First of all, Welcome to the site !
As Ross Millikan answered, taking the logarithm of the $y$'s is a solution. In fact, it almost corresponds to the minimization of the sum of squares of relative errors.
If you do it, the residual is
$$r_i=\log(y_i^{calc})-\log(y_i^{exp})=\log\left(\frac{y_i^{calc}} {y_i^{exp} } \right)=\log\left(1+\frac{y_i^{calc}-y_i^{exp}} {y_i^{exp} } \right)$$ and, if the error is small, by Taylor,
$$r_i \approx \frac{y_i^{calc}-y_i^{exp}} {y_i^{exp} }$$
This is a typical problem in some areas; for example, the vapor pressure of any molecule is always represented as $\log(P)=f(T)$ and the fit is done that way.
Edit
For illustration purposes, let us consider the vapor pressure of water (values taken here). Units being Kelvin and Pascal, the data are
$$\left(
\begin{array}{cc}
T & P \\
212.45 & 1 \\
230.95 & 10 \\
252.85 & 100 \\
280.15 & 1000 \\
318.95 & 10000 \\
372.75 & 100000
\end{array}
\right)$$ and Antoine's very simplistic model is
$$P=\exp\left(a+ \frac b {T+c} \right)$$ The fit does not present any difficulties but let us look at the predicted values
$$\left(
\begin{array}{ccc}
T & P_{exp} & P_{calc} \\
212.45 & 1 & 1.40872 \\
230.95 & 10 & 13.5177 \\
252.85 & 100 & 117.420 \\
280.15 & 1000 & 993.933 \\
318.95 & 10000 & 10000.6 \\
372.75 & 100000 & 100000.
\end{array}
\right)$$ showing the same problem as in your case (very large relative errors at low temperature.
Let us repeat the problem with the logarithmic transform
$$\log(P)=a+ \frac b {T+c}$$ and repeat the calculations
$$\left(
\begin{array}{ccc}
T & P_{exp} & P_{calc} \\
212.45 & 1 & 0.96378 \\
230.95 & 10 & 10.6333 \\
252.85 & 100 & 102.584 \\
280.15 & 1000 & 937.705 \\
318.95 & 10000 & 9954.24 \\
372.75 & 100000 & 101906.
\end{array}
\right)$$
Finally, using the nonlinear model but minimizing the sum of the squares of relative errors
$$\left(
\begin{array}{ccc}
T & P_{exp} & P_{calc} \\
212.45 & 1 & 0.96119 \\
230.95 & 10 & 10.5950 \\
252.85 & 100 & 102.199 \\
280.15 & 1000 & 934.653 \\
318.95 & 10000 & 9934.34 \\
372.75 & 100000 & 101902.
\end{array}
\right)$$
As you can see, the second and third steps lead to very similar results.