A (negative) exponential law takes the form $y=-\exp(-x)$. When you allow for changes of units in the $x$ and $y$ values, though, say to $y = \alpha y' + \beta$ and $x = \gamma x' + \delta$, then the law will be expressed as
$$\alpha y' + \beta = y = -\exp(-x) = -\exp(-\gamma x' - \delta),$$
which algebraically is equivalent to
$$y' = \frac{-1}{\alpha} \exp(-\gamma x' - \delta) - \beta = a\left(1 - u\exp(-b x')\right)$$
using three parameters $a = -\beta/\alpha$, $u = 1/(\beta\exp(\delta))$, and $b = \gamma$. We can recognize $a$ as a scale parameter for $y$, $b$ as a scale parameter for $x$, and $u$ as deriving from a location parameter for $x$.
As a rule of thumb, these parameters can be identified at a glance from the plot:
The parameter $a$ is the value of the horizontal asymptote, a little less than $2000$.
The parameter $u$ is the relative amount the curve rises from the origin to its horizontal asymptote. Here, the the rise therefore is a little less than $2000 - 937$; relatively, that's about $0.55$ of the asymptote.
Because $\exp(-3) \approx 0.05$, when $x$ equals three times the value of $1/b$ the curve should have risen to about $1-0.05$ or $95\%$ of its total. $95\%$ of the rise from $937$ to almost $2000$ places us around $1950$; scanning across the plot indicates this took $20$ to $25$ days. Let's call it $24$ for simplicity, whence $b \approx 3/24 = 0.125$. (This $95\%$ method to eyeball an exponential scale is standard in some fields that use exponential plots a lot.)
Let's see what this looks like:
plot(Days, Emissions)
curve((y = 2000 * (1 - 0.56 * exp(-0.125*x))), add = T)

Not bad for a start! (Even despite typing 0.56
in place of 0.55
, which was a crude approximation anyway.) We can polish it with nls
:
fit <- nls(Emissions ~ a * (1- u * exp(-b*Days)), start=list(a=2000, b=1/8, u=0.55))
beta <- coefficients(fit)
plot(Days, Emissions)
curve((y = beta["a"] * (1 - beta["u"] * exp(-beta["b"]*x))), add = T, col="Green", lwd=2)

The output of nls
contains extensive information about parameter uncertainty. E.g., a simple summary
provides standard errors of estimates:
> summary(fit)
Parameters:
Estimate Std. Error t value Pr(>|t|)
a 1.969e+03 1.317e+01 149.51 2.54e-10 ***
b 1.603e-01 1.022e-02 15.69 1.91e-05 ***
u 6.091e-01 1.613e-02 37.75 2.46e-07 ***
We can read and work with the entire covariance matrix of the estimates, which is useful for estimating simultaneous confidence intervals (at least for large datasets):
> vcov(fit)
a b u
a 173.38613624 -8.720531e-02 -2.602935e-02
b -0.08720531 1.044004e-04 9.442374e-05
u -0.02602935 9.442374e-05 2.603217e-04
nls
supports profile plots for the parameters, giving more detailed information about their uncertainty:
> plot(profile(fit))
Here is one of the three output plots showing variation in $a$:

E.g., a t-value of $2$ corresponds roughly to a 95% two-sided confidence interval; this plot places its endpoints around $1945$ and $1995$.
fit <- nls(Emissions ~ a* (1- u*exp(-b*Days)), start = list(a = 2000, b = 0.1, u=.5)); beta <- coefficients(fit); curve((y = beta["a"] * (1 - beta["u"] * exp(-beta["b"]*x))), add = T)
. $\endgroup$