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CHAPTER 3 NUMBERS AND PHYSICAL REALITY
How big are things and are they really changing?
Science depends on the comparison of theory with experiments; experiments depend on
measurements and measurements involve numbers. Likewise, theories are most reliably
expressed with numbers. Ultimately scientific decisions are made when someone compares the
numbers predicted by a scientific theory with the numbers produced in an experiment. Because
science often involves numbers and mathematics, we will develop enough mathematics to give
students an idea of how scientists view and use mathematics. We emphasize two things: 1)
numbers associated with experimental data (this chapter), and 2) the vocabulary and grammar of
the mathematical language used in theory (next chapter). These are central tools for science
literacy.
Expectations
When dealing with experimental data or theoretical calculations associated with physical
phenomena, we are always dealing with physical quantities that are expressed via numbers and
units. After completing this chapter, successful students are expected:
To recognize that there are two distinct ways in which numbers are used: discrete
counting and continuous measurements.
To develop basic skills as estimating quantities and understanding the role of units and
simple formulas in estimations.
To understand that numbers in science not only include the value and units, but also
an estimate of the error. To recognize the difference between precision and accuracy, and
why each is important. The successful student will also develop basic skills in estimating
errors.
To understand different sources of fluctuations in experiments and how scientists use
basic statistical quantities, such as mean and standard deviation, to quantify fluctuations.
To have a basic understanding of the importance of probability in describing physicalphenomena.
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3-A Numbers
Numbers appear in experimental measurements and in theoretical equations throughout the field
of physics, chemistry, biology, and engineering. Scientists generally work hard to see to it that
the numbers they use are as precise as is possible. William Thomson (later Lord Kelvin) is often
quoted as follows: When you can measure what you are speaking about, and express it innumbers, you know something about it; but when you cannot express it in numbers, your
knowledge is of a meager and unsatisfactory kind. Many scientists might believe that
Thomsons quote was an overstatement, but all would agree that numbers play a crucial role in
the success of science. As a science spectator, there are some basic features of numbers you need
to review, or recognize for the first time! The first issue is that numbers come in different types.
In everyday life, we dont spend a lot of time worrying about different types of numbers and
their accuracy explicitly. And yet, implicitly it shows up everywhere. When you arrange to meet
someone, because most peoples watches do not agree exactly, there is generally a 5 minute
rule, or some other range of allowed values that people could show up within and not be
late. However, as everyone switches to cell phone time that is tied to the same GPS system, the
range of allowed values may shrink! This is a great example of how the improvement in
technology (our tools) changes how we measure things. In contrast, when you are getting your
prescription filled, you expect the number of pills to be exact! There should be no error in this
case, because one pill too few is not acceptable and pills come in discrete units (each pill is its own
countable object). Just thinking about these everyday situations a little carefully suggests there is
even more to numbers than we usually think.
Therefore, it should be no surprise that scientists and mathematicians use a wide variety of types
of numbers. You probably learned about integers, whole numbers, rational numbers, real
numbers, and maybe even imaginary and complex numbers. For our purposes, it is useful to
categorize numbers found when describing nature as either countable or measurable. This is the
distinction we made between meeting at a certain time and counting out pills. It is a distinctionthat focuses on the degree of error associated with a particular quantity.
Countable quantities are generally expressed as integers (such as 1, 2, 3, ), and another word
that is often used for such quantities is discrete such as the number of pills you need. There are
cases where you can use fractions for discrete entities. For example, when using money, a half
dollar is an exact quantity and is considered countable. In physics, we find this in music, where
we can make waves that are exact fractions of a wavelength, or more esoterically, in quantum
mechanics where objects can possess a half integer spin value.
Measurable quantities are expressed as decimals and are generally associated with continuous
processes or situations such as telling time. Measurable numbers can never be exact
(completely free of error and uncertainty). Though we mentioned some special examples where
fractions were countable, they are more generally measurable quantities. Think of the classic
challenge of splitting a cookie between two people. Since it is almost impossible to split it exactly
in half, one person breaks and the other person chooses! This is an example of one half being
measurable and having an error associated with it.
