Calculator
Example data table
| i | x | sin(x) |
|---|---|---|
| 0 | 0.000000 | 0.000000 |
| 1 | 0.523599 | 0.500000 |
| 2 | 1.047198 | 0.866025 |
| 3 | 1.570796 | 1.000000 |
| 4 | 2.094395 | 0.866025 |
| 5 | 2.617994 | 0.500000 |
| 6 | 3.141593 | 0.000000 |
Formula used
How to use
- Pick Function of x or Tabulated data.
- For a function, enter f(x), bounds a, b, and intervals n.
- Choose one method or compare all methods.
- Press Calculate. Results appear above the form.
- Use Download CSV or Download PDF for reporting.
Integration in field and motion models
Numerical integration converts sampled forces, fields, and spectra into physically meaningful totals. For example, impulse equals ∫F(t)dt, charge equals ∫I(t)dt, and displacement equals ∫v(t)dt. With experimental sensors, values arrive as discrete points, so a stable rule is needed to approximate the area under the curve.
Choosing step size with measurable targets
The interval count n controls the step h=(b−a)/n. If the signal varies rapidly, smaller h captures curvature and reduces bias. A practical target is convergence: double n and watch the estimate change. When |I(2n)−I(n)| becomes small compared with your measurement uncertainty, refinement beyond that point adds little value. For many labs, keeping the relative change below 0.5% is a sensible threshold, especially when calibration drift or digitization noise dominates the uncertainty budget.
Trapezoidal rule for sampled measurements
The trapezoidal rule assumes the curve is linear between samples. For unequal spacing, it sums (xᵢ₊₁−xᵢ)(yᵢ+yᵢ₊₁)/2. It performs well for oscilloscope traces, calorimetry logs, and tabulated cross‑section data, and it remains robust when noise makes higher‑order curvature fitting unreliable.
Simpson’s rule for smooth analytical curves
Simpson’s 1/3 rule blends parabolic arcs across pairs of sub‑intervals, using endpoint and midpoint weighting. It typically achieves higher accuracy than trapezoids for smooth functions, such as Gaussian beam profiles or potential energy curves. Because it requires an even n, the calculator flags odd interval counts to prevent misuse.
Midpoint rule to reduce endpoint sensitivity
The midpoint rule samples each sub‑interval at its center. This can be advantageous when endpoints have discontinuities or when boundary values are uncertain. In physics, it can reduce sensitivity to singular behavior near a, such as 1/√x, by avoiding direct evaluation at the boundary while still representing the interior contribution.
Reporting results for reproducible analysis
Professional reporting should include the chosen method, bounds, n, and a trace of sampled points. Exporting a CSV supports lab notebooks and code review, while a PDF summary works for quick sharing. Comparing multiple methods helps detect instability: large divergence suggests insufficient resolution, sharp discontinuities, or an input expression that becomes non‑finite inside the range.