I have trouble understanding the definition of a line integral over $\mathbb C$. If we take a line $\gamma$ that is $C^{1}$ or $C^1$ by pieces included in an open and connex set $\Omega$ for instance, the textbook definition of the integral of a continuous complex function function is that by taking a $C^1$ parametrisation of $\gamma$, let's call it $z : [a,b]\rightarrow \mathbb \gamma$ then we have
$$\int_{\gamma}f(z)dz=\int_{a}^{b} f(z(t))z'(t)dt$$.
Now i understand that if we take another equivalent parametrisation of $\gamma$ (that is to say $y:[c,d]\rightarrow \gamma$ such that a bijective, orientation-preserving function $t$ exists such that $z(t(s))=y(s)$ and $t'>0$) then $$\int_{\gamma}f(z)dz=\int_{c}^{d} f(y(t))y('t)dt$$.
However i have don't see why by taking another parametrisation $w$ of $\gamma$ that is non equivalent to $z$ we can't end up with another value of $$\int_{\gamma}f(z)dz$$. I have tried to prove that two $C^1$ parametrisations of same orientation of the same line $\gamma$ are equivalent to no avail. Thanks in advance for your help.