It is worth mentioning a third category of numbers: defined numbers. These are quantities with a
very precise definition, such as the number which relates the radius and circumference of a
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circle. Most physical constants are in this category. Generally, these numbers have an exact value
inprinciple that is given by their definition, but in practice, we have to use an approximation for
these numbers.
Examples: Here are a few examples of different types of numbers.Measurable: 14.2 meters
Defined and exact: 3.14159 ....
(the famous Pi that relates the circumference and radius of circles)
Defined and countable: 5! (= 5 4 3 2 1 = 120)
(a mathematical operation calledfactorial).
Measurable: 3 x 102 kilograms
Countable: 47 eggs (or any other item you might count)
Why do we care about countable versus measurable numbers? The main reason is our interest inthe error in any given measurements. We will return to this concept in Section 3-C.
3-B. Estimations: how big are things?
A central skill for any science spectator is developing a feel for how big things are. For example, if
you were asked how big a typical sports stadium is, you should know that it is probably bigger
than 100 yards (the size of a football or soccer field, depending on the sport central to your
culture!) if it is going to fit a sports field. Also, it is probably not 100 times bigger than that. So,
adding some room for stands, you might guess 200 300 yards for the diameter. (Or, you might
guess something similar in meters if you prefer the metric system.) A quick search of some
typical stadiums finds dimensions in exactly this range. For example, the famous RomanCollosseum is basically 200 yard across. Notice, this estimate involves two key pieces: units and a
basic feel for the size of things.
Figure: When making an estimate, it can help to draw a quick
sketch. In this case, by drawing the field (rectangle in the center)
and the stands (gray area) roughly to scale, we see that our
estimate of 200 300 yards is quite reasonable.
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3-B.1. Units
In discussing numbers related to science, most people are aware that most numbers in science
come with units. People often complain about units and why do we even bother. But, as we
already pointed out, one of the most important science spectator skills is having an
understanding for the size of things that matters most! And this is a fundamental role of units they are associated with the size of something. Think of all the medical horror stories of people
receiving the wrong dosage because the units were wrong. After all, there is a big difference
between 2 mg and 2 g of the typical medicine. Another common example is a persons height. It
makes no sense to say that you are 6 tall. Is this 6 feet (which seems reasonable) or 6 inches
(which does not)? If you are in charge of a company and an employee predicts there will be a $2
million loss, you want to know is this expected in the next few days, years, or decade? Or, as
scientists would put it what is the time scale? Your response to the expected loss clearly depends
on how much time you have to deal with it. Finally, when considering variations in the climate,
you want to have a good idea of the time scale. Are the changes occurring over months, years,
decades, or centuries? Again, our response depends on this. Another way of saying all this is that
units provide the ability to determine what is large, small, fast or slow because ultimately these
concepts are only meaningful relative to some standard. The units tell us what standard we are
comparing to.
In addition to units telling us the scale of the measurement, units tell the kind of quantity being
measured. For the time being, we will start with three basic units (length, mass and time) that can
be used to construct all other physical units. The units for these quantities are called fundamental
units (discussed previously in Chapter 2). For example, the units of distance (a fundamental
quantity) can be meters, inches, feet, kilometers, and so on. Here we see the two uses of units
coming together. If scale (the size of things) did not matter, we would have just one unit for
length, to distinguish it from the other quantities, like time and mass. Instead, we have many
different units because they help immediately identify the scale that is involved. Hence, inches
versus feet immediately provide information of the size of interest. (There is also the historicalissue of different systems of units metric and English!) The units directly relate to the
operational definition of the quantity of interest and form the building blocks for all
measurements. The combination of numbers to indicate multiples (or fractions) of the referenced
unit, coupled with an indication of the errors, forms the complete quantitative representation of
data in science.
How do we determine the basic building blocks for our units? These come directly from our
operational definitions. Historically, physicists used to maintain standard building blocks in
Paris, France. The reference standards for length and mass were made out of a tough alloy
whose shape and dimensions changed only slightly with temperature; they were kept in a
carefully controlled dry environment. Today we use more invariant and more precise standards.
These may include the mass of an electron, the oscillation of a molecule (for time), and the
wavelength of a specific laser light. Standards are continually improving.
