Physics 114: Lecture 12 Error Analysis, Part II Dale E. Gary NJIT Physics Department.

Slides:



Advertisements
Similar presentations
Completing the Square and the Quadratic Formula
Advertisements

Complex Numbers.
CALCULATOR MANIPULATION. Due to the differences in calculators you will have to be able to use your own effectively.
Quadratic Equations.
Complex Power – Background Concepts
Physics 114: Lecture 9 Probability Density Functions Dale E. Gary NJIT Physics Department.
Physics 114: Lecture 7 Uncertainties in Measurement Dale E. Gary NJIT Physics Department.
Physics 114: Lecture 16 Linear and Non-Linear Fitting Dale E. Gary NJIT Physics Department.
The standard error of the sample mean and confidence intervals
Physics and Measurements.
The standard error of the sample mean and confidence intervals How far is the average sample mean from the population mean? In what interval around mu.
Test Taking Strategies circle important terms underline any numbers Mark the Text double-underline the question Cross out wrong answers Use LOGIC Plug.
Physics 114: Lecture 11 Error Analysis
So are how the computer determines the size of the intercept and the slope respectively in an OLS regression The OLS equations give a nice, clear intuitive.
+ Completing the Square. + In your notes: Simplify the following: (5 – 3i)(4 + 2i) 3.
The standard error of the sample mean and confidence intervals How far is the average sample mean from the population mean? In what interval around mu.
Radical Jeopardy $100 $200 $300 $400 $500 Final Jeopardy
Perfect Squares
Copyright © Cengage Learning. All rights reserved.
Solving Quadratic (and polynomial) Equations by Factoring.
Quadratics       Solve quadratic equations using multiple methods: factoring, graphing, quadratic formula, or square root principle.
Physics 114: Lecture 17 Least Squares Fit to Polynomial
5.7 Complex Numbers 12/17/2012.
Physics 114: Lecture 15 Probability Tests & Linear Fitting Dale E. Gary NJIT Physics Department.
Introduction l Example: Suppose we measure the current (I) and resistance (R) of a resistor. u Ohm's law relates V and I: V = IR u If we know the uncertainties.
Systems of Nonlinear Equations in Two Variables
2.5 Introduction to Complex Numbers 11/7/2012. Quick Review If a number doesn’t show an exponent, it is understood that the number has an exponent of.
Physics 114: Exam 2 Review Lectures 11-16
R Kass/SP07 P416 Lecture 4 1 Propagation of Errors ( Chapter 3, Taylor ) Introduction Example: Suppose we measure the current (I) and resistance (R) of.
Physics 430: Lecture 19 Kepler Orbits Dale E. Gary NJIT Physics Department.
Pre calculus Problem of the Day Homework: p eoo, odds Factor the following:
Treatment of Uncertainties
Rules for Means and Variances. Rules for Means: Rule 1: If X is a random variable and a and b are constants, then If we add a constant a to every value.
Precalculus Fifth Edition Mathematics for Calculus James Stewart Lothar Redlin Saleem Watson.
Algebra II Honors POD Homework: p odds, odds (you must use completing the square), and 77, 83 Find all real solutions for the following:
Solving Quadratic Equations. Solving by Factoring.
Physics 114: Lecture 14 Mean of Means Dale E. Gary NJIT Physics Department.
5.7 Complex Numbers 12/4/2013. Quick Review If a number doesn’t show an exponent, it is understood that the number has an exponent of 1. Ex: 8 = 8 1,
Derivation of the Quadratic Formula The following shows how the method of Completing the Square can be used to derive the Quadratic Formula. Start with.
Dear Power point User, This power point will be best viewed as a slideshow. At the top of the page click on slideshow, then click from the beginning.
Chapter 1: Square Roots and the Pythagorean Theorem Unit Review.
Solving Quadratic (and polynomial) Equations by Factoring.
How to solve Quadratic Equations By John Jackson.
Example x y We wish to check for a non zero correlation.
Unit 2: Exponents Review. What is on the test??? 1.Exponent Rules 2.Perfect Squares 3.Square Roots / Cube Roots 4.Estimating Non-Perfect Squares 5.Scientific.
CHAPTER- 3.2 ERROR ANALYSIS. 3.3 SPECIFIC ERROR FORMULAS  The expressions of Equations (3.13) and (3.14) were derived for the general relationship of.
7.2 Means & Variances of Random Variables AP Statistics.
Uncertainties and errors
Dear Power point User, This power point will be best viewed as a slideshow. At the top of the page click on slideshow, then click from the beginning.
Directions 1.With a method similar to that of the previous lab, you will be using a Rutherford analysis to uncover a value hidden in your data. 2.Begin.
Variability. The differences between individuals in a population Measured by calculations such as Standard Error, Confidence Interval and Sampling Error.
Variability.
Quadrant II where x is negative and y is positive
Physics 114: Lecture 12 Mean of Means
Physics 114: Exam 2 Review Weeks 7-9
Physics 114: Lecture 7 Probability Density Functions
ECE 2202 Circuit Analysis II
YES! The Quadratic Formula
Physics 114: Lecture 10 Error Analysis/ Propagation of Errors
The Irrational Numbers and the Real Number System
Completing the Square.
Physics 1 – Aug 26, 2016 P3 Challenge – Do Now (on slips of paper)
TRIGONOMETRY 5.3 RADICALS Ms. Albarico.
Physics 114: Lecture 11 Error Analysis, Part II
Warm Up Simplify: a)
Solving Quadratic Equations by Factoring
Treatment of Uncertainties
Treatment of Uncertainties
Concepts of Computation
Presentation transcript:

