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DATA HANDLING AND
MEASUREMENT
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With every measurement,no matter how carefully it ismade, there is an
associated error anduncertainty inherent withthe measurement
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The magnitude of the erroris due to the precision ofthe measuring device, the
proper calibration of thedevice, and the competentapplication of the device
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Random ErrorIf you measure a quantity many times
and get lots of slightly different
readings then this called a random
error.For example, when measuring the
bounce of a ball it is very difficult to
get the same value every time even if
the ball is doing the same thing.
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Sources of random errors include:The readability of the instrument
The observer being less thanperfectThe effects of change in the
surroundings
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Systematic Error
This is when there is somethingwrong with the measuringdevice or method.
Using a ruler with a broken endcan lead to a zero error. Evenwith no random error in theresults, youd still get the wronganswer.
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Sources of systematic errors
include:
An instrument with zero error. To
correct for zero error, the valueshould be subtracted from every
reading
An instrument being wronglycalibrated
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Reducing Errors
To reduce random errors youcan repeat your measurements.
If the uncertainty is truly random,
they will lay either side of the true
reading and the mean of these
values will be close to the actual
value.
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To reduce a systematic error you
need to find out what is causing
it and correct yourmeasurements accordingly
Sometimes when you look at the
graph of your results
An accurate experiment is one
that has a small systematic error,
whereas a precise experiment is
one that has a small random
error.
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Estimate The Uncertainty Range
An uncertainty range applies toany experimental value.
The idea is that, instead of just
giving one value that implies
perfection, we give the likely range
of measurement.
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Uncertainties Representation.
Uncertainty can be written in 3
formats. If a value of a measurementis 6.25 m and the uncertainty is 0.05
cm, this uncertainty can be
represented in the forms below :
Absolute uncertainty : 6.25 0.05cm
Relative uncertainty : 6.25 (1.000.008) cm
Fractional (percentage) uncertainty: 6.25 (1.00 0.008) cm = 6.25
0.8%
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State uncertainties as absoluteuncertainties.
Add 1 of the smallest significantfigure.
13.21 m 0.010.002 g 0.001
1.2 s 0.1
12 V 1
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Determine the uncertainties in results.
The uncertainty in data is not enough, we
need to include it in any calculations we dowith the data.
Addition and subtraction
When performing additions and subtractions
we simply need to add together the absoluteuncertainties.
Example:
Add the values 1.2 0.1, 12.01 0.01, 7.21
0.011.2 + 12.01 + 7.21 = 20.42
0.1 + 0.01 + 0.01 = 0.12
20.42 0.12
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Graphical Representation of
Uncertainty
In many situations the best method of
presenting and analysing data is to use graph.
If this is the case, a neat way of representing
the uncertainties is to use error bars. The
graphs below explain their use.
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Error bars are a graphical representationof the variability of data and are used
on graphs to indicate the error, or
uncertainty in a reported measurement.
They give a general idea of how
accurate a measurement is.
http://en.wikipedia.org/wiki/Error%23Experimental_sciencehttp://en.wikipedia.org/wiki/Error%23Experimental_science7/30/2019 measuremt errorbar
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To add error bars to a point on a
graph, we simply take the
uncertainty range (expressed as" value" in the data) and drawlines of a corresponding size
above and below the point
depending on the axis the valuecorresponds to.
.
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Since the error bar represents the uncertainty
range,
the best-fit line of the graph should pass
through ALL of the error rectangles created by
the error bars
(ie. vertical error bar & horizontal error bar for
a graph point).
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Best-Fit" Line
The "best-fit" line is the straight line which
passes as near to as many of the pointsas possible.
By drawing such a line, we are
attempting to minimise the effects ofrandom errors in the measurements.
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Time 0.2 s Distance 2 m
3.4 135.1 36
7 64
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Determine the uncertainties in the
gradient Gradient
To calculate the uncertainty in the
gradient, we simply add error bars to the
first and last point, and then draw a
straight line passing through the lowest
error bar of the one points and the
highest in the other and vice versa.
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