Here are some widely used fundamental units:
Quantity Units
Distance Meter, inch, footTime Second, minute, hour, day, year
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Mass Kilogram, gram, slug
Note that most of the units are frequently expressed with abbreviation: foot = ft, meter = m,
second = sec or s, minute = min, kilogram = kg, etc. The choice of a set of units is generally
referred to as a system of units. There are many different systems of units. The two common
systems that we will most often use in the textbook is the metric system (also referred to as the
MKS system or as the SI system) or the English system. (SI means Systeme
Internationale, the international system of metric units.) These systems are people-sized. We
are familiar with things whose size is expressed in these units, and as a result we usually feel
comfortable with these units. This sense of comfort frequently is helpful when developing an
intuitive understanding of a physical system.
System Distance Time Mass
Metric (SI) Meter Second Kilogram
English Foot Second Slug (or pounds for
weight, a topic for
later)
For objects that are slightly smaller, it is common to use a variation on each of these:
System Distance Time Mass
Metric (cgs) centimeter Second gram
English inches Second Ounces (for weight)
Addition and subtraction involve operations only on the numbers (the units are unchanged).
Thus physical quantities can be added (or subtracted) only if they have the same units. These
guidelines need to be kept in mind whenever mathematical operations are performed withphysical quantities. Once again, we have a signal to look for in the use of numbers in scientific
reports. By definition, if a report attempts to add quantities of different units, it just cannot be
done, and you should be suspicious! We also see that it makes no sense to measure area in inches:
square inches is the appropriate unit. Likewise, volume is measured in cubic inches or cubic
meters, etc. If you can remember the basic units for quantities, you can use this as a check on the
science that you are evaluating.
In contrast, numbers with units can be multiplied and divided to make more complex units. The
reader is probably already familiar with the concepts of area and volume an example of
multiplying units, and with speed an example of dividing units However, these are such a
common use of numbers with units that it is worth briefly reviewing the two concepts.
The area of rectangle is one of the first things students learn. For example, the length ( L ) of a
rectangle might be 4 inches, and the height ( H) might be 2 inches. Then the area ( A ) is1:
2(4 in)(2 in) 8 in (which reads "8 square inches")A L H= = =
1 Notice how we use a letter in parenthesis to indicate the variable that will represent a certain quantity. This isreviewed in Appendix A.
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Note we have multiplied both the numbers and the units. We can demonstrate area and volume
graphically with stacked squares and blocks.
Figure illustrating the concept of area and volume by breaking a surface or volume
into smaller pieces. One question this helps answer is w many square inches are
there in a square foot? Answer: 1 ft2 = (12 in)2 = 144 in2. This often causes
confusion, but the key is to remember that whatever mathematical manipulation
you perform on the number 12 must also be performed on the units: (12 in)2 = 122
in2. Thus a cube that is one foot long on each side has a volume of 1 cubic foot or
(123 =) 1728 cubic inches.
Surprisingly, our example of dividing units, speed, is something that many people seem to forget
when in a science classroom and there is a test in front of them. But, driving on the freeway, they
can generally tell you how long it will take to get to a particular exit if they know their speed and
the distance to the exit (assuming no traffic jams occur!) They use the fact that average speed is
defined to be distance traveled divided by time elapsed:
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distancespeed = ,
time
sometimes written asspeed /x t=
,
where x is the distance traveled and t is the time it takes (more on symbols and equations in
Chapter 4).If distance is measured in meters (or miles) and time in seconds (or hours), then theunit of speed is m/s (or mi/hr), which is read meters per second (or miles per hour). If this
seemed confusing, just do the exercise mentioned above if the exit you want on the freeway is
20 miles away and you are going 60 miles per hour, how long will it take to get there?
Example: my car traveled 400 miles in 8 hours. What is the average speed?
average speed = distance/time = 400 mi / 8 hr = 50 mi/hr. This result is read Fifty
miles per hour.
Notice that in ordinary speech, people are often careless with compound units and it may not
matter for the application at hand. This is especially true for the compound units we discussed.
For example, a store might sell you 3 yards of material. This is really 3 yards long and, say, 1
yard wide, so the area is really 3 square yards. Similarly, some people might say that the speed
limit is 55, but that overlooks the units entirely. They assume that you know the units are miles
per hour, but the appropriate units might be mi/hr, or kilometers/hr, or even meters/sec. It
cannot be overlying emphasized: when doing science, it is important to specify units correctly
when describing measurable quantities. If you have ever done any baking, you know how true
this is! Just confuse tablespoons and teaspoons, or dry measure and liquid measure and see how
your cake turns out. (This could be a fun experiment try baking something with the wrong
units. Worst case scenario, you produce something inedible. Best case scenario, you discover a
new awesome dish!)
