User`s guide
3 Fitting Data
3-4
Parametric Fitting
Parametric fitting involves finding coefficients (parameters) for one or more
models that you fit to data. The data is assumed to be statistical in nature and
is divided into two components: a deterministic component and a random
component.
data = deterministic component + random component
The deterministic component is given by the fit and the random component is
often described as error associated with the data.
data = fit + error
The fit is given by a model that is a function of the independent (predictor)
variable and one or more coefficients. The error represents random variations
in the data that follow a specific probability distribution (usually Gaussian).
The variations can come from many different sources, but are always present
at some level when you are dealing with measured data. Systematic variations
can also exist, but they can be difficult to quantify.
The fitted coefficients often have physical significance. For example, suppose
you have collected data that corresponds to a single decay mode of a radioactive
nuclide, and you want to find the half-life (T
1/2
) of the decay. The law of
radioactive decay states that the activity of a radioactive substance decays
exponentially in time. Therefore, the model to use in the fit is given by
where y
0
is the number of nuclei at time t = 0, and λ is the decay constant.
Therefore, the data can be described by
Both y
0
and λ are coefficients determined by the fit. Because T
1/2
= ln(2)/λ, the
fitted value of the decay constant yields the half-life. However, because the
data contains some error, the deterministic component of the equation cannot
completely describe the variability in the data. Therefore, the coefficients and
half-life calculation will have some uncertainty associated with them. If the
uncertainty is acceptable, then you are done fitting the data. If the uncertainty
is not acceptable, then you might have to take steps to reduce the error and
repeat the data collection process.
yy
0
e
λt–
=
data y
0
e
λt–
error+=