The differential element, \(ds\), is a small segment of the curve's length that plays a central role in evaluating line integrals. This concept breaks down the curve into infinitesimally small parts, making integration over the curve possible.
The expression for \(ds\) in terms of a parameter \(t\) is given by:
\(ds = ||\vec{r'}(t)|| \, dt\)
Here's how you compute and use \(ds\):
- Find the derivative \(\vec{r'}(t)\) of the parameterized path \(\vec{r}(t)\).
- Compute the magnitude \(||\vec{r'}(t)||\), which represents the instantaneous rate of change of the arc length with respect to \(t\).
- Multiply this magnitude by \(dt\), the differential change in \(t\), to get \(ds\).
Once \(ds\) is effective expressed, it allows us to integrate a function \(f\) over the path \(C\) as: \[ \int_{C} f \, ds = \int_{a}^{b} f(\vec{r}(t)) ||\vec{r'}(t)|| \, dt \] This approach simplifies the integral from one over a complicated path \(C\) to an integral over a simple interval \([a, b]\).