We will take a brief detour to examine in more detail the character of derived units. We noted
earlier that length, mass, and time are the fundamental quantities that are most commonly used,
and each of them can be associated with an operational definition. This makes the quantities
precise and unambiguous. They can be used to do work that is relatively objective. Velocity is a
derived unit. You might not measure velocity by a direct operation; you might make a distance
measurement the value of which is divided by the value of a time measurement. The business of
division is an operation that can be precisely and unambiguously described. In other words, the
operational character of the quantity (velocity) is still highly reliable; its just a bit more
complicated.
Similarly, we find that some fundamental quantities cant be measured directly. For example, we
cannot lay out a measuring tape to the stars to find out how far away they are. But we can
perform some operations that will provide such information. Specifically, we can use the
triangulation method to measure a nearby stars distance from us. In the triangulation process,
we measure the angle to the star at one time and again six months later. These two angles are
different, and trigonometric operations (along with the radius of the earths orbit) will allow us to
calculate the stars distance. In other words, if direct measurement is impractical, the quantity of
interest might be obtained by indirect means. Measurement of other quantities can be used (like
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the angles toward stars), provided that operations exist that can relate these other measurements
to the desired quantities. We just need to have clear and precise operational rules to connect
measurements with theory. As long as we have these operational rules, science proceeds reliably.
Modern Aside: Length, mass, and time are not entirely independent. The theory of special
relativity shows that space and time are related to each other; in fact it is common to talk of the
spacetime continuum. The general theory then proceeds to show that there is a link between
mass and spacetime.
3B-2 People-Sized: The Scale of Things
We use the phrase people-sized to describe quantities that people are familiar with in everydayexperiences. We dont need microscopes or telescopes to examine such things. Note, as a
reference point, that a meter is slightly larger than 1 yard (which is 3 feet long). I am 1.75 (or one
and three-fourths) meters tall. My mass is 77 kilograms. It takes me about 33 seconds to walk
from one end of a football field to the other. My best sprinters speed is almost 9 meters per
second. These routine quantities (typical of daily life) are expressed in comfortable numbers
when the MKS (or SI) system is used. In different units they are less appealing. Consider the
following: I am also 17,500,000,000 Angstroms tall; my mass is 77 106 milligrams; and it takes
me 0.00038 days (or 1.05 106 years) to walk from one end of a football field to the other. My
best sprinters speed is an extremely small fraction (about 3 108) of the speed of light. The
speed of light is definitely not part of our experience base. (P.S. 106 =10 x 10 x 10 x 10 x 10 x 10 ...,
i.e., 10 multiplied 6 times, AND 106
=1
/10
x1
/10
x1
/10
x1
/10
x1
/10
x1
/10
..., i.e.,1
/10
multiplied 6times)2.
It is possible to convert from one system of units to another. For example, there are 0.3049 meters
in a foot. Whenever conversions are needed, we perform an operation that is nothing more than
multiplying by 1, but a special form of 1. For example: 0.3048 meter = 1 foot. Therefore, 1 =
0.3048 m / 1 ft. = 0.3048 m/ft. Also 1 = 1 ft / 0.3048 m. All we did here was invert the fraction,
because 1 divided by 1 is still 1. Either form of 1 is useful as a multiplier for conversions when
going from one system of units to another.
Example: I am 5 ft 9 in. tall = 5912 ft = 5.75 ft x (0.3048 meters/ft) = 1.75 meter.
Note that we discard ft/ft, which equals 1.
Exercise: What is your height in meters?
2 Not comfortable with scientific notation? See Appendix A.
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Example: Peggy Sue is 1.52 meters tall = 1.52 meters (3.28 ft / meter) = 5.00 ft.
Here we discard meters/meter
Exercise: A famous NBA basketball player is 2.14 meters tall.
What is his height in feet and inches?
