Week Exp Date Lecture topic(s) Assignment. Course Overview. Intro: Measurements, uncertainties. Lab: Discussion of Exp 3 goals, setup
|
|
- April Amy Norman
- 5 years ago
- Views:
Transcription
1 Schedule for Physics BL - Fall 01 Find relevan Lab Guides on he course web sie o prepare for Quizzes. Reading maerial and pracice problems are from Taylor, Error Analysis. Week Exp Dae Lecure opic(s) Assignmen Oc 8-Oc 3 15-Oc 4 -Oc 5 9-Oc Nov Course Overview. nro: Measuremens, uncerainies. Discussion of Exp 1 goals, seup (Deduce mean densiy of earh) Saisical Analysis Saisical Analysis Hisograms & Disribuions The Gaussian Disribuion Discussion of Exp goals, seup (Deducion of mass disribuions) Maximum Likelihood, Rejecion of Daa, Weighed Mean Discussion of Exp 3 goals, seup (Tune a shock absorber) 7 1-Nov No Lecure Veerans Day Nov 9 6-Nov 10 3-Dec Discussion of Exp 4 goals, seup (Calibrae a volmeer) Covariance and Correlaion, es of a disribuion Final Exam Monday evening, 7PM, Peer 110 Taylor: -Read Chaps 1-3. Lab: Taylor: Lab: Taylor: Lab: Taylor: Lab: Taylor: Lab: Taylor: Lab: Taylor: Lab: Taylor: Lab: -Be prepared for Quiz #1, -Read Guidelines for Exp -Sudy probs. 3.10, 3.8, 3.36, 3.41 (HW1 pracice) -Hand in Exp. 1 lab repor -Read Chap 4. -Sudy probs. 4.18, 4.6, 4.6, 4.14 (HW pracice) -Be prepared for Quiz # -Read Chap 5 -Sudy probs. 5.0, 5.36, 5., 5.6 (HW3 pracice) -Hand in Exp. lab repor -Read Chap 6 & 7 -Sudy probs. 7., 6.4 (HW4 pracice) -Be prepared for Quiz #3 -Read Chap 8 -Sudy probs. 8.10, 8.6, 8.4 (HW5 pracice) -Hand in Exp. 3 lab repor -Read Chap 9 & 1. -Be prepared for Quiz #4 -Sudy probs. 9.14, 1.3, 1.14 (HW6 pracice) -Hand in Exp. 4 lab repor -Prepare for Final Exam -Aend review session nd Pre-Lab Quiz 3 rd Pre-Lab Quiz 4 h Pre-Lab Quiz 1
2 Today s Lecure: ssues from las week lab secions? Logisics nroducion o experimen # Sraegy Non-desrucive measuremen of variaion Discussion of daa nerpreaion & Error Analysis Compaibiliy of measured resuls T-score Confidence Level
3 Logisics During Thanksgiving week A04,A06,A07 need o be rescheduled: Sign-up shees for make-up sessions are already posed in he labs 3
4 The Four Experimens Deermine he average densiy of he earh Weigh he Earh, Measure is volume Measure simple hings like lenghs and imes Learn o esimae and propagae errors Non-Desrucive measuremens of densiies, inner srucure of objecs Absolue measuremens Vs. Measuremens of variabiliy Measure momens of ineria Use repeaed measuremens o reduce random errors Consruc, and une a shock absorber Adjus performance of a mechanical sysem Demonsrae criical damping of your shock absorber Measure coulomb force and calibrae a volmeer. Reduce sysemaic errors in a precise measuremen. 4
5 Noe Changes: The Rubric for his Experimen changed. Please download i again from he course websie. New Rubric since Sunday 11/1 evening. There is also a minor change in he experimen guidelines. Please download hem again from he course websie as well. New experimen guidelines since Monday 11/ lae afernoon. 5
6 Experimen Sufficien accuracy High speed Perform a simple, fas, and non-desrucive experimen o measure he variaion in hickness of he shell of a large number of racque balls in shipmens arriving a a number of sores, o deermine if he variaion in hickness is much less han 10%. The problem can be solved by measuring he mass and momen of ineria of he balls. Noe, we only need o measure he variaion in hickness 6
7 Racque Balls R R r R r = M 5 R r d Counerfeiers make balls wih he same mass and he same average momen of ineria,, bu have worse qualiy conrol on he hickness, d, and hence on. We are looking for a larger spread in d implying a spread in. 7
8 Reminder- Wha is momen of ineria? Momen of ineria (), also called mass momen of ineria or he angular mass, (S unis kg m), is he roaional analog of mass. Tha is, i is he ineria of a rigid roaing body wih respec o is roaion. Momen of neria is a measure of resisance o change of angular velociy. = r dm Where m is he mass, and r is he (perpendicular) disance of he poin mass o he axis of roaion. Slide solen from Mike Riley 8
9 momen of ineria for spheres and cylinders Based on dimensional analysis alone, he momen of ineria of a non poin objec mus ake he form: = kim ir Where: M is he mass R is he radius of he objec from he cener of mass (in some cases, he lengh of he objec is used insead.) k is a dimensionless consan ha varies wih he objec in consideraion. nerial consans are used o accoun for he differences in he placemen of he mass from he cener of roaion. Examples include: k = 1, hin ring or hin walled cylinder around is cener k = /5, solid sphere around is cener k = 1/, solid cylinder or disk around is cener Slide solen from Mike Riley 9
10 Wha s he message? This is an experimen abou using repeaed measuremens o deermine he accuracy of a measuremen echnique. Experimenal mehods can be modified and improved in ligh of he resul of repeaed measuremens. We should learn o use averages o improve he accuracy of our resuls. Learn o disinguish beween sources of uncerainies. Error Propagaion is no a mahemaical exercise need o look, analyze and undersand he daa o do hese 10
