Maths and data tools
A graphing calculator, derivatives with steps, Riemann sums, Fourier series and the unit circle, plus regression, chi-square and error propagation tools.
21 tools
The calculus tools show their working. The derivative calculator names every rule it applies, the tangent explorer traces a gradient along a curve until the derivative appears beneath it, and the Riemann sum explorer draws left, right, midpoint, trapezoid and Simpson strips closing in on an integral. The Fourier series visualiser builds square, sawtooth and triangle waves out of sine waves and shows the overshoot at a jump that no number of terms removes, and the unit circle explorer puts one movable point where the sine, the cosine and the tangent are all read off the same construction rather than memorised as three separate tables.
A measurement without an uncertainty is not a result, it is a number. The data tools handle the part of lab work that turns raw readings into something defensible: how uncertainties combine, how far a value sits from the accepted one, how much of the scatter in a data set is real, and, where two quantities were measured against each other, what the best straight line through them is and how well the slope itself is pinned down.
The distinction that runs through all of it is between accuracy and precision. They are independent, they fail for different reasons, and they are fixed by different actions.
The arithmetic is short. The judgement is in deciding which uncertainty dominates, which operation you are propagating through, and how many digits you are entitled to keep. A mean quoted to seven figures from readings taken off a ruler is a claim nobody can defend.
Simulators
Calculators
Visualisers and reference
Accuracy and precision fail differently
Precision is how tightly repeated readings cluster. Poor precision is random error, and it averages down: take more measurements and the mean tightens as the square root of the count. Accuracy is how close the result sits to the true value. Poor accuracy is systematic error, and averaging does nothing at all. A balance reading half a gram heavy reads half a gram heavy however many times you use it.
This is why the sign of an error is worth looking at before you discard it. Readings scattered either side of the accepted value point to noise you can average away. Readings consistently on one side point to a calibration problem, and no amount of repetition will help.
That square root also sets what more data is worth. Halving the standard error of the mean takes four times as many measurements, and quartering it sixteen times as many. Somewhere on that curve the random component drops below the systematic one, and past that point more repetition buys nothing.
Combine uncertainties in quadrature
For independent random uncertainties, the combined uncertainty is the square root of the sum of the squares, not the plain sum. Adding linearly assumes every error conspires in the same direction at the same moment, which overstates the true uncertainty. Add linearly only for correlated or systematic effects, where they genuinely do move together.
One consequence is worth internalising: quadrature is dominated by the largest term. Take uncertainties of 1 and 3 in the same units, combining to about 3.16. Eliminating the smaller one entirely gets you to 3.00, an improvement of 5 percent. Halving the larger one gets you to 1.80, an improvement of 43 percent. Spend the effort on the dominant term.
Absolute or relative depends on the operation
For sums and differences, absolute uncertainties combine in quadrature. For products, quotients and powers it is the relative uncertainties that combine, and a power multiplies the relative uncertainty by its exponent. That last rule bites: a 1 percent uncertainty in the radius of a sphere becomes 3 percent in its volume, because the radius is cubed.
The dangerous case is subtracting two similar numbers, because the absolute uncertainty survives while the result shrinks. Two masses of 15.2 g and 14.8 g, each good to 0.1 g, are individually known to better than 0.7 percent. Their difference is 0.4 g with a combined uncertainty of about 0.14 g, which is 35 percent. Nothing went wrong in the measurement. The precision was destroyed by the subtraction.
Weighing by difference is how this shows up at the bench, and the fix is to make the difference large relative to the reading error rather than to buy a better balance. The same reasoning explains why percent error needs a non-zero accepted value: dividing by something near zero inflates the percentage without adding information.
How many digits you are entitled to
Quote the uncertainty to one significant figure, or two when the leading digit is 1, then round the value to the same decimal place. Reporting 4.28371 ± 0.05 is wrong; 4.28 ± 0.05 is right. The extra digits are not more information, they are a claim the uncertainty figure contradicts.
Significant figures are a crude stand-in for a stated uncertainty. Writing 1.0 rather than 1.00 does convey something about precision, but it cannot express an uncertainty that is not a power of ten. Where it matters, state the uncertainty and say whether it is a standard deviation, a standard error or a confidence interval, since the three differ by a factor of several and readers cannot tell which you meant.
Round once, at the end. Carry a couple of guard digits through intermediate steps and round only the final answer, because rounding at every stage accumulates a bias that has nothing to do with the measurement. For the same reason a conversion should use the exact defined factor where one exists, such as 25.4 mm to the inch or 101,325 Pa to the standard atmosphere, rather than a remembered approximation.
Common questions
Should my error bars show standard deviation or standard error?
It depends on what the figure is claiming. Standard deviation describes how spread out the individual measurements are and does not shrink as you add data, so it is the right choice when the point is variability within the sample. Standard error, or a confidence interval, describes how precisely the mean is known and falls as one over the square root of the number of measurements. Whichever you use, label it, because standard error bars are always the smaller of the two and an unlabelled figure is impossible to interpret.
How many measurements do I actually need?
Random error falls as the square root of the count, so four times the data halves the standard error and sixteen times quarters it. That is a rapidly diminishing return, and it only ever reduces the random component. Once the standard error has dropped below the systematic uncertainty in your setup, such as an instrument calibration offset, further repetition does not improve the result at all. The better investment at that point is calibration or a different method, not more readings.