Although we will not make a big issue of unit conversions, they do come in handy when making
certain estimates, as we will see in a later example. Also, scientists and engineers must be adroit
at these manipulations. Earlier, we also gave some masses and times using different units. The
reader should be aware that all kinds of quantities (velocity, force, energy, etc.) can be expressed
in a wide variety of units, and that conversion from one set of units to another is straightforward.
Thought Exercise: How big a number can you imagine or visualize? When do numbers becomeso big or so small that they lose their meaning to you? Here is one way to think of a million
people-sized things. Consider a pattern of balls one meter in diameter (people-sized). Space
the balls along the sideline of a football field, and then extend the pattern to three-dimensional
space with a pattern of one hundred balls in each direction. This pattern has 100 100 100 (or
one million) balls. So it is not too hard to imagine one million somethings. Now imagine this
cube becoming the single item that is used to repeat the 3-D pattern (100 100 100) for a trillion
one-meter balls. This is harder to grasp.
It is unfortunate that 25 years after Congress mandated a switch to the metric system, few groupsin the U.S. use it or are familiar with it. This presents problems in trade, since (for example) it
may be hard for a French repairman to find a metric wrench that is suitable for a 12-inch bolt.
This could be one reason we do not sell many different kinds of products in France. The only
other country that has not adapted metric units is Liberia. The emergence of the global village
might force the U.S. to accept the metric system.
3B-3: Advanced Estimates
It is one thing to estimate the size of common objects. The more challenging skill is to estimate
things that require simple mathematical operations. For example, the typical acceleration of a car
can be estimated from television commercials3
. In the U.S., you regularly hear about cars goingzero to sixty in a few seconds. Lets take if to be 0 to 60 mph in 4 s. Using conversion of units (go
back and review the unit section if need be!):
3 For this example, it helps to remember that acceleration is the change in velocity during a given interval of time. If you
do not remember this, it is ok for now, as we will review these ideas in later chapters. The point of this example is to show
the value of remembering simple formulas and sizes of key things to make basic estimates.
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2miles 1 hr 5280 ft 160 22 ft/shr 3600 s 1 mile 4 s
converts mph to ft/s divide by time to estimate acceleration
=
When we compare this to the acceleration due to gravity, which is232 ft/s , we can get a sense for
the acceleration of a car. We would call this acceleration 0.7 gs, because it is 0.7 times theacceleration due to gravity. For comparison, roller coasters can generate 2 4 gs! So, we can
immediately see why many people can get sick or do not like roller coasters, but fewer people
complain about accelerating their care!
Now, at this point you might be ready to give up acceleration, gravity, units, gs - do I really
need to know all this? The real answer is yes and no. We will review these topics here and in later
chapters, because it is very powerful to understand and use these basic concepts to make
estimates. You will find that with just a few ideas like these you can estimate a wide-range of
important things:
1)
What do you expect the cost of energy in your house to be?2) How much do you expect a typical school to cost? Given this, are your taxes being
wasted or well-spent?
3) What might the impact be of a few degrees of average heating? Should I really be
worried?
Estimates provide a quick check on claims in the media. They are not the final word, and can be
wrong in important ways, but they are a first step. In order to get better at them, there are two
useful ideas that we will review here. In preparation for these sections, if you are not completely
comfortable with significant figures and scientific notation, please see Appendix A for a review.
Example: Suppose you wanted an order of magnitude estimate of what the daily costs to runyour local 24-hour fast-food restaurant is? At first glance, this seems almost impossible as there
are some many aspects to the business: rent, salary, energy costs, food and supplies! But, if we
made it a bit easier and asked what is the minimum costs? There are some obvious estimates you
can make:
Salary for workers: average 5 workers at $10/hour: $1200
One manager at $100,000 for the year: $300
overhead (rent/energy/food/supplies): $500
___________________________________________________________________
Total $2000
There are a number of important features of this estimate that are important to notice. First, I did
not bother to figure out exactly how many workers or what they got paid. I used my experience
that there generally 3 8 workers in a fast food place at any time, and I picked a nice round
number for a minimum salary. Some workers are certainly making more, especially when benefits
are included, but this will give me a good minimum. I know the place has at least one manager,
probably more, but again, to get a minimum estimate, I went with one. Once again, no idea of
their salary, but it is unlikely to be off by factors of 10. Also, when I divided by the number of
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days in a year, I rounded the answer. Finally, I really have no idea about the other costs, but a
good rule of thumb (some estimates require either these rules of thumb or outright guesses) is
that overhead costs are at least 50% of the other costs you know. If you did not want to use my
50% rule, you could make some educated guesses based on what you pay for rent and utilities,
and assume they serve at least 100 hamburgers in a day and pay a few dollars per pound for their
meat. This will give you a good order of magnitude for the minimum costs. Notice, the actual daily
costs could be as much as $6000 or as little as $1000, and I am still within my factor of 10 for my
estimate!
