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MEASUREMENT &
UNCERTAINTY
Estimating Uncertainties In
Experimental Results

   All experimental scientists need to know how
    well they can trust their results.
   The results of any experiment are only as valid as
    the degree of error in those results.
   A lot of time, effort , and money has been spent
    by scientists developing more “accurate”
    machines to measure events more precisely.
   This unit is all about making and keeping tracks
    of errors during experimental measurements.
Estimating Uncertainties In
Experimental Results
Examine the image show below:




  What is the diameter of the
  tennis ball in cm?            (answer: ~ 6.4 cm)
Estimating Uncertainties In
Experimental Results
  Does this mean it is exactly 6.4 cm?
  Could the diameter be 6.3 or 6.5 or even 6.44
    cm?




 Look again…
Estimating Uncertainties In
Experimental Results
  All measured values must be accompanied by an
  estimate of the error or uncertainty associated
  with the measured value.
  The tennis ball has a diameter of

                     6.4 + 0.1 cm.


    Measurement value                Estimated error value
Estimating Uncertainties In
Experimental Results
 Let’s look at some other possible ways of trying
   to report this value:

 6.4 + 0.15 cm        What is inconsistent here?



  6 + 0.1 cm           What is inconsistent here?


 6.42 + 1 cm           What is inconsistent here?
Estimating Uncertainties In
Experimental Results

  So what does 6.4 + 0.1 cm really mean?

  The real or actual diameter of the tennis ball lies
  between a maximum and a minimum value.
                                      The actual value lies
  Maximum value:          6.5 cm      somewhere in between
                                      these two values!

   Minimum value:         6.3 cm      We can not be any
                                      more precise than
                                      this!
Estimating Uncertainties In
Experimental Results
Types of Errors:
Measurement errors fall into two main types:

   Systematic errors:
        These errors consistently influence a set of
        measurements in a particular direction , either too
        high or too low.

        These errors are associated with the precision of the
        measuring device (eg. not calibrated correctly), or
        errors in experimental procedures.
Estimating Uncertainties In
Experimental Results
    Random errors:
         These errors arise due to fluctuations in the
         experimental conditions or in the judgment of the
         experimenter.
         These errors are random, some being too high while
         others being too low and tend to average out if the
         experimenter repeats the experiment often enough.

After you have identified the factors that may influence your
results in the collection of experimental results, it is important to
design strategies to minimize both of these two types of errors.
Estimating Uncertainties In
Experimental Results
Think:
  Drop a tennis ball from some height allowing it
  to hit the ground and measure the height to
  which it rebounds to.

   1) Think and discuss all of the factors that could
      affect the outcome.
   2) Think and discuss all of the possible error sources
      including both Systematic and Random.
Estimating Uncertainties In
Experimental Results
 Dealing with errors:
    Adding and Subtracting Measured Values:

A student measures the mass of a          123.4 + 0.1 g
beaker + copper to be :
 A student measures the mass of a
 beaker to be :                           113.8 + 0.1 g

 Mass of Copper is:                          9.6 + ? g


  But what about the uncertainty? What happens to it? Does it
  stay at 0.1? Or does change to a higher or lower number?
Estimating Uncertainties In
Experimental Results
The rule is:
  When adding or subtracting numbers the
  numerical uncertainty is simply added!

 In order to determine the mass of copper the student
 subtracted two measured values: therefore simply
 add the numerical error!


  Mass of Copper is:                      9.6 + 0.2 g


                             Numerical error
Estimating Uncertainties In
Experimental Results
 Now try these:
4.5 + 0.2 m + 2.3 + 0.1m + 6.3 + 0.3 m =              13.1 + 0.6 m


 67.9 + 0.2 g - 45.7 + 0.2 g =         22.2 + 0.4 g


 (34.5 + 0.2 cm) + (12.3 + 0.3 cm) - (14.3 + 0.2 cm) =

                                             32.5 + 0.7 cm

 (1.5 + 0.5 m) - (4.3 + 0.5 m) + (8.8 + 0.3 m) =          6+1m
Estimating Uncertainties In
Experimental Results
Multiplying or Dividing Measured Values:
 This becomes a little more complicated.

