Propagation of Error Ch En 475 Unit Operations. Quantifying variables (i.e. answering a question with a number) 1. Directly measure the variable. - referred.

Slides:



Advertisements
Similar presentations
Estimation of Means and Proportions
Advertisements

Design of Experiments Lecture I
Welcome to PHYS 225a Lab Introduction, class rules, error analysis Julia Velkovska.
General Statistics Ch En 475 Unit Operations. Quantifying variables (i.e. answering a question with a number) 1. Directly measure the variable. - referred.
Materials for Lecture 11 Chapters 3 and 6 Chapter 16 Section 4.0 and 5.0 Lecture 11 Pseudo Random LHC.xls Lecture 11 Validation Tests.xls Next 4 slides.
Sampling: Final and Initial Sample Size Determination
Ch11 Curve Fitting Dr. Deshi Ye
Sampling Distributions (§ )
Design of Experiments and Data Analysis. Let’s Work an Example Data obtained from MS Thesis Studied the “bioavailability” of metals in sediment cores.
Sample size computations Petter Mostad
Introduction to Inference Estimating with Confidence Chapter 6.1.
Statistics: Data Analysis and Presentation Fr Clinic II.
L Berkley Davis Copyright 2009 MER301: Engineering Reliability Lecture 14 1 MER301: Engineering Reliability LECTURE 14: Chapter 7: Design of Engineering.
Quality Control Procedures put into place to monitor the performance of a laboratory test with regard to accuracy and precision.
Types of Errors Difference between measured result and true value. u Illegitimate errors u Blunders resulting from mistakes in procedure. You must be careful.
Inferences About Process Quality
1 BA 555 Practical Business Analysis Review of Statistics Confidence Interval Estimation Hypothesis Testing Linear Regression Analysis Introduction Case.
Relationships Among Variables
Regression and Correlation Methods Judy Zhong Ph.D.
Quantify prediction uncertainty (Book, p ) Prediction standard deviations (Book, p. 180): A measure of prediction uncertainty Calculated by translating.
Inference for regression - Simple linear regression
LINEAR REGRESSION Introduction Section 0 Lecture 1 Slide 1 Lecture 5 Slide 1 INTRODUCTION TO Modern Physics PHYX 2710 Fall 2004 Intermediate 3870 Fall.
Development of An ERROR ESTIMATE P M V Subbarao Professor Mechanical Engineering Department A Tolerance to Error Generates New Information….
Statistical Methods For UO Lab — Part 1 Calvin H. Bartholomew Chemical Engineering Brigham Young University.
Copyright © 2013, 2010 and 2007 Pearson Education, Inc. Chapter Inference on the Least-Squares Regression Model and Multiple Regression 14.
Statistics Primer ORC Staff: Xin Xin (Cindy) Ryan Glaman Brett Kellerstedt 1.
Mote Carlo Method for Uncertainty The objective is to introduce a simple (almost trivial) example so that you can Perform.
Topic 5 Statistical inference: point and interval estimate
Lecture 12 Statistical Inference (Estimation) Point and Interval estimation By Aziza Munir.
PARAMETRIC STATISTICAL INFERENCE
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 1 Part 4 Curve Fitting.
Measurement Uncertainties Physics 161 University Physics Lab I Fall 2007.
General Statistics Ch En 475 Unit Operations. Quantifying variables (i.e. answering a question with a number) Each has some error or uncertainty.
Basic Probability (Chapter 2, W.J.Decoursey, 2003) Objectives: -Define probability and its relationship to relative frequency of an event. -Learn the basic.
LECTURER PROF.Dr. DEMIR BAYKA AUTOMOTIVE ENGINEERING LABORATORY I.
L Berkley Davis Copyright 2009 MER301: Engineering Reliability Lecture 16 1 MER301: Engineering Reliability LECTURE 16: Measurement System Analysis and.
Chapter 11 Linear Regression Straight Lines, Least-Squares and More Chapter 11A Can you pick out the straight lines and find the least-square?
General Statistics Ch En 475 Unit Operations. Quantifying variables (i.e. answering a question with a number) 1. Directly measure the variable. - referred.
Ch 6-1 © 2004 Pearson Education, Inc. Pearson Prentice Hall, Pearson Education, Upper Saddle River, NJ Ostwald and McLaren / Cost Analysis and Estimating.
Lecture 8 Simple Linear Regression (cont.). Section Objectives: Statistical model for linear regression Data for simple linear regression Estimation.
Inference for Regression Simple Linear Regression IPS Chapter 10.1 © 2009 W.H. Freeman and Company.
A Process Control Screen for Multiple Stream Processes An Operator Friendly Approach Richard E. Clark Process & Product Analysis.
Confidence intervals: The basics BPS chapter 14 © 2006 W.H. Freeman and Company.
Propagation of Error Ch En 475 Unit Operations. Quantifying variables (i.e. answering a question with a number) 1. Directly measure the variable. - referred.
Statistics Presentation Ch En 475 Unit Operations.
VI. Regression Analysis A. Simple Linear Regression 1. Scatter Plots Regression analysis is best taught via an example. Pencil lead is a ceramic material.
LECTURE 3: ANALYSIS OF EXPERIMENTAL DATA
Experimental Data Analysis Prof. Terry A. Ring, Ph. D. Dept. Chemical & Fuels Engineering University of Utah
Statistical Data Analysis
Chapter 10: Confidence Intervals
NON-LINEAR REGRESSION Introduction Section 0 Lecture 1 Slide 1 Lecture 6 Slide 1 INTRODUCTION TO Modern Physics PHYX 2710 Fall 2004 Intermediate 3870 Fall.
Analysis of Experimental Data; Introduction
Statistics Presentation Ch En 475 Unit Operations.
Introduction to inference Estimating with confidence IPS chapter 6.1 © 2006 W.H. Freeman and Company.
Introduction to Engineering Calculations Chapter 2.
ChE 551 Lecture 04 Statistical Tests Of Rate Equations 1.
1 DATA ANALYSIS, ERROR ESTIMATION & TREATMENT Errors (or “uncertainty”) are the inevitable consequence of making measurements. They are divided into three.
Yandell – Econ 216 Chap 15-1 Chapter 15 Multiple Regression Model Building.
Chapter 13 Simple Linear Regression
Chapter 4 Basic Estimation Techniques
Basic Estimation Techniques
Introduction, class rules, error analysis Julia Velkovska
Materials for Lecture 18 Chapters 3 and 6
Statistics Presentation
Basic Estimation Techniques
Statistical Methods For Engineers
CHAPTER 29: Multiple Regression*
Statistics Review ChE 477 Winter 2018 Dr. Harding.
Statistical Data Analysis
Sampling Distributions (§ )
Presentation transcript:

Propagation of Error Ch En 475 Unit Operations

Quantifying variables (i.e. answering a question with a number) 1. Directly measure the variable. - referred to as “measured” variable ex. Temperature measured with thermocouple 2. Calculate variable from “measured” or “tabulated” variables - referred to as “calculated” variable ex. Flow rate m =  A v (measured or tabulated) Each has some error or uncertainty

Example: You take measurements of , A, v to determine m =  Av. What is the range of m and its associated uncertainty? Calculate variable from multiple input (measured, tabulated, …) variables (i.e. m =  Av) What is the uncertainty of your “calculated” value? Each input variable has its own error Uncertainty of Calculated Variable Details provided in Applied Engineering Statistics, Chapters 8 and 14, R.M. Bethea and R.R. Rhinehart, 1991).

To obtain uncertainty of “calculated” variable DO NOT just calculate variable for each set of data and then average and take standard deviation DO calculate uncertainty using error from input variables: use uncertainty for “calculated” variables and error for input variables Plan: Obtain max error (  ) for each input variable then obtain uncertainty of calculated variable Method 1: Propagation of max error - brute force Method 2: Propagation of max error - analytical Method 3: Propagation of variance - analytical Method 4: Propagation of variance - brute force – Monte Carlo simulation

Value and Uncertainty Value used to make decisions - need to know uncertainty of value Potential ethical and societal impact How do you determine the uncertainty of the value? Sources of uncertainty ( from Rhinehart, Applied Engineering Statistics, 1991 ): 1. Estimation - we guess! 2. Discrimination - device accuracy (single data point) 3. Calibration - may not be exact (error of curve fit) 4. Technique - i.e. measure ID rather than OD 5. Constants and data - not always exact! 6. Noise - which reading do we take? 7. Model and equations - i.e. ideal gas law vs. real gas 8. Humans - transposing, …

Estimates of Error (  ) for input variables (  ’s are propagated to  find uncertainty) 1. Measured: measure multiple times; obtain s;  ≈ 2.5s Reason: 99% of data is within ± 2.5s Example: s = 2.3 ºC for thermocouple,  = 5.8 ºC 2. Tabulated :  ≈ 2.5 times last reported significant digit (with 1) Reason: Assumes last digit is ± 2.5 (± 0 assumes perfect, ± 5 assumes next left digit is fuzzy) Example:  = 1.3 g/ml at 0º C,  = 0.25 g/ml Example: People = 127,000  = 2500 people

Estimates of Error (  ) for input variables 3. Manufacturer spec or calibration accuracy: use given spec or accuracy data Example: Pump spec is ± 1 ml/min,  = 1 ml/min 4.Variable from regression (i.e. calibration curve):  ≈ 2.5*standard error (std error is stdev of residual) Example: Velocity is slope with std error = 2 m/s 5. Judgment for a variable: use judgment for  Example: Read pressure to ± 1 psi,  = 1 psi

Estimate of Error for Calculated Variables (i.e., Propagation of Error) A.Max error: 1.propagating error with brute force 2.propagating error analytically B.Probable error: 1.propagating variance analytically 2.propagating variance with brute force (i.e., Monte Carlo)

Example Problem Data from a computer show that the flow rate is 562 ml/min ± 3 ml/min (stdev of computer noise). Your calibration shows 510 ml/min ± 8 ml/min (stdev). What flow rate do you use and what is  ? In the following propagation methods, it’s assumed that there is no bias in the values used - let’s assume this for all lab projects.