11 Basic Sraegy - Overview Measure a ime. Repea measuremens o deermine error on. Calculae he Momen of neria,, from. Propagae error on o ge error on. Calculae he desired quaniy q (hickness) from. Propagae error on o ge error on q. The acual value of q is no ineresing in is own righ i maers only for comparison beween racke balls. >> Deermine how many repeaed measuremens are needed o ge he desired accuracy. 11
12 x 1 Rolling ball rackeball x h x 1 phoogae imer disance before saring imer Parameers you need o measure once and use for all ess: - disance, x, beween he saring poin and he nd phoo-gae; - disance, x 1, beween he saring poin and he 1s phoo-gae; - heigh difference, h, beween he wo phoo-gaes: h rolling = xsin radius R - widh of he groove, w, on he rail. Rolling radius of he ball, R, is differen from he acual radius of he ball, R. R ' = R ( w/ ) R w R 1
13 x 1 x h x 1 rackeball phoogae imer disance before saring imer v v/ How o use he measured parameers (ime and geomery) o calculae? 1 1 Mgh = Mv + Energy conservaion. v = R" Rolling radius. v = x 1 # $ % & ' ( Mgh = v M + R " x # $ gh = 1 % + & ' MR" ( MR # gh $ = ) 1 " % x & ' ( Newonian Mechanics for uniform acceleraion. Plug i all ino equaion. Solve for, we ge: = MR' gh " $ # x 1 % ' & 13
14 Repeaing Measuremens The errors on rolling ime will likely be bigger han he smalles division on your imer. You will need o measure repeaedly o find ou wha he error is. You may hen use he repeaed measuremens o reduce he random error on mean ime. # = = n 1 Mean ime for one ball afer n measuremens, 1,,, n, - i n i= 1 1 n n " 1 i= 1 our bes esimae of he acual ime. ( i " ) How many imes should you measure o ge he SDOM o 30% (0.3) of he SD? Sandard deviaion, SD, a measure of scaer of he individual daa poins, 1,,, n, and our esimae of error of an individual measuremen = n Sandard deviaion (error) of he mean (SDOM) our esimae of error of he calculaed mean value, based on he random uncerainies of a large number of individual measuremens. can be reduced o minimum by repeaing he measuremens. Key is reproducibiliy 14
15 Measuring Variaion in Balls 1. Measure rolling ime of one ball many imes o deermine he measuremen error in, σ measuremen N Nex week Chauvene. Measure rolling ime of many, differen balls o deermine he oal spread in, σ oal N one_ball calculae measured RMS variaion of average ime for Penn balls: ball 3. Calculae he spread in ime due o ball manufacure, σ manufacure, by subracing he measuremen error ball 4. Propagae error on ino error on and hen ino error on hickness d oal = manufacure measuremen oal > measuremen σ σ σ d variaion in variaion in variaion in d 15
16 Relaing <> o he hickness We now know how o analyze he iming of he balls. We nex need o relae his o he hickness of he balls. We need his in order o undersand how a 10% variaion in hickness (as claimed by he manufacurer) urns ino a X% variaion in <>..e. we need o deermine X here. We will find ha he mah involved is oo painful o do analyically. We will hus learn how o do his numerically. 16
17 Normalized momen of ineria We measured he momen of ineria of he ball(s),, Defined as: Side-Bar: We measure a ime and compue he momen of ineria. The Momen of neria is a useful inermediae quaniy. We have compued, bu have specified accuracy needed on hickness We need o compue hickness and is associaed error. Do i numerically for he ball Don ry o solve he 5h order equaion We define normalized momen of ineria: = 5 M R5 r 5 R 3 r 3 ; MR = R" $ gh R x # 1 ' & % ) ( And finally: = MR = 5 1 (r / R) 5 1 (r / R) 3 17
18 Propagae Error from o d - Numerically We measure ~ and wan o know, how much he error of ~ influences he error of d = R r Typical value for he balls are d = 4.5 mm and R = 8.5 mm, r = 3.75 mm: 5 ~ 1 (3.75/ 8.5) = = Make a small (3.75/ 8.5) perurbaion Le s ake d = 4.4 mm; we obain for i r = 3.85 mm and 5 ~ 1 (3.85/ 8.5) = = (3.85/ 8.5) ~ d 0.1 " We have = = 0.0 and ~ = = d d 0.0 ~ ~ Tha is = " ~ = 6.7 ~ for he fracional errors d To ge he error of d down o 5%, we need o know ~ wih a precision of 0.75% 18
19 Propagae Error from o d - Summary We needed o propagae errors for a complex funcion ~ ( d) = 5 1 [( R 1 [( R d) / R] d) / R] The numerical mehod we used was o perurb he argumen near a known value, o calculae he change in he funcion and he relaive values of he wo. can be applied in general and is exacly he same as calculaing: ~ ~ " = d " d We needed o know and plug in he acual approximae values of d and R
20 0 Propagae Error from Time o d d ~ ~.7 = 6 We have go and ' ~ " # $ % & ' ( = = x gh R R MR We wan o evaluae in erms of (because i is ha we measure) ~ ~ x gh R R ' ~ ~ = " " = Go sraigh o: R R x gh R R " # $ % & ' + ( = = ' ~ ' ~ R R R R ) / ' (0.57 ~ ) / ' ~ ( ~ ~ " + # " + # = Finally, we obain: d d ~ ~.7 6 " # " " The error analysis indicaes ha o obain d wih a precision of 10%, we need a precision of ~0.4% in. Muliply by / & Rearrange