The rule is:
When measured values are multiplied or divided the percentage
errors are added.

 What is a percentage error?


    Answer: a numerical error changed to be represented as a
    percentage of the measured value
Estimating Uncertainties In
Experimental Results
How is this done?
   Easily:
             Remember the copper:

 Mass of Copper is:   9.6 + 0.2 g

                      0.2
  Percent error =                   X 100   = 2%
                      9.6


 Mass of Copper is:   9.6 + 2 % g
Estimating Uncertainties In
Experimental Results
Formula for finding Percentage Error:



                      Numerical Error
 Percentage error =                     X 100
                      Measured Value
Estimating Uncertainties In
Experimental Results
 Now try These:
 Change numerical to percentage error:

 13.1 + 0.6 m              13.1 + 5 % m

  22.2 + 0.4 g             22.2 + 2 % g

  32.5 + 0.7 cm            32.5 + 2 % cm

   6+1m                     6 + 17 % m
Estimating Uncertainties In
Experimental Results
Now try these:
  Remember when measured values are multiplied
  or divided, add the percentage errors!

  1) 22.2 cm + 2 % x 45.2 cm + 5% =         1000 cm2 + 7 %

  2) 2.31 g + 2 % ÷ 0.76 mL + 3% =      3.0 g/mL + 5 %

  3) 45 + 1 m x 342 + 3 m =            15400 m2 + 3 %

 4) {(2.2 cm + 2 % x 5.4 cm + 5%) + 14 + 0.3 cm2} =
           Careful on this last one!
                                          26 + 1 cm2
Estimating Uncertainties In
Experimental Results
How to determine the numerical error?
 1) Reading a scale:
    • Use ½ of the smallest division
 2) Fluctuating scale:
    • Look at the range of fluctuations and
       divide by 2
   •   1/2(maximum value – minimum error)
Estimating Uncertainties In
Experimental Results
Graduated Cylinder




                     Volume = 12.3 + 0.3 mL
           13
           12
           11
           10


                          Fill water up to this point

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Measurement & uncertainty pp presentation