 Brute force method: obtain upper and lower limits of all input variables (from maximum errors); plug into equation to get uncertainty of calculated variable (y).  Uncertainty of y is between y min and y max.  This method works for both symmetry and asymmetry in errors ( i.e. 10 psi + 3 psi or - 2 psi ) Method 1: Propagation of max error- brute force

Example: Propagation of max error- brute force  = 2.0 g/cm 3 (table) A = 3.4 cm 2 (measured avg) v = 2 cm/s (slope of graph) s A = 0.03 cm 2 std. error (v) = 0.05 cm/s minmax  A v Brute force method: All combinations Additional information: What is  for each input variable?

Example: Propagation of max error- brute force  = 2.0 g/cm 3 (table)2.5  lowest digit = 0.25 A = 3.4 cm 2 (measured avg)2.5  s A = v = 2 cm/s (slope of graph)2.5  std. error (v) = s A = 0.03 cm 2 std. error (v) = 0.05 cm/s Additional information: What is  for each input variable? Compute  (look at cheat sheet)

Example: Propagation of max error- brute force  = 2.0 g/cm 3 (table) A = 3.4 cm 2 (measured avg) v = 2 cm/s (slope of graph) s A = 0.03 cm 2 std. error (v) = 0.05 cm/s minmax  A v Brute force method: All combinations Additional information: What is  for each input variable? 

Method 2: Propagation of max error- analytical Propagation of error: Utilizes maximum error of input variable (  ) to estimate uncertainty range of calculated variable (y) Uncertainty of y: y = y avg ±  y Assumptions: input errors are symmetric input errors are independent of each other equation is linear (works o.k. for non-linear equations if input errors are relatively small) * Remember to take the absolute value!!

Example: Propagation of max error- analytical y x 1 x 2 x 3 = (3.4)(2)(0.25) = 0.60 (2.85) m = m avg ±  m =  Av ±  m = 13.6 ± 2.85 g/s Av  v  A 3.4  22  22  3.4  = 2.0 g/cm 3 (table) A = 3.4 cm 2 (measured avg) v = 2 cm/s (slope of graph) For  s  = 0.1 g/cm 3    s A = 0.03 cm 2,    std. error (v) = 0.05 cm/s  v  Remember from above: f error,   (fractional error)

Propagation of max error If linear equation, symmetric errors, and input errors are independent  brute force and analytical are same If non-linear equation, symmetric errors, and input errors are independent  brute force and analytical are close if errors are small. If large errors (i.e. >10% or more than order of magnitude), brute force is more accurate. Must use brute force if errors are dependent on each other and/or asymmetric. Analytical method is easier to assess if lots of inputs. Also gives info on % contribution from each error.

Method 3: Propagation of variance- analytical 1. Maximum error can be calculated from max errors of input variables as shown previously: a) Brute force b) Analytical 2. Probable error is more realistic Errors are independent (some may be “+” and some “-”). Not all will be in same direction. Errors are not always at their largest value. Thus, propagate variance rather than max error You need variance (   ) of each input to propagate variance. If  (stdev) is unknown, estimate  =  /2.5

Method 3: Propagation of variance- analytical y = y avg ± 1.96 SQRT(   y ) 95% y = y avg ± 2.57 SQRT(   y ) 99% gives propagated variance of y or (stdev) 2 gives probable error of y and associated confidence error should be <10% (linear approximation) use propagation of max error if not much data, use propagation of variance if lots of data

Example: Propagation of variance Calculate  and its 95% probable error All independent variables were measured multiple times (Rule 1); averages and s are given M = 5.0 kg s = 0.05 kg L = 0.75 m s = 0.01 m D = 0.14 m s = m

Propagation of Variance

Method 4: Monte Carlo Simulation (propagation of variance – brute force) Choose N (N is very large, e.g. 100,000) random ±δ i from a normal distribution of standard deviation σ i for each variable and add to the mean to obtain N values with errors: – rnorm(N,μ,σ) in Mathcad generates N random numbers from a normal distribution with mean μ and std dev σ Find N values of the calculated variable using the generated x’ i values. Determine mean and standard deviation of the N calculated variables.

Monte Carlo Example 1

Monte Carlo Simulation Example 2 Estimate the uncertainty in the critical compressibility factor of a fluid if T c = 514 ± 2 K, P c = ± 0.6 bar, and V c = ± m 3 /kmol?

Overall Summary A.Measured variables: (use all) 1.Average 2.Std dev (data range) 3.Confidence interval from student t-test (mean range and mean comparison) B.Calculated variable: determine uncertainty (pick one) 1.Max error: propagating error with brute force 2.Max error: propagating error analytically 3.Probable error: propagating variance analytically 4.Probable error: propagating variance with brute force (i.e., Monte Carlo)

Data and Statistical Expectations (for UO Lab reports) 1.Summary of raw data (table format) 2.Sample calculations– including statistical calculations 3.Summary of all calculations- table format is helpful 4.If measured variable: average and standard deviation for all, confidence of mean for at least one variable 5.If calculated variable: 1 of the 4 methods. Please state in report. If messy equation, you may show 1 of 4 methods for small part and then just average (with std dev.) the value (although not the best method).