introduction to fundamental physics laboratory lecture i
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Introduction to Fundamental Physics Laboratory Lecture I. Dr. Yongkang Le March 5 th , 20 10 http://phylab.fudan.edu.cn/doku.php?id=course:fund_phy_exp:start. For share. In science, there is only physics. All the rest is stamp collecting. By Ernest Rutherford - PowerPoint PPT PresentationTRANSCRIPT
Introduction toIntroduction toFundamental Physics LaboratoryFundamental Physics Laboratory
Lecture ILecture I
Dr. Yongkang LeDr. Yongkang LeMarch 5March 5thth, 2010, 2010
http://phylab.fudan.edu.cn/doku.php?id=course:fund_phy_exp:starthttp://phylab.fudan.edu.cn/doku.php?id=course:fund_phy_exp:start
For shareFor share
☺ In science, there is only physics. All the rest is stamp collecting.
By Ernest Rutherford
☺ Experiments are the only means of knowledge at our disposal. The
rest is poetry, imagination. By Max Plank
ContentContent
Introduction Arrangement Importance of physics experiment Error and uncertainty Significance digit Uncertainty estimation
IntroductionIntroduction Name: Fundamental Physics Laboratory Course duration: ~3 hours Credit: 2 Content: 2 lectures, 8 labs, 4 discussion
and final test (oral) Marking: labs and discussions 70%
test 30% Supervisors: Mrs. Weifeng Su and Dr. Le
ArrangementArrangement Each group two students (Registration on web)
Unit 1 Unit 2 Unit 3 Unit 4
1,2 W 3-8 W 9,12-16 W 17 W
2 Lec.
H.W.
Mech.+Ele.
4 Labs+2 Dis.
Th. + Op.+Mod.
4 Labs+2 Dis.Test
Phy.403 GH Bld. GH Bld.+Phy. Bld N/A
Le Le+Su Le+Su Le+Su
PurposePurpose Support the learning and understanding of basi
c physical principles Assist acquirement of basic techniques for han
dling the practical problems To be familiar with the experimental research on the
physical phenomena How to design an experiment to reach the proposed
objective How to analyze the experimental data and the errors How to report what you obtain a physical experiment
to others
Importance of physics experimentImportance of physics experiment
Historical view Classical Physics Development of modern physics
Support to other fields Statistic of Nobel Prize
Real Experiment can not be perfect Most laws are quantitative relationship
F=ma Criterion and convertion
c = (299792.50±0.10) km/s
• Data processingNormative calculation and expression
To derive :Quantitative law and reliable conclusion
Error and UncertaintyError and Uncertainty Error:
Difference between measured value
and true value Origin:
Method—— Error Devices Operator: estimation
Uncertainty
Measuring the length of an object
Left end: 10.00cmRight end: 15.25cm
Display of a digital ammeter
1. When the display is stable: 3.888A
2. How about when the display is instable?
Two ExamplesTwo Examples
Uncertainty estimationUncertainty estimation‘‘Guide to the Expression of Uncertainty in Measurement ISO 1993
(E)”
from BIPM and ISO etc., issued in 1993
Uncertainty--Distribution property of measured results
Important: too large--waste; too small--wrong。
Two Type :
Type A--- Evaluated with statistical methods
Type B---Evaluated with other methods
Uncertainty type AUncertainty type AAfter n time same measurement of unknown x:
uA decreases with increasing n
where
Uncertainty type BUncertainty type B From measurement(For single measurement):
From device:
2B
au
c
Best situation
In case
Worst situation
d: smallest deviation
uB2=a/3 : Average distribution, uB2=a/3 : normal distribution, large na: maximum uncertainty of the device, usually given with the device
Combination of Combination of UncertaintyUncertaintySingle measurement:
)()()( 22
21 xuxuxu BB
)()()()( 222
211
21 xuxuxuxu BBB
2 22( ) ( ) ( )A Bu x u x u x
For length measurements, since x=x2-x1, we have:
Multiple measurements(n>=5):
Expression of the resultsExpression of the results
1 、 Usually : e.g., L = 1.05±0.02 cm.
2 、 Percentage expression of the uncertainty :
e.g. , L =1.05cm , percentage uncertainty 2% .
3 、 Use significant figures to indicate the uncertainty
e.g. L =1.05cm, uL ~ 0.01cm (not specified)
)(xux
%100)(
x
xu
Significant figuresSignificant figuresAll digits from first nonzero digit: e.g. 0.35 (2); 3.54 (3); 0.003540 (4); 3.5400 (5) 。
Uncertainty is usually given in one digit(max 2). Results should has the last digit same as the uncertainty.i.e. : The last digit of the result is uncertain.
Rounding : 4 - abandon 6 - rounding 5 - rounding for even end e.g. , x=3.54835 or 3.65325
If ux=0.0003, then x=3.5484; 3.6532
If ux=0.002, then x=3.548 ; 3.653
If ux=0.04, then x=3.55; 3.65
If ux=0.1, then x=3.5; 3.7
5 - rounding for even end
abandon rounding
Rule in calculationRule in calculation+ , -: highst digits
57.31+ 0.0156- 2.24342( =55.08218) =55.08
* , / : minimum significant figures 57.31×0.0156÷2.24342( =0.398514767) =0.399
If the results is calculated:
+ , - : * , / : xn:
General equation: Measured quantities are independ from each other
22)()(
x
xun
y
yunxy
Propagation of UncertaintyPropagation of Uncertainty
or
Example: Density of a metal cylinder Mass measured with an electronic balance:
M=80.36g, d =0.01g, a =0.02g.Height measure with a ruler:H= H2- H1, where H1= 4.00cm,
H2= 19.32cm; d =0.1cm, uB1 =d /5; a =0.01cm.Diameter measure with a slide callipers (D data are given in the table); d =0.002cm; a =0.002cm。
Please calculate the density and its uncertainty.
D/cm2.014 2.018 2.016 2.020 2.018
2.018 2.020 2.022 2.016 2.020
Uncertainty estimation:For mass:
g015.0g3
02.001.0))(())(()(2
222
21
MuMuMu BB
cm32.15cm)00.432.19(12 HHH
cm029.0cm3
01.002.02)()(2)(2
222
21
HuHuHu BB
cm0184.210
1 10
1
i
iDD
cm00078.0 )110(10
)()(
10
1
2
i
i
A
DDDu
cm0014.0cm3
002.0)00078.0())(())(()(2
222
2
DuDuDu BA
For height:
Average value of the diameter:
3322 cmg639.1
cmg
32.15)0184.2(1416.3
36.8044
HD
M
V
M
222)()(
2)()(
H
Hu
D
Du
M
Muu
2 2 2
0.015 0.0014 0.0292
80.36 2.0184 15.32
33 cmg004.0
cmg639.1%24.0
)()(
u
u
33
3 mkg10)004.0639.1(
cmg)004.0639.1()( u
%24.01058.31092.11048.3 668
Results:
Density :
Question?Question?
Thank you!Thank you!
Homework: see the webpageHomework: see the webpage