21 Summary We are only rying o find differences beween balls, herefore, many errors can be ignored. Only he measured rolling imes are imporan. We mus measure one ball many imes o deermine he measuremen accuracy. We mus measure many balls of each ype experimenally o deermine he spread in hickness. Propagae error on ino error on hickness. n pracical erms: as long as he seup and he inended ball saring poin do no change, only random errors of phoo-gaes ime are imporan. To make a conclusion, wheher he hicknesses of differen balls are uniform wihin 10%, i is desirable o measure individual shell hicknesses o ~1% error. ==> An error of 3% in ball hickness, d, implies ha error of average ime,, as small as 0.04% 1
22 Coninuing from las lecure Quick reminder T-score Compaibiliy of measuremens Confidence level
23 GX, Gauss disribuion: he meaning of σ x = σ X σ G X, = e " X + σ G X," X - σ = dx #( x# X ) 1 = x = 0.68 The area under a segmen from X -σ o X+σ accouns for 68% of he oal area under he bell-shaped curve. Tha is, 68% of he measured poins fall wihin σ from he bes esimae x = X
24 GX, Wha abou he probabiliies o find a poin wihin 0.5σ from X, 1.7σ from X, or in general σ from X? 0.5σ 0.5σ 1.7σ 1.7σ σ σ G = e X, " G 1 #( x# X ) To find hose probabiliies we need o calculae X + # X " # X ( x),# Unforunaely, we canno do i analyically and have o look i up in a able
25 =
26 Compaibiliy of a measured resul -score Bes esimae of x: " x bes ± X Compare wih expeced answer x exp and compue -score: " x bes " x exp eced # X " This is he number of sandard deviaions ha x bes differs from x exp. " Therefore, he probabiliy of obaining an answer ha differs from x exp by or more sandard deviaions is: " Prob(ouside σ) = 1-Prob(wihin σ)) 6
27 Accepabiliy of a measured resul Convenions Large probabiliy means likely oucome and hence reasonable discrepancy. reasonable is a maer of convenion We define: < 5 % - significan discrepancy, > 1.96 < 1 % - highly significan discrepancy, >.58 boundary for unreasonable improbabiliy erf() error funcion f he discrepancy is beyond he chosen boundary for unreasonable improbabiliy, ==> he heory and he measuremen are incompaible (a he saed level) 7
28 Example: Confidence Level Two sudens measure he radius of a plane. Suden A ges R=9000 km and esimaes an error of σ = 600 km Suden B ges R=6000 km wih an error of σ =1000 km Wha is he probabiliy ha he wo measuremens would disagree by more han his (given he error esimaes)? ==> Define he discrepancy q = R A -R B = 3000 km. The expeced q is zero. Use propagaion of errors o deermine he error on q. = + = 1170 km q A B Compue he number of observed sandard deviaions from he expeced value of q: q 9000 " 6000 = = = q Now we look a Table A ==>.56 σ corresponds o 98.95% So, The probabiliy o ge a worse resul is 1.05% (= ) We call his he Confidence Level, and his is a bad one. 8
29 Example: Confidence Level A suden measures g, he acceleraion of graviy, repeaedly and carefully, and ges a final answer of 9.5 m/s wih a sandard deviaion of 0.1 m/s. f he measuremens were normally disribued, wih a cener a he acceped value of 9.8, wha is he probabiliy of geing an answer ha differs from 9.8 by as much as (or more han) his resul = = 0.1 s hree sandard deviaions off he mean. Looking up he probabiliy, 3 we see ha 99.73% are wihin 3 sigma, so he required probabiliy is 0.7%. Slide solen from Jim Branson 9
30 Example: Confidence Level The Confidence Level is he probabiliy o ge a worse resul han you measured. Average R e = 6191± 167 km compared o 6370 rue. Wha is he probabiliy o be furher off he correc radius of he earh han he measured value? = = Looking in able A for 1.07, we read 71.54%. Wha are he unis of? This is he probabiliy o be less han 1.07 sigma away so he C.L. is 100% % =8.46%. 30
31 Example: Confidence Level (from one of your colleagues) The Confidence Level is he probabiliy o ge a worse resul han you measured. Average R e = 3000 ± 500 km compared o 6370 rue. Wha is he probabiliy o be furher off he correc radius of he earh han he measured value? = = 6.74 Looking in able A for 6.74, we read %. Try i wih an uncerainy of 000km This is he probabiliy o be more han 6 sigma away so he C.L. is 100% % = very very small number. 31
32 The Normal Disribuion - Example The grades of sudens in a course where found o be normally disribued wih a mean of 80 poins and sandard deviaion of 5 poins. There were 75 sudens in he course. How many sudens would you expec o have scores: a) Beween 75 and 85 poins? b) Higher han 90 poins? c) Beween 70 and 90 poins? d) Bellow 65 Poins? Soluion: a) This grades range is: +/- 1σ herefore, 68% of he scores should be wihin his range 75*0.68 = 187 sudens. b) Grades higher han 90 poins are +σ and above he average. Therefore: N = 0.5 * (1 prob(" )) * 75 = 0.5 * ( ) * 75 = 6 c) Scores beween poins are wihin +/-σ of he mean. Therefore 95.45% of scores are expeced o be wihin his range: N = * 75 = 6 d) Scores bellow 65 poins are more han -3σ bellow he average score. We know ha +/-3σ is expeced o conain 99.7% of he scores. The negaive ail (ouside his range) is expeced o conain half as many: N = 0.5 * (1 prob(3" )) * 75 = 0.5 * ( ) * 75 = 0.4 Noe: one sided ---> 0.5 3
33 33
34 Nex Week s Lecure: ssues from las week s lab-secions Rejecion of Daa The Principle of Maximum Likelihood The weighed average nroducion o fiing Read Taylor Chap 7 34
Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles
Diebold, Chaper 7 Francis X. Diebold, Elemens of Forecasing, 4h Ediion (Mason, Ohio: Cengage Learning, 006). Chaper 7. Characerizing Cycles Afer compleing his reading you should be able o: Define covariance
More informationComparing Means: t-tests for One Sample & Two Related Samples
Comparing Means: -Tess for One Sample & Two Relaed Samples Using he z-tes: Assumpions -Tess for One Sample & Two Relaed Samples The z-es (of a sample mean agains a populaion mean) is based on he assumpion
More informationKINEMATICS IN ONE DIMENSION
KINEMATICS IN ONE DIMENSION PREVIEW Kinemaics is he sudy of how hings move how far (disance and displacemen), how fas (speed and velociy), and how fas ha how fas changes (acceleraion). We say ha an objec
More information20. Applications of the Genetic-Drift Model
0. Applicaions of he Geneic-Drif Model 1) Deermining he probabiliy of forming any paricular combinaion of genoypes in he nex generaion: Example: If he parenal allele frequencies are p 0 = 0.35 and q 0
More informationPhysics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle
Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,
More informationMatlab and Python programming: how to get started
Malab and Pyhon programming: how o ge sared Equipping readers he skills o wrie programs o explore complex sysems and discover ineresing paerns from big daa is one of he main goals of his book. In his chaper,
More informationBiol. 356 Lab 8. Mortality, Recruitment, and Migration Rates
Biol. 356 Lab 8. Moraliy, Recruimen, and Migraion Raes (modified from Cox, 00, General Ecology Lab Manual, McGraw Hill) Las week we esimaed populaion size hrough several mehods. One assumpion of all hese
More informationLAB 5 - PROJECTILE MOTION
Lab 5 Projecile Moion 71 Name Dae Parners OVEVIEW LAB 5 - POJECTILE MOTION We learn in our sudy of kinemaics ha wo-dimensional moion is a sraighforward exension of one-dimensional moion. Projecile moion
More informationIB Physics Kinematics Worksheet
IB Physics Kinemaics Workshee Wrie full soluions and noes for muliple choice answers. Do no use a calculaor for muliple choice answers. 1. Which of he following is a correc definiion of average acceleraion?
More informationLab #2: Kinematics in 1-Dimension
Reading Assignmen: Chaper 2, Secions 2-1 hrough 2-8 Lab #2: Kinemaics in 1-Dimension Inroducion: The sudy of moion is broken ino wo main areas of sudy kinemaics and dynamics. Kinemaics is he descripion
More informationIntroduction to Probability and Statistics Slides 4 Chapter 4
Inroducion o Probabiliy and Saisics Slides 4 Chaper 4 Ammar M. Sarhan, asarhan@mahsa.dal.ca Deparmen of Mahemaics and Saisics, Dalhousie Universiy Fall Semeser 8 Dr. Ammar Sarhan Chaper 4 Coninuous Random
More informationBias in Conditional and Unconditional Fixed Effects Logit Estimation: a Correction * Tom Coupé
Bias in Condiional and Uncondiional Fixed Effecs Logi Esimaion: a Correcion * Tom Coupé Economics Educaion and Research Consorium, Naional Universiy of Kyiv Mohyla Academy Address: Vul Voloska 10, 04070
More informationSPH3U: Projectiles. Recorder: Manager: Speaker:
SPH3U: Projeciles Now i s ime o use our new skills o analyze he moion of a golf ball ha was ossed hrough he air. Le s find ou wha is special abou he moion of a projecile. Recorder: Manager: Speaker: 0
More informationNon-uniform circular motion *
OpenSax-CNX module: m14020 1 Non-uniform circular moion * Sunil Kumar Singh This work is produced by OpenSax-CNX and licensed under he Creaive Commons Aribuion License 2.0 Wha do we mean by non-uniform
More informationVehicle Arrival Models : Headway
Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where
More informationLecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.
Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in
More informationMath 10B: Mock Mid II. April 13, 2016
Name: Soluions Mah 10B: Mock Mid II April 13, 016 1. ( poins) Sae, wih jusificaion, wheher he following saemens are rue or false. (a) If a 3 3 marix A saisfies A 3 A = 0, hen i canno be inverible. True.
More informationACE 562 Fall Lecture 5: The Simple Linear Regression Model: Sampling Properties of the Least Squares Estimators. by Professor Scott H.
ACE 56 Fall 005 Lecure 5: he Simple Linear Regression Model: Sampling Properies of he Leas Squares Esimaors by Professor Sco H. Irwin Required Reading: Griffihs, Hill and Judge. "Inference in he Simple
More informationLinear Response Theory: The connection between QFT and experiments
Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and
More informationSummary:Linear Motion
Summary:Linear Moion D Saionary objec V Consan velociy D Disance increase uniformly wih ime D = v. a Consan acceleraion V D V = a. D = ½ a 2 Velociy increases uniformly wih ime Disance increases rapidly
More informationAP CALCULUS AB 2003 SCORING GUIDELINES (Form B)
SCORING GUIDELINES (Form B) Quesion A blood vessel is 6 millimeers (mm) long Disance wih circular cross secions of varying diameer. x (mm) 6 8 4 6 Diameer The able above gives he measuremens of he B(x)
More informationt is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...
Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger
More informationSome Basic Information about M-S-D Systems
Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,
More information2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes
Some common engineering funcions 2.7 Inroducion This secion provides a caalogue of some common funcions ofen used in Science and Engineering. These include polynomials, raional funcions, he modulus funcion
More informationChristos Papadimitriou & Luca Trevisan November 22, 2016
U.C. Bereley CS170: Algorihms Handou LN-11-22 Chrisos Papadimiriou & Luca Trevisan November 22, 2016 Sreaming algorihms In his lecure and he nex one we sudy memory-efficien algorihms ha process a sream
More informationDisplacement ( x) x x x
Kinemaics Kinemaics is he branch of mechanics ha describes he moion of objecs wihou necessarily discussing wha causes he moion. 1-Dimensional Kinemaics (or 1- Dimensional moion) refers o moion in a sraigh
More informationSolutions to Odd Number Exercises in Chapter 6
1 Soluions o Odd Number Exercises in 6.1 R y eˆ 1.7151 y 6.3 From eˆ ( T K) ˆ R 1 1 SST SST SST (1 R ) 55.36(1.7911) we have, ˆ 6.414 T K ( ) 6.5 y ye ye y e 1 1 Consider he erms e and xe b b x e y e b
More informationTwo Coupled Oscillators / Normal Modes
Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own
More informationSolutions from Chapter 9.1 and 9.2
Soluions from Chaper 9 and 92 Secion 9 Problem # This basically boils down o an exercise in he chain rule from calculus We are looking for soluions of he form: u( x) = f( k x c) where k x R 3 and k is
More informationAnalyze patterns and relationships. 3. Generate two numerical patterns using AC
envision ah 2.0 5h Grade ah Curriculum Quarer 1 Quarer 2 Quarer 3 Quarer 4 andards: =ajor =upporing =Addiional Firs 30 Day 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 andards: Operaions and Algebraic Thinking
More informationMOMENTUM CONSERVATION LAW
1 AAST/AEDT AP PHYSICS B: Impulse and Momenum Le us run an experimen: The ball is moving wih a velociy of V o and a force of F is applied on i for he ime inerval of. As he resul he ball s velociy changes
More informationWednesday, November 7 Handout: Heteroskedasticity
Amhers College Deparmen of Economics Economics 360 Fall 202 Wednesday, November 7 Handou: Heeroskedasiciy Preview Review o Regression Model o Sandard Ordinary Leas Squares (OLS) Premises o Esimaion Procedures
More informationNotes on Kalman Filtering
Noes on Kalman Filering Brian Borchers and Rick Aser November 7, Inroducion Daa Assimilaion is he problem of merging model predicions wih acual measuremens of a sysem o produce an opimal esimae of he curren
More informationTesting What You Know Now
Tesing Wha You Know Now To bes each you, I need o know wha you know now Today we ake a well-esablished quiz ha is designed o ell me his To encourage you o ake he survey seriously, i will coun as a clicker
More informationModule 2 F c i k c s la l w a s o s f dif di fusi s o i n
Module Fick s laws of diffusion Fick s laws of diffusion and hin film soluion Adolf Fick (1855) proposed: d J α d d d J (mole/m s) flu (m /s) diffusion coefficien and (mole/m 3 ) concenraion of ions, aoms
More informationACE 562 Fall Lecture 4: Simple Linear Regression Model: Specification and Estimation. by Professor Scott H. Irwin
ACE 56 Fall 005 Lecure 4: Simple Linear Regression Model: Specificaion and Esimaion by Professor Sco H. Irwin Required Reading: Griffihs, Hill and Judge. "Simple Regression: Economic and Saisical Model
More informationUNC resolution Uncertainty Learning Objectives: measurement interval ( You will turn in two worksheets and
UNC Uncerainy revised Augus 30, 017 Learning Objecives: During his lab, you will learn how o 1. esimae he uncerainy in a direcly measured quaniy.. esimae he uncerainy in a quaniy ha is calculaed from quaniies
More informationAcceleration. Part I. Uniformly Accelerated Motion: Kinematics & Geometry
Acceleraion Team: Par I. Uniformly Acceleraed Moion: Kinemaics & Geomery Acceleraion is he rae of change of velociy wih respec o ime: a dv/d. In his experimen, you will sudy a very imporan class of moion
More informationEstimation of Poses with Particle Filters
Esimaion of Poses wih Paricle Filers Dr.-Ing. Bernd Ludwig Chair for Arificial Inelligence Deparmen of Compuer Science Friedrich-Alexander-Universiä Erlangen-Nürnberg 12/05/2008 Dr.-Ing. Bernd Ludwig (FAU
More informationd = ½(v o + v f) t distance = ½ (initial velocity + final velocity) time
BULLSEYE Lab Name: ANSWER KEY Dae: Pre-AP Physics Lab Projecile Moion Weigh = 1 DIRECTIONS: Follow he insrucions below, build he ramp, ake your measuremens, and use your measuremens o make he calculaions
More informationHamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t
M ah 5 2 7 Fall 2 0 0 9 L ecure 1 0 O c. 7, 2 0 0 9 Hamilon- J acobi Equaion: Explici Formulas In his lecure we ry o apply he mehod of characerisics o he Hamilon-Jacobi equaion: u + H D u, x = 0 in R n
More informationCSE 3802 / ECE Numerical Methods in Scientific Computation. Jinbo Bi. Department of Computer Science & Engineering
CSE 3802 / ECE 3431 Numerical Mehods in Scienific Compuaion Jinbo Bi Deparmen of Compuer Science & Engineering hp://www.engr.uconn.edu/~jinbo 1 Ph.D in Mahemaics The Insrucor Previous professional experience:
More informationFinal Spring 2007
.615 Final Spring 7 Overview The purpose of he final exam is o calculae he MHD β limi in a high-bea oroidal okamak agains he dangerous n = 1 exernal ballooning-kink mode. Effecively, his corresponds o
More informationDecimal moved after first digit = 4.6 x Decimal moves five places left SCIENTIFIC > POSITIONAL. a) g) 5.31 x b) 0.
