Experimental Experimental Errors Errors and and Error Error Analysis Analysis Rajeev Prabhakar University of Texas at Austin, Austin, TX Freeman Research Group Meeting March 10, 2004 Topics covered • Types of experimental errors • Reducing errors • Describing errors quantitatively – Measured variables – Quantities calculated from measured variables (error propagation) • Least-squares fit – straight line – polynomial – arbitrary function Ref: Bevington and Robinson, Data Reduction and Error Analysis for the Physical Sciences, 2nd edition, McGraw Hill, NY 1992 Quality of Experiments and Experimental Error • Accuracy – Measure of correctness of result • Precision – Measure of reproducibility of result • Types of errors – Mistakes • Wrong membrane used • Number recorded incorrectly, 1.92 written as 1.29 – Systematic error • Change in membrane casting conditions • Incorrect calibration – Random error • Fluctuations in temperature, pressure etc. Reducing Errors • Planning experiments carefully – Objective is to understand and reduce sources of systematic error – Don’t give in to the “it’s always been done this way” mentality • Use more accurate instruments • Repeat the measurement, if possible Uncertainties in Measured Variables • Fluctuations – Often independent of actual value • Reading an analog instrument – ½ of smallest scale division/least count • Uncertainty estimate – standard deviation, σ – ½ of least count – Repeat measurement if possible and take standard deviation of the data Parameters calculated from measured variables • Propagation of Errors – e.g. Volume measurement Vo = LoWo H o If the measured values are L, W and H , ∂V ∂V ∂V V ( L,W , H ) Vo + ∆L + ∆W + ∆H ∂L WoHo ∂W LoHo ∂H LoWo Error , ∆V = V − Vo 2 2 N N 1 1 2 Variance, σ V = ∑ (Vi − Vo ) = lim Vi − V ∑ N →∞ N i =1 N i =1 ( ) Propagation of errors – general formula y = f (u , v) ∂y ∂y yi − y = (ui − u ) + (vi − v) ∂u ∂v 2 N 1 σ y2 = lim y − y ∑ i N →∞ N 1 i = ( ) 2 2 1 y y ∂ ∂ ∂y ∂y 2 2 2 σ y = lim ∑ (ui − u ) + ∑ (vi − v) + ∑ 2(ui − u )(vi − v) N →∞ ∂u ∂v ∂u ∂v N 2 2 ∂y ∂y ∂y ∂y σ y2 = σ u2 + σ v2 + 2σ uv2 ∂u ∂v ∂u ∂v (1) co-variance Neglecting the co - variance, 2 ∂y ∂y σ y2 σ u2 + σ v2 ∂u ∂v 2 (2) Volume example – simplified equation 2 ∂y 2 ∂y σ σ +σv ∂u ∂v 2 y 2 2 u 2 2 2 2 ∂V 2 ∂V 2 ∂V σV σ L + σW +σH L W H ∂ ∂ ∂ Since V = LWH , σ σ (WH ) + σ 2 V 2 2 L 2 2 W ( HL ) + σ ( LW ) 2 2 H 2 V 2 V 2 V σ σ + σW + σ H L W H 2 V 2 2 2 2 L 2 2 2 σV σ L σW σ H V L + W + H 2 Simplified form of equation valid when the dependent variable is a product of independent variables to the 1 or -1 power only Example - Limitations of simplified equation If V = π R 2 H , 2 ∂V 2 ∂V σ σ +σH ∂R ∂H 2 V 2 R σ σ ( 2π RH ) + σ 2 V 2 2 2 R 2 H (π R ) 2 2 2V 2 V σ σ +σH R H 2 V 2 2 R 2 2 σ V 2σ R σ H V R + H 2 2 Least-squares fit to a straight line • y = a + b*x • Objective is to find the values of a and b that provide the best prediction of y for a given x 2 χ • Goodness-of-fit parameter, 1 2 2 χ = ∑ 2 ( yi − a − bxi ) σ i (3) To minimize the error, ∂χ 2 ∂χ 2 =0= ∂a ∂b • Resulting equations for a and b – pgs. 104 and 113 of Bevington • Errors in a and b - Equations on pgs. 109 & 114 of Bevington Least-squares fit to an equation linear in the coefficients • Example, Polynomial: y = a + b*x + c*x2 + ….. Other functions: y = a + b*ex • Similar mathematical treatment as for straight line. However, determinants get bigger and more numerous. See pg 117 (last 3 lines) and 118 for example of quadratic equation. • Alternate method – Matrix solution (pg. 121) Matrix Method for equation linear in coefficients m y ( xi ) = ∑ ak f k ( xi ) k =1 The coefficient matrix a is given by, a = βα −1 where 1 β k = ∑ 2 yi f k ( xi ) ; row matrix σ i 1 α lk = ∑ 2 f l ( xi ) f k ( xi ) ; symmetric matrix σ i Error in the coefficients are elements of the inverse α matrix - Diagonal elements are variances σ a2k = α kk−1 - Off-diagonal elements are co-variances σ a2l ak = α lk−1 Example – Quadratic fit to Permeability data P = b + c ∆p + d ( ∆ p ) 2 Compare with, m y ( xi ) = ∑ ak f k ( xi ) = a1 f1 ( xi ) + a2 f 2 ( xi ) + a3 f 3 ( xi ) k =1 Therefore, a1 = b; a2 = c; a3 = d ; f1 = 1; f 2 = ∆p; f 3 = ( ∆p ) 2 Solve for a, b and c using matrix method You will also obtain variances and covariances (previous slide) Then, calculate error in P using eqs. (1) or (2). Example in Excel file: Error analysis demo.xls; sheet: P For more details, including an example, Bevington: pgs. 121-125 Least-squares fit to any function • Best-fit for functions that are not linear in the coefficients • Trial-and-error methods (Ch. 8, Bevington) • Find coefficient values by using SOLVER function in Excel • 2 χ To get errors, vary one coefficient at a time to increase by 1 • The change in the coefficient is it’s standard deviation Example – S fit to dual mode equation f *g S =e+ 1+ g * p Determine coefficients by minimizing χ 2 , 2 N S S − 1 χ 2 = ∑ calc exp t σi N i =1 by varying the coefficients e, f and g. Change initial guess values of the coefficients to confirm best - fit values. Then determine σ for each coefficient, by the method described on the previous slide. Example in Excel file: Error analysis demo.xls; sheet: S Calculating Deff from best fit equations of P and S dP dp Deff (C2 ) = P + ∆p dC ∆ d p p2 p2 b + 2c(∆p ) + 3d (∆p) 2 NUMR = = fg DENR e+ (1 + g p ) 2 Calculate NUMR & DENR and their errors. Calculate Deff . σ Deff Error in Deff , D eff 2 σ NUMR 2 σ DENR 2 = + NUMR DENR References Bevington •Pgs. 1-6: Accuracy, precision and uncertainties •Pgs. 41-48: Propagation of errors with specific examples •Pgs. 101-114: Least-squares fit to a straight line •Pgs. 115-125: Least-squares fit to a function linear in the coefficients, including an example for a quadratic fit Microsoft Excel Help •MINVERSE worksheet function •MMULT worksheet function Questions
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