  • 2. Estimating Uncertainties In Experimental Results  All experimental scientists need to know how well they can trust their results.  The results of any experiment are only as valid as the degree of error in those results.  A lot of time, effort , and money has been spent by scientists developing more “accurate” machines to measure events more precisely.  This unit is all about making and keeping tracks of errors during experimental measurements.
  • 3. Estimating Uncertainties In Experimental Results Examine the image show below: What is the diameter of the tennis ball in cm? (answer: ~ 6.4 cm)
  • 4. Estimating Uncertainties In Experimental Results  Does this mean it is exactly 6.4 cm?  Could the diameter be 6.3 or 6.5 or even 6.44 cm? Look again…
  • 5. Estimating Uncertainties In Experimental Results All measured values must be accompanied by an estimate of the error or uncertainty associated with the measured value. The tennis ball has a diameter of 6.4 + 0.1 cm. Measurement value Estimated error value
  • 6. Estimating Uncertainties In Experimental Results Let’s look at some other possible ways of trying to report this value: 6.4 + 0.15 cm What is inconsistent here? 6 + 0.1 cm What is inconsistent here? 6.42 + 1 cm What is inconsistent here?
  • 7. Estimating Uncertainties In Experimental Results So what does 6.4 + 0.1 cm really mean? The real or actual diameter of the tennis ball lies between a maximum and a minimum value. The actual value lies Maximum value: 6.5 cm somewhere in between these two values! Minimum value: 6.3 cm We can not be any more precise than this!
  • 8. Estimating Uncertainties In Experimental Results Types of Errors: Measurement errors fall into two main types: Systematic errors: These errors consistently influence a set of measurements in a particular direction , either too high or too low. These errors are associated with the precision of the measuring device (eg. not calibrated correctly), or errors in experimental procedures.
  • 9. Estimating Uncertainties In Experimental Results Random errors: These errors arise due to fluctuations in the experimental conditions or in the judgment of the experimenter. These errors are random, some being too high while others being too low and tend to average out if the experimenter repeats the experiment often enough. After you have identified the factors that may influence your results in the collection of experimental results, it is important to design strategies to minimize both of these two types of errors.
  • 10. Estimating Uncertainties In Experimental Results Think: Drop a tennis ball from some height allowing it to hit the ground and measure the height to which it rebounds to. 1) Think and discuss all of the factors that could affect the outcome. 2) Think and discuss all of the possible error sources including both Systematic and Random.
  • 11. Estimating Uncertainties In Experimental Results Dealing with errors: Adding and Subtracting Measured Values: A student measures the mass of a 123.4 + 0.1 g beaker + copper to be : A student measures the mass of a beaker to be : 113.8 + 0.1 g Mass of Copper is: 9.6 + ? g But what about the uncertainty? What happens to it? Does it stay at 0.1? Or does change to a higher or lower number?
  • 12. Estimating Uncertainties In Experimental Results The rule is: When adding or subtracting numbers the numerical uncertainty is simply added! In order to determine the mass of copper the student subtracted two measured values: therefore simply add the numerical error! Mass of Copper is: 9.6 + 0.2 g Numerical error
  • 13. Estimating Uncertainties In Experimental Results Now try these: 4.5 + 0.2 m + 2.3 + 0.1m + 6.3 + 0.3 m = 13.1 + 0.6 m 67.9 + 0.2 g - 45.7 + 0.2 g = 22.2 + 0.4 g (34.5 + 0.2 cm) + (12.3 + 0.3 cm) - (14.3 + 0.2 cm) = 32.5 + 0.7 cm (1.5 + 0.5 m) - (4.3 + 0.5 m) + (8.8 + 0.3 m) = 6+1m
  • 14. Estimating Uncertainties In Experimental Results Multiplying or Dividing Measured Values: This becomes a little more complicated. The rule is: When measured values are multiplied or divided the percentage errors are added. What is a percentage error? Answer: a numerical error changed to be represented as a percentage of the measured value
  • 15. Estimating Uncertainties In Experimental Results How is this done? Easily: Remember the copper: Mass of Copper is: 9.6 + 0.2 g 0.2 Percent error = X 100 = 2% 9.6 Mass of Copper is: 9.6 + 2 % g
  • 16. Estimating Uncertainties In Experimental Results Formula for finding Percentage Error: Numerical Error Percentage error = X 100 Measured Value
  • 17. Estimating Uncertainties In Experimental Results Now try These: Change numerical to percentage error: 13.1 + 0.6 m 13.1 + 5 % m 22.2 + 0.4 g 22.2 + 2 % g 32.5 + 0.7 cm 32.5 + 2 % cm 6+1m 6 + 17 % m
  • 18. Estimating Uncertainties In Experimental Results Now try these: Remember when measured values are multiplied or divided, add the percentage errors! 1) 22.2 cm + 2 % x 45.2 cm + 5% = 1000 cm2 + 7 % 2) 2.31 g + 2 % ÷ 0.76 mL + 3% = 3.0 g/mL + 5 % 3) 45 + 1 m x 342 + 3 m = 15400 m2 + 3 % 4) {(2.2 cm + 2 % x 5.4 cm + 5%) + 14 + 0.3 cm2} = Careful on this last one! 26 + 1 cm2
  • 19. Estimating Uncertainties In Experimental Results How to determine the numerical error? 1) Reading a scale: • Use ½ of the smallest division 2) Fluctuating scale: • Look at the range of fluctuations and divide by 2 • 1/2(maximum value – minimum error)
  • 20. Estimating Uncertainties In Experimental Results Graduated Cylinder Volume = 12.3 + 0.3 mL 13 12 11 10 Fill water up to this point