OK. You defined the function like this:
And you told me to find:
[itex]
\int_0^bf[/itex]
Now. If the function is continuous on interval [0,b] then it is integrable on [0,b].
But if function is bounded and have finitely many discontinuity on [0,b] it is still integrable.
So, we can find
[itex]
\int_0^bf[/itex]
Lets consider any partition on [0,b]. Then either [itex]x_{k}^{*}=0[/itex] or it does not.
If not then
[tex]\sum_{k=1}^{n}f(x_{k}^{*})\Delta x_{k} = \sum_{k=1}^{n}\Delta x_{k} = b[/tex]
else
[tex]\sum_{k=1}^{n}f(x_{k}^{*})\Delta x_{k} = -\Delta x_{k} + \sum_{k=1}^{n}\Delta x_{k} = b - \Delta x_{k}[/tex]
which means that the difference between the Riemann sum and b is at most [itex]\Delta x_{k}[/itex]. BUT, since [itex]\Delta x_{k}[/itex] approaches zero as [itex]max \Delta x_{k} \rightarrow 0[/itex] it follows that:
[tex]\int_{0}^{b}f(x)dx = b[/tex]
But the Fundamental Theorem of Calculus Part 2 states that "If f is continious on an interval [0,b] then f has an antiderivative on [0,b]. In particular if a is any number in [0,b] then the function F defined by:
[tex]F(x)=\int_{a}^{x}f(t)dt[/tex]
is an antiderivative of f on [0,b]; that is F'(x)=f(x) for each x in [0,b], or in an alternative notation:
[tex]\frac{d}{dx}\left [ \int_{a}^{x}f(t)dt \right ] = f(x)[/tex]
So f must be continious so that we can conclude that f has an antiderivative. If f is not continious anything can follow.