An important hint when making an estimate for things is to focus on using integers that are a
good approximation to the quantity of interest. In fact, the language you most often hear is good
to an order of magnitude or good to a factor of two. An order of magnitude is another way
to say factor of ten, and it is one reason for the popularity of scientific notation. So, factor of 2
estimates are generally more accurate than order of magnitude ones, but order of magnitude is
much easier to achieve! Consider again the example of the acceleration of a car. There are two
parts to it: (1) the change in speed from 0 to 60 mph; and (2) the time this takes. The time is thepart we are approximating. We know it is greater than 1 s and less than 10 s, so to make a
reasonable estimate that is probably good to a factor of 2, we picked 4 s. It is still unlikely that the
time was less than 2 s or more than 8 s, numbers that are half and twice the time we picked.
Hence, we are able to claim that this estimate is good to a factor of two.
Challenge: One of the most common issues in public debates is the funding for school systems.
Using ideas in this section, estimate the minimum cost to run a school system. The challenge is to
NOT look up the actual spending in your area now, but to honestly estimate what you expect the
minimum cost to be. Then, compare that to what your area spends. If your estimate is higher than
your area spends, ask yourself how that might be? Could this explain problems with education inyour area? If your estimate is lower, now ask the really hard questions. Since you went for a
minimum, are there clear benefits from the additional spending? Can you determine if you missed
key areas of spending, or perhaps you actually identified waste in the system? Just a fair
warning: if you are not a teacher, most people under estimate what it takes to pay for qualified
teachers!
3-B. Errors: quantifying reliability
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Figure showing two different ways to measure a foot:
an actual foot and a ruler! Which method is more
accurate, and which is more precise?
We cannot repeat too much that science, especially physics, involves measurement. This
measurement process is an operation that is well defined; it is the operational property of
measurements that gives physical science its reliability. Reality in the philosophical sense is notthe issue! What does matter is the fact that no measurement is perfectly accurate. Even
theoretical equations are never perfect because they always contain some physical constants
whose values were determined by experiments. It is important to remember that physics is
ultimately based on human sensory observations and measurements performed according to
precisely prescribe operations (sometimes aided by instruments) of natural phenomena. Again
we note the fundamental fact that physical science is an experimental endeavor.
3-B.1. Precision versus Accuracy
There are two main classes of error in scientific measurements. We refer to these as: precision and
accuracy. They are different things and should not be confused with each other. As you considerthis, you might wonder, what does a detail like this have to do with being a good science
spectator? Lets briefly return to the sports analogy. For example, in baseball there are at least two
ways to get a person out: force out or tag out. Both are an out, and it might not seem to matter as
a spectator to know the different types of outs. But, it certainly increases your ability to enjoy the
sport and provide intelligent commentary and critiques of the sport if you know this difference.
Ironically, it is less important to know the specific names, then the fact that there is more than one
way to get an out! Precision and accuracy are somewhat analogous to this situation they both
describe errors in measurements, but sufficiently different types of errors that it is important to
know the difference. And, having the correct name for the two main types of errors just makes
you that much better at evaluating science when it is necessary to do so!
Precision is the easier of the two to define carefully. It helps if you are familiar with significant
figures. If not, it is useful to review this topic in Appendix A. The precision of a measurement is
your ability to tell the difference between two numbers. For example, if you are sure that an
object is 0.10 cm long and not 0.09 cm or 0.11 cm, your precision is 0.01 cm. In generally, the last
significant figure in a measurement generally determines the precision. Thus 9.613 kilograms has
a precision (or uncertainty) of 0.001 kilograms (because the measurement was not 9.612 or 9.614
kilograms.) Another way to say this is that precision is an estimate of the smallest increment you
have access to when you make a measurement (usually due to the limitations of the measuring
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instrument). Hence 9.613 kilograms and 0.026 kilograms have exactly the same precision (0.001
kilograms) because it is the last significant figure that matters, not the size of the measurement.
