What you call the “First part” is usually called the second part. And it doesn’t state what you say. What is states is that if $f(t)$ is continuous on $[a,b]$, and we define the function $F(x)$ by the formula
$$F(x) = \int_a^x f(t)\,dt$$
then $F(x)$ is differentiable, and is in fact an antiderivative for $f$; that is, that
$$\frac{d}{dx} F(x) = \frac{d}{dx}\int_a^x f(t)\,dt = f(x).$$
That’s what that part states.
What you call the second part, which is usually called the first part, also doesn’t quite say what you are writing. What it says is that if $f(x)$ is continuous and $G(x)$ is any antiderivative for $f(x)$ on $[a,b]$, then
$$\int_a^b f(t)\,dt = G(b)-G(a).$$
Now, you could try to use the funtion $F(x)$ in your “first part”, but it doesn’t actually give you anything useful: it just says
$$\begin{align*}
\int_a^b f(t),dt &= F(b)-F(a)\\
&= \int_a^b f(t)\,dt - \int_a^a f(t)\,dt\\
&= \int_a^b f(t)\,dt
\end{align*}$$
which doesn’t really give you a way to compute the integral.
The “Second part” (usually called the First Part) says:
If you have an antiderivative of the continuous function $f(x)$, then you can use the antiderivative to calculate the integral $\int_a^b f(t)\,dt$
(though implicit is that you need to be able to compute values of the antiderivative independently of the integral...)
The “First part” (usually called the Second Part) says:
If $f(x)$ is continuous, then it definitely has (at least one) antiderivative.
This tells you that the first part is not an empty promise: if you can find a (useful, independently calculable) antiderivative, then you are set, and antiderivatives exist to be found. However, the antiderivative it shows you is not a useful antiderivative as far as the first part is concerned.