Uncertain
Provides tools to manipulate numbers with inherent experimental/measurement
uncertainty, and propagates them through functions based on principles from
statistics.
Documentation maintained at https://mstksg.github.io/uncertain.
Usage
import Numeric.Uncertain
Create numbers
7.13 +/- 0.05
91800 +/- 100
12.5 `withVar` 0.36
exact 7.9512
81.42 `withPrecision` 4
7 :: Uncert Double
9.18 :: Uncert Double
fromSamples [12.5, 12.7, 12.6, 12.6, 12.5]
Can be descontructed/analyzed with :+/-
(pattern synonym/pseudo-constructor
matching on the mean and standard deviation), uMean
, uStd
, uVar
, etc.
Manipulate with error propagation
ghci> let x = 1.52 +/- 0.07
ghci> let y = 781.4 +/- 0.3
ghci> let z = 1.53e-1 `withPrecision` 3
ghci> cosh x
2.4 +/- 0.2
ghci> exp x / z * sin (y ** z)
10.9 +/- 0.9
ghci> pi + 3 * logBase x y
52 +/- 5
Propagates uncertainty using second-order multivariate Taylor expansions of
functions, computed using the ad library.
Arbitrary numeric functions
ghci> liftUF (\[x,y,z] -> x*y+z)
[ 12.2 +/- 0.5
, 56 +/- 2
, 0.12 +/- 0.08
]
680 +/- 40
Can propagate uncertainty on complex functions take from potentially correlated
samples.
ghci> import Numeric.Uncertain.Correlated
ghci> evalCorr $ do
x <- sampleUncert $ 12.5 +/- 0.8
y <- sampleUncert $ 15.9 +/- 0.5
z <- sampleUncert $ 1.52 +/- 0.07
let k = y ** x
resolveUncert $ (x+z) * logBase z k
1200 +/- 200
"Interactive" Exploratory Mode
Correlated module functionality can be used in ghci or IO
or ST
, for
"interactive" exploration.
ghci> x <- sampleUncert $ 12.5 +/- 0.8
ghci> y <- sampleUncert $ 15.9 +/- 0.5
ghci> z <- sampleUncert $ 1.52 +/- 0.07
ghci> let k = y**x
ghci> resolveUncert $ (x+z) * logBase z k
1200 +/- 200
Monte Carlo-based propagation of uncertainty
Provides a module for propagating uncertainty using Monte Carlo
simulations
ghci> import qualified Numeric.Uncertain.MonteCarlo as MC
ghci> import System.Random.MWC
ghci> let x = 1.52 +/- 0.07
ghci> let y = 781.4 +/- 0.3
ghci> let z = 1.53e-1 `withPrecision` 3
ghci> g <- create
ghci> cosh x
2.4 +/- 0.2
ghci> MC.liftU cosh x g
2.4 +/- 0.2
ghci> exp x / z * sin (y ** z)
10.9 +/- 0.9
ghci> MC.liftU3 (\a b c -> exp a / c * sin (b**c)) x y z g
10.8 +/- 1.0
ghci> pi + 3 * logBase x y
52 +/- 5
ghci> MC.liftU2 (\a b -> pi + 3 * logBase a b) x y g
51 +/- 5
Comparisons
Note that this is very different from other libraries with similar data types
(like from intervals and rounding); these do not attempt to maintain intervals or
simply digit precisions; they instead are intended to model actual
experimental and measurement data with their uncertainties, and apply
functions to the data with the uncertainties and properly propagating the
errors with sound statistical principles.
For a clear example, take
> (52 +/- 6) + (39 +/- 4)
91. +/- 7.
In a library like intervals, this would result in 91 +/- 10
(that is, a
lower bound of 46 + 35 and an upper bound of 58 + 43). However, with
experimental data, errors in two independent samples tend to "cancel out", and
result in an overall aggregate uncertainty in the sum of approximately 7.
Copyright
Copyright (c) Justin Le 2016