PHYSICS 20 UNIT 1 SCIENCE MATH WORKSHEET NAME: A. Sandard Noaion Very large and very small numbers are easily wrien using scienific (or sandard) noaion, raher han decimal (or posiional) noaion. Sandard
More information04. Kinetics of a second order reaction
4. Kineics of a second order reacion Imporan conceps Reacion rae, reacion exen, reacion rae equaion, order of a reacion, firs-order reacions, second-order reacions, differenial and inegraed rae laws, Arrhenius
More informationSuggested Practice Problems (set #2) for the Physics Placement Test
Deparmen of Physics College of Ars and Sciences American Universiy of Sharjah (AUS) Fall 014 Suggesed Pracice Problems (se #) for he Physics Placemen Tes This documen conains 5 suggesed problems ha are
More informationSimulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010
Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid
More information2002 November 14 Exam III Physics 191
November 4 Exam III Physics 9 Physical onsans: Earh s free-fall acceleraion = g = 9.8 m/s ircle he leer of he single bes answer. quesion is worh poin Each 3. Four differen objecs wih masses: m = kg, m
More informationSub Module 2.6. Measurement of transient temperature
Mechanical Measuremens Prof. S.P.Venkaeshan Sub Module 2.6 Measuremen of ransien emperaure Many processes of engineering relevance involve variaions wih respec o ime. The sysem properies like emperaure,
More informationACE 562 Fall Lecture 8: The Simple Linear Regression Model: R 2, Reporting the Results and Prediction. by Professor Scott H.
ACE 56 Fall 5 Lecure 8: The Simple Linear Regression Model: R, Reporing he Resuls and Predicion by Professor Sco H. Irwin Required Readings: Griffihs, Hill and Judge. "Explaining Variaion in he Dependen
More informationMath 221: Mathematical Notation
Mah 221: Mahemaical Noaion Purpose: One goal in any course is o properly use he language o ha subjec. These noaions summarize some o he major conceps and more diicul opics o he uni. Typing hem helps you
More informationWEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x
WEEK-3 Reciaion PHYS 131 Ch. 3: FOC 1, 3, 4, 6, 14. Problems 9, 37, 41 & 71 and Ch. 4: FOC 1, 3, 5, 8. Problems 3, 5 & 16. Feb 8, 018 Ch. 3: FOC 1, 3, 4, 6, 14. 1. (a) The horizonal componen of he projecile
More informationGround Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan
Ground Rules PC11 Fundamenals of Physics I Lecures 3 and 4 Moion in One Dimension A/Prof Tay Seng Chuan 1 Swich off your handphone and pager Swich off your lapop compuer and keep i No alking while lecure
More informationLet us start with a two dimensional case. We consider a vector ( x,
Roaion marices We consider now roaion marices in wo and hree dimensions. We sar wih wo dimensions since wo dimensions are easier han hree o undersand, and one dimension is a lile oo simple. However, our
More informationLecture 33: November 29
36-705: Inermediae Saisics Fall 2017 Lecurer: Siva Balakrishnan Lecure 33: November 29 Today we will coninue discussing he boosrap, and hen ry o undersand why i works in a simple case. In he las lecure
More informationIn this chapter the model of free motion under gravity is extended to objects projected at an angle. When you have completed it, you should
Cambridge Universiy Press 978--36-60033-7 Cambridge Inernaional AS and A Level Mahemaics: Mechanics Coursebook Excerp More Informaion Chaper The moion of projeciles In his chaper he model of free moion
More informationPhysics 2107 Moments of Inertia Experiment 1
Physics 107 Momens o Ineria Experimen 1 Prelab 1 Read he ollowing background/seup and ensure you are amiliar wih he heory required or he experimen. Please also ill in he missing equaions 5, 7 and 9. Background/Seup
More informationTime series Decomposition method
Time series Decomposiion mehod A ime series is described using a mulifacor model such as = f (rend, cyclical, seasonal, error) = f (T, C, S, e) Long- Iner-mediaed Seasonal Irregular erm erm effec, effec,
More information1. Kinematics I: Position and Velocity
1. Kinemaics I: Posiion and Velociy Inroducion The purpose of his eperimen is o undersand and describe moion. We describe he moion of an objec by specifying is posiion, velociy, and acceleraion. In his
More informationMathcad Lecture #8 In-class Worksheet Curve Fitting and Interpolation
Mahcad Lecure #8 In-class Workshee Curve Fiing and Inerpolaion A he end of his lecure, you will be able o: explain he difference beween curve fiing and inerpolaion decide wheher curve fiing or inerpolaion
More informationEE100 Lab 3 Experiment Guide: RC Circuits
I. Inroducion EE100 Lab 3 Experimen Guide: A. apaciors A capacior is a passive elecronic componen ha sores energy in he form of an elecrosaic field. The uni of capaciance is he farad (coulomb/vol). Pracical
More informationCHEAPEST PMT ONLINE TEST SERIES AIIMS/NEET TOPPER PREPARE QUESTIONS
CHEAPEST PMT ONLINE TEST SERIES AIIMS/NEET TOPPER PREPARE QUESTIONS For more deails see las page or conac @aimaiims.in Physics Mock Tes Paper AIIMS/NEET 07 Physics 06 Saurday Augus 0 Uni es : Moion in
More informationThe Influence of Gravitation on the Speed of Light and an Explanation of the Pioneer 10 & 11 Acceleration Anomaly
www.ccsene.org/apr Applied Physics Research Vol. 3, No. 2; November 2011 The Influence of Graviaion on he Speed of Ligh and an Explanaion of he Pioneer 10 & 11 Acceleraion Anomaly Gocho V. Sharlanov Sara
More informationChapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws
Chaper 5: Phenomena Phenomena: The reacion (aq) + B(aq) C(aq) was sudied a wo differen emperaures (98 K and 35 K). For each emperaure he reacion was sared by puing differen concenraions of he 3 species
More informationPhysics 20 Lesson 5 Graphical Analysis Acceleration
Physics 2 Lesson 5 Graphical Analysis Acceleraion I. Insananeous Velociy From our previous work wih consan speed and consan velociy, we know ha he slope of a posiion-ime graph is equal o he velociy of
More informationOscillations. Periodic Motion. Sinusoidal Motion. PHY oscillations - J. Hedberg
Oscillaions PHY 207 - oscillaions - J. Hedberg - 2017 1. Periodic Moion 2. Sinusoidal Moion 3. How do we ge his kind of moion? 4. Posiion - Velociy - cceleraion 5. spring wih vecors 6. he reference circle
More information1 Review of Zero-Sum Games
COS 5: heoreical Machine Learning Lecurer: Rob Schapire Lecure #23 Scribe: Eugene Brevdo April 30, 2008 Review of Zero-Sum Games Las ime we inroduced a mahemaical model for wo player zero-sum games. Any
More informationHOMEWORK # 2: MATH 211, SPRING Note: This is the last solution set where I will describe the MATLAB I used to make my pictures.
HOMEWORK # 2: MATH 2, SPRING 25 TJ HITCHMAN Noe: This is he las soluion se where I will describe he MATLAB I used o make my picures.. Exercises from he ex.. Chaper 2.. Problem 6. We are o show ha y() =
More informationInnova Junior College H2 Mathematics JC2 Preliminary Examinations Paper 2 Solutions 0 (*)
Soluion 3 x 4x3 x 3 x 0 4x3 x 4x3 x 4x3 x 4x3 x x 3x 3 4x3 x Innova Junior College H Mahemaics JC Preliminary Examinaions Paper Soluions 3x 3 4x 3x 0 4x 3 4x 3 0 (*) 0 0 + + + - 3 3 4 3 3 3 3 Hence x or
More informationk 1 k 2 x (1) x 2 = k 1 x 1 = k 2 k 1 +k 2 x (2) x k series x (3) k 2 x 2 = k 1 k 2 = k 1+k 2 = 1 k k 2 k series
Final Review A Puzzle... Consider wo massless springs wih spring consans k 1 and k and he same equilibrium lengh. 1. If hese springs ac on a mass m in parallel, hey would be equivalen o a single spring
More information1. VELOCITY AND ACCELERATION
1. VELOCITY AND ACCELERATION 1.1 Kinemaics Equaions s = u + 1 a and s = v 1 a s = 1 (u + v) v = u + as 1. Displacemen-Time Graph Gradien = speed 1.3 Velociy-Time Graph Gradien = acceleraion Area under
More informationMATHEMATICAL DESCRIPTION OF THEORETICAL METHODS OF RESERVE ECONOMY OF CONSIGNMENT STORES
MAHEMAICAL DESCIPION OF HEOEICAL MEHODS OF ESEVE ECONOMY OF CONSIGNMEN SOES Péer elek, József Cselényi, György Demeer Universiy of Miskolc, Deparmen of Maerials Handling and Logisics Absrac: Opimizaion
More informationSTRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN
Inernaional Journal of Applied Economerics and Quaniaive Sudies. Vol.1-3(004) STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN 001-004 OBARA, Takashi * Absrac The
More informationLab 10: RC, RL, and RLC Circuits
Lab 10: RC, RL, and RLC Circuis In his experimen, we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors. We will sudy he way volages and currens change in
More informationEquations of motion for constant acceleration
Lecure 3 Chaper 2 Physics I 01.29.2014 Equaions of moion for consan acceleraion Course websie: hp://faculy.uml.edu/andriy_danylo/teaching/physicsi Lecure Capure: hp://echo360.uml.edu/danylo2013/physics1spring.hml
More informationR t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t
Exercise 7 C P = α + β R P + u C = αp + βr + v (a) (b) C R = α P R + β + w (c) Assumpions abou he disurbances u, v, w : Classical assumions on he disurbance of one of he equaions, eg. on (b): E(v v s P,
More informationPredator - Prey Model Trajectories and the nonlinear conservation law
Predaor - Prey Model Trajecories and he nonlinear conservaion law James K. Peerson Deparmen of Biological Sciences and Deparmen of Mahemaical Sciences Clemson Universiy Ocober 28, 213 Ouline Drawing Trajecories
More information72 Calculus and Structures
72 Calculus and Srucures CHAPTER 5 DISTANCE AND ACCUMULATED CHANGE Calculus and Srucures 73 Copyrigh Chaper 5 DISTANCE AND ACCUMULATED CHANGE 5. DISTANCE a. Consan velociy Le s ake anoher look a Mary s
More informationZürich. ETH Master Course: L Autonomous Mobile Robots Localization II
Roland Siegwar Margaria Chli Paul Furgale Marco Huer Marin Rufli Davide Scaramuzza ETH Maser Course: 151-0854-00L Auonomous Mobile Robos Localizaion II ACT and SEE For all do, (predicion updae / ACT),
More informationKriging Models Predicting Atrazine Concentrations in Surface Water Draining Agricultural Watersheds
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 Kriging Models Predicing Arazine Concenraions in Surface Waer Draining Agriculural Waersheds Paul L. Mosquin, Jeremy Aldworh, Wenlin Chen Supplemenal Maerial Number
More informationAP Physics 1 - Summer Assignment
AP Physics 1 - Summer Assignmen This assignmen is due on he firs day of school. You mus show all your work in all seps. Do no wai unil he las minue o sar his assignmen. This maerial will help you wih he
More informationToday: Falling. v, a
Today: Falling. v, a Did you ge my es email? If no, make sure i s no in your junk box, and add sbs0016@mix.wvu.edu o your address book! Also please email me o le me know. I will be emailing ou pracice
More informationI. OBJECTIVE OF THE EXPERIMENT.
