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If I have a function $f(t)$, and an indefinite integral of this function, $g(x) = int f(t), dt$, is there any way I can express $g(x)$ as a definite integral whose bounds depend on $x$?

I thought I saw somewhere that I could express it as
$$g(x) = int_a^x f(t), dt$$
but I don't know what $a$ is. Is this representation correct? Or is there a better way to express $g$?

That fixed but arbitrary lower limit is essentially the "arbitrary constant" you use when finding antiderivatives, because
$$
g(x) = int_a^x f(t), dt =
int_b^x f(t), dt +
int_a^b f(t), dt .
$$
The second term in that sum is just a number.

The fundamental theorem of calculus says that both integrals with upper limit $x$ have derivative $f$ with respect to $x$.

The "indefinite integral" with no limits specified refers to the whole set of antiderivatives, not any particular one of them.

Edit in response to comment.

A loose common way to describe the indefinite integral is to say
$$
int f(t), dt = F(x) + c
$$
for a function $F$ whose derivative is $f$ and any real number $c$. That's really a set of functions, one for each value of $c$.

In my answer you can take
$$
F(x) = int_b^x f(t), dt
quad text{ and } quad
c = int_a^b f(t), dt
$$
to get the $g(x)$ in the question.

No, not always.

In fact, the definite integral with variable bounds can be and is strictly more restrictive than the indefinite integral, in the most general case where both can be taken as sensibly existing to their fullest extent that we can say one defines the same kind of function as the other.

While it is true that if we have two functions $F_1$ and $F_2$ defined by definite integrals of the same function with different bounds, i.e.

$$F_1(x) := int_{a_1}^{x} f(t) dt mathrm{and} F_2(x) := int_{a_2}^{x} f(t) dt$$

with $a_1 ne a_2$, then we will have that $F_1 - F_2$ is a constant function, the range of possible such constants may be limited. A simple counterexample is to take $f(x) := sin(x)$. Now the integral from any lower bound $a$ to $x$ is just $int_a^x sin(t) dt = cos(a) - cos(x)$, but here $cos(a)$ - the "constant" of our integration - can only range in $[-1, 1]$ (and the difference of any two such "constants" only within $[-2, 2]$), but the constant in $int sin(x) dx = -cos(x) + C$ can be any real number whatsoever, even one far outside this range, say assign $C := mbox{Graham's number}$. Thus the integrals with variable bounds are not exhaustive of the full family of antiderivatives, which is what is represented by the indefinite integral, and if we are really pedantic should be truly written as the set it is: in "reality", not in the informalities of school calculus,

$$int f(x) dx = left{ F(x) + C : C in mathbb{R} right}$$

where $F'(x) = f(x)$. Actually, if we want to be really correct - and in fact this is important but only in cases where the definite integral technically doesn't make sense as evaluable between arbitrary pairs of points - we should take

$$int f(x) dx = left{ F(x) in mathbb{R}^mathbb{R} : mbox{$F'$ exists and $F'(x) = f(x)$} right}$$.