Physics 114: Lecture 12 Error Analysis, Part II Dale E. Gary NJIT Physics Department

Mar 8, 2010 Method of Propagation of Errors  Start with original relation, in this case:  Use the chain rule:  Here, dI represents the deviations of individual measurements :  We now square both sides to give the square deviations:  Finally, average over many measurements:

Mar 8, 2010 A Great Simplifier—Relative Error  Notice that we can take:  And divide through by I 2 = V 2 /R 2 :  What about this term ? This is the product of random fluctuations in voltage and resistance. When we multiply these random fluctuations and then average them—they should average to zero!  Thus, we have the final result:  The general formula, developed in the text, is Square of relative error in I

Mar 8, 2010 Other Examples  For homework, you should have calculated some uncertainties for quantities made up of calculations of other quantities with their own measurement uncertainties.  Let me point out a few patterns:  You see the quadratic nature of the resultant error—the errors behave like the pythagorean theorem. This is a good way to think about errors, and can be a big help in estimating errors. Note the effect of powers, which expand the influence of errors of a quantity. error in v error in u error in x All covariances assumed zero (i.e. u and v not correlated)

Mar 8, 2010 MatLAB Examples  Make random arrays u = randn(1,1000); and v = randn(1,1000); then plot v vs. u (i.e. plot(u,v,’.’)). Set ‘axis equal’ to see them on the same scale. The cloud of points form a circular pattern, concentrated in the center.  Now multiply v by 2, and plot again with axis equal. The clouds form an oval cloud of points.  Add 10 to u and 15 to v and replot with axis equal. Adding constants does not change the errors, only the mean.  Now calculate the relative errors for u, v, and x=u.*v. Do they obey the expected relationship?  Now calculate the relative errors for x=u./v. They should obey the same relationship. Do they?  Look at hist(u,20), hist(v,20), hist(u.*v,20), hist(u./v,20).  Now subtract 13 from v and calculate relative errors for x=u./v. What is wrong?

Mar 8, 2010 Estimating Error  As noted, the way to think about errors is to consider relative uncertainty (or percent error). If we have a 10% error in both u and v, what is the percent error in x for this expression?  What if u has a 1% relative error and v has a 10% relative error? What is percent error in x then?  So thinking in terms of the Pythagorean Theorem, errors are dominated by the biggest term, unless both have similar errors.  What if both u and v have 10% errors, and x = uv 4 ? 40%, in this case

Mar 8, 2010 Reducing Error  Knowing how errors propagate is very important in reducing sources of error. Let’s say you do an experiment that results in a measurement whose errors are a factor of 2 too high. You have a budget that allows you do reduce the errors in one quantity by a factor of 2. Where do you put your resources?  If the relationship is then if the relative errors are equal you are doomed to failure, because you can only reduce the total by 1.4 (square root of 2). But if the relative error in u is much smaller than that in v, you put your resources into reducing the error in v. Likewise, if the relationship is then you put your resources into reducing the error in v, unless the relative error in v is already 4 times smaller than in u.