If f is differentiable, is f ' continuous?

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The discussion centers around whether the derivative of a differentiable function is continuous. It is established that if a function is differentiable at a point, it must be continuous at that point. However, the derivative itself may not be continuous even if the function is differentiable everywhere. Examples like f(x) = x^2 sin(1/x) illustrate that while the derivative exists, it can be discontinuous at certain points. Ultimately, the derivative must satisfy the intermediate value property, meaning it can only be discontinuous if the one-sided limits do not exist.
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So, a certain discussion occurred in class today...

If f is differentiable, is f ' continuous?

At first sight, there seems no reason to think so. However, we couldn't think any counterexample. It also seems logical that f' is continuous since otherwise f wouldn't be differentiable.

For example, suppose f(x) = ln x, for x > 0

Then f'(x) = 1/x. Yes, this is discontinuous, but it's not for the domain x > 0.

So, the question remains:

If f is differentiable, is f ' continuous?
 
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x2sin(1/x) if x is not zero
0 if x is zero
 


^Haha, yes, I was just talking about that with a friend.

You mean, f(x) = x2 sin(1/x) for x =/= 0, 0 otherwise, right?

EDIT:

However, wouldn't that make f not differentiable since it's not differentiable at x = 0?

For example, f(x) = l x l , it's not differentiable at x = 0, thus we deem it "not differentiable". Wouldn't the same apply here?

EDIT #2: Nevermind, just an error. Alright. I think I got it for sure now! Haha.
 
Last edited:


If a function is differentiable at a point, it is necessarily continuous at this point. To see this, recall the definition of a limit:

lim h->0 f(x+h) - f(x) / h

Since it presumably exists, and the denominator goes to 0, lim h->0 f(x+h) - f(x) = 0. From this, it's clear the function is continuous at x.

So if a function is differentiable (everywhere), it's continuous.
 


Werg22 said:
So if a function is differentiable (everywhere), it's continuous.

Remember though, that although the above is true, "if a function is continuous, then it is differentiable" is not necessarily true. Consider y = |x| at x = 0.
 


Werg22 said:
If a function is differentiable at a point, it is necessarily continuous at this point. To see this, recall the definition of a limit:

lim h->0 f(x+h) - f(x) / h

Since it presumably exists, and the denominator goes to 0, lim h->0 f(x+h) - f(x) = 0. From this, it's clear the function is continuous at x.

So if a function is differentiable (everywhere), it's continuous.
That is true but was not the original question. The question was, if a function is differentiable at x= a is the derivative continuous there.

Office Shredder's answer was "no, the derivative is not necessarily continuous".

And, l'Hopital, it is not the same situation as |x|.

The difference quotient, at x= 0, is
\frac{h^2 sin(1/h)}{h}= h sin(1/h)
for h\ne 0 and that goes to 0 as h goes to 0. Unlike |x|, the derivative at x=0 does exist and is 0.

That derivative is not continuous at x=0 because, for x\ne 0, the derivative is 2xcos(1/x)+ sin(1/x) and that has no limit as x goes to 0.

It is, however, true that the derivative must satisfy the "intermediate value property". That is, if f' exists on [a, b], then it must take all values between f'(a) and f'(b). That means, in particular, that if the two one sided limits, \lim_{x\to a^+}f'(x) and \lim_{x\to a^-}f'(x), exist, they must be equal and equal to the value of the derivative at a (in which case, f' is continuous there. The only way a derivative can exist at a point and not be continuous there is if the two one sided limits themselves do not exist, as in Office Shredder's example.
 
Relativistic Momentum, Mass, and Energy Momentum and mass (...), the classic equations for conserving momentum and energy are not adequate for the analysis of high-speed collisions. (...) The momentum of a particle moving with velocity ##v## is given by $$p=\cfrac{mv}{\sqrt{1-(v^2/c^2)}}\qquad{R-10}$$ ENERGY In relativistic mechanics, as in classic mechanics, the net force on a particle is equal to the time rate of change of the momentum of the particle. Considering one-dimensional...

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