I. OBJECTIVE OF THE EXPERIMENT. Swissmero raels a high speeds hrough a unnel a low pressure. I will hereore undergo ricion ha can be due o: ) Viscosiy o gas (c. "Viscosiy o gas" eperimen) ) The air in
More informationRC, RL and RLC circuits
Name Dae Time o Complee h m Parner Course/ Secion / Grade RC, RL and RLC circuis Inroducion In his experimen we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors.
More information!!"#"$%&#'()!"#&'(*%)+,&',-)./0)1-*23)
"#"$%&#'()"#&'(*%)+,&',-)./)1-*) #$%&'()*+,&',-.%,/)*+,-&1*#$)()5*6$+$%*,7&*-'-&1*(,-&*6&,7.$%$+*&%'(*8$&',-,%'-&1*(,-&*6&,79*(&,%: ;..,*&1$&$.$%&'()*1$$.,'&',-9*(&,%)?%*,('&5
More informationWeek 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem)
Week 1 Lecure Problems, 5 Wha if somehing oscillaes wih no obvious spring? Wha is ω? (problem se problem) Sar wih Try and ge o SHM form E. Full beer can in lake, oscillaing F = m & = ge rearrange: F =
More informationAcceleration. Part I. Uniformly Accelerated Motion: Kinematics & Geometry
Acceleraion Team: Par I. Uniformly Acceleraed Moion: Kinemaics & Geomery Acceleraion is he rae of change of velociy wih respec o ime: a dv/d. In his experimen, you will sudy a very imporan class of moion
More information2. Nonlinear Conservation Law Equations
. Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear
More informationThe average rate of change between two points on a function is d t
SM Dae: Secion: Objecive: The average rae of change beween wo poins on a funcion is d. For example, if he funcion ( ) represens he disance in miles ha a car has raveled afer hours, hen finding he slope
More informationInterpretation of special relativity as applied to earth-centered locally inertial
Inerpreaion of special relaiviy as applied o earh-cenered locally inerial coordinae sysems in lobal osiioning Sysem saellie experimens Masanori Sao Honda Elecronics Co., Ld., Oyamazuka, Oiwa-cho, Toyohashi,
More informationPhysics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution
Physics 7b: Saisical Mechanics Fokker-Planck Equaion The Langevin equaion approach o he evoluion of he velociy disribuion for he Brownian paricle migh leave you uncomforable. A more formal reamen of his
More informationAP Physics 1 - Summer Assignment
AP Physics 1 - Summer Assignmen This assignmen is due on he firs day of school. You mus show all your work in all seps. Do no wai unil he las minue o sar his assignmen. This maerial will help you wih he
More informationNavneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi
Creep in Viscoelasic Subsances Numerical mehods o calculae he coefficiens of he Prony equaion using creep es daa and Herediary Inegrals Mehod Navnee Saini, Mayank Goyal, Vishal Bansal (23); Term Projec
More informationObject tracking: Using HMMs to estimate the geographical location of fish
Objec racking: Using HMMs o esimae he geographical locaion of fish 02433 - Hidden Markov Models Marin Wæver Pedersen, Henrik Madsen Course week 13 MWP, compiled June 8, 2011 Objecive: Locae fish from agging
More informationTesting the Random Walk Model. i.i.d. ( ) r
he random walk heory saes: esing he Random Walk Model µ ε () np = + np + Momen Condiions where where ε ~ i.i.d he idea here is o es direcly he resricions imposed by momen condiions. lnp lnp µ ( lnp lnp
More informationFITTING EQUATIONS TO DATA
TANTON S TAKE ON FITTING EQUATIONS TO DATA CURRICULUM TIDBITS FOR THE MATHEMATICS CLASSROOM MAY 013 Sandard algebra courses have sudens fi linear and eponenial funcions o wo daa poins, and quadraic funcions
More information15. Vector Valued Functions
1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,
More informationUnit 1 Test Review Physics Basics, Movement, and Vectors Chapters 1-3
A.P. Physics B Uni 1 Tes Reiew Physics Basics, Moemen, and Vecors Chapers 1-3 * In sudying for your es, make sure o sudy his reiew shee along wih your quizzes and homework assignmens. Muliple Choice Reiew:
More informationRobotics I. April 11, The kinematics of a 3R spatial robot is specified by the Denavit-Hartenberg parameters in Tab. 1.
Roboics I April 11, 017 Exercise 1 he kinemaics of a 3R spaial robo is specified by he Denavi-Harenberg parameers in ab 1 i α i d i a i θ i 1 π/ L 1 0 1 0 0 L 3 0 0 L 3 3 able 1: able of DH parameers of
More information