–Leibniz evaluates its integral
Example
Define by
Then is differentiable on , with
The derivative is bounded and is continuous except at , but it is not continuous at . Consequently is Riemann integrable and
Moreover, arbitrarily near the derivative takes the values and up to terms tending to : at and , and for every integer .
Facts & Assumptions
Given: The function above.
Sine and cosine are differentiable with derivatives cosine and negative sine; the chain and product rules apply (The derivatives of sine and cosine are cosine and minus sine, The chain rule, in one line from Carathéodory: if is differentiable at and is differentiable at , then is differentiable at with , Sums, scalar multiples, products and quotients: , , , and when ).
and for every real (Parity and the Pythagorean identity for sine and cosine).
The number is positive, and shifts by alternate the signs of sine and cosine (Pi as twice the smallest positive zero of cosine, Quarter-turn values and shifts by pi/2 and pi).
Reciprocals of positive natural numbers tend to zero (For every in a complete ordered field there is a natural with ).
A bounded function with an at-most-countable discontinuity set is Riemann integrable (A bounded function on whose set of discontinuities is at most countable is Riemann integrable).
Newton--Leibniz holds for a continuous function with an interior derivative having an integrable extension (Newton–Leibniz needs only continuity on , differentiability on , and a Riemann-integrable extension of the interior derivative).
Verification
Since , the quotient has absolute value at most and tends to ; hence .
For , [L1] gives .
By [L2], on , so is bounded. The displayed formula is continuous away from .
By [L3], sine vanishes and cosine equals at , while sine vanishes and cosine equals at ; substituting gives and . Both sequences tend to by [L4], so is discontinuous there.
Thus the discontinuity set is exactly , and [L5] makes Riemann integrable.
Applying [L6] to and yields .
Depends on
- Newton–Leibniz needs only continuity on $[a,b]$, differentiability on $(a,b)$, and a Riemann-integrable extension of the interior derivative
- A bounded function on $[a,b]$ whose set of discontinuities is at most countable is Riemann integrable
- Sums, scalar multiples, products and quotients: $(f+g)'(c) = f'(c) + g'(c)$, $(\alpha f)'(c) = \alpha f'(c)$, $(fg)'(c) = f'(c)g(c) + f(c)g'(c)$, and $(f/g)'(c) = \bigl(f'(c)g(c) - f(c)g'(c)\bigr)/g(c)^{2}$ when $g(c) \ne 0$
- The chain rule, in one line from Carathéodory: if $g$ is differentiable at $c$ and $f$ is differentiable at $g(c)$, then $f \circ g$ is differentiable at $c$ with $(f \circ g)'(c) = f'(g(c))\,g'(c)$
- The derivatives of sine and cosine are cosine and minus sine
- Parity and the Pythagorean identity for sine and cosine
- Pi as twice the smallest positive zero of cosine
- Quarter-turn values and shifts by pi/2 and pi
- For every $\varepsilon > 0$ in a complete ordered field there is a natural $n \ge 1$ with $1/n < \varepsilon$
Used by
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Sources
- J. K. Hunter, An Introduction to Real Analysis, Example 12.2 (standard reference, not scraped)