Precision is also referred to at times as the resolution of the measurement.
There are times that the precision may be less than the last significant figure but greater than the
second to last significant figure. For example, you might be using a ruler that is marked precisely
in increments of 1 cm. In this case, you can certainly estimate the result to some fraction of a cm.
Depending on your confidence in your ability to estimate the values less than a cm, you might
state your results as a certain number of centimeters plus or minus 0.5 cm. For example, for the
object in the figure, you would the length as 4.5 0.5 cm to indicate that even though you are
quoting the result with a significant figure of 0.1 cms, your estimate of the precision is actually
0.5 cm.
Figure: The ruler in the figure is marked in centimeter increments. The objectbeing measured falls between 4 and 5 cm. A reasonable estimate of the
precision is 0.5 cm. If one was really confident, you might even use a
precision of 0.2 cm!
Often you do want to know the precision with respect to the actual size of the measurement itself.
Relative precision refers to the size of the error or uncertainty relative to the size of the measured
quantity. Hence 0.001 kg out of 9.613 kg is a relative precision of 0.01%, while 0.001 kg out of
0.026 kg is about 4%. Thus, the relative precision associated with 9.613 kg is better than that
associated with 0.026 kg. Note that relative precision is dimensionless (usually given as a
percentage), but precision is expressed with units. Similar arguments apply to theoretical
calculations.
Accuracy expresses the size of the error or departure of a measurement from the exact answer.
Unlike precision, which is well-defined, we never know the exact answer; thus we can only guess
or estimate the accuracy of any given quantity. Two common examples of the difference between
precision and accuracy are the use of scales and watches. For example, it is not uncommon for a
inexpensive household scale to measure with a certain precision, say to 0.1 pounds, but to have
an unknown offset that is larger. For example, the scale may be offset by 2 pounds and we do not
know it. This is why most scales have a way to zero the scale, which is an attempt to get the
measurement as accurate as possible by making sure the scale measures zero when nothing is on
it. The other common example of accuracy is when people set their watch forward a few minutes
to make sure they are not late for things. The precision of the watch is not affected by this, and
remains seconds (if it has a second hand), but the accuracy is only minutes.
Often, the best that we can do is to infer that the accuracy is no better than some given value
based on our experience. However, as errors are eliminated (or when corrections are made to
account for errors), precision and accuracy tend to converge. The reason for this is that once you
have eliminated the sources of error not related to the resolution of your measuring device, the
only error left is the precision. At this point, the precision becomes a good estimate of accuracy
because it tells you how likely the number is to be different from the real result. But, how do
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we go about eliminating or accounting for error? For this, we need to understand the different
sources of errors and the ways to account for them.
3-B.3 Systematic versus statistical errors
When evaluating sources of error, especially issues with accuracy, there are two types of errorswe need to consider: systematic and statistical. Systematic errors arise when there is a specific and
consistent mistake that is made in a measurement. For example, a meter stick would expand at an
elevated temperature required for a certain experiment. If we did not notice or account for this
expansion, then length measurements using this ruler would produce values that are too small.
Also, a systematic error might happen if an experimenter consistently uses an instrument poorly.
Many students learn to use protractors to measure angles in school. Generally, one has to line the
protractor up correctly, or the angle that is measured is wrong. Systematic errors are often the
most difficult to identify because they are by definition mistakes you make that you are not aware
of! This is why having multiple people review an experiment is incredibly useful for identifying
systematic errors.
A common method for dealing with systematic errors is to design experiments measure thedifferences in the quantities of interest. By computing the difference of two measurements with the
same potential systematic error, the error cancels out. Lets consider the case of our ruler that
expanded so that any given measurement of length is 2 cm longer than the actual length. Suppose
we want to measure the height of two people: Susan and John. We measure Susan to be 150 cm,
and John to be 160 cm. In reality, Susan is 148 cm and John is 158 cm. This represents the
systematic error in each measurement. But, if we ask for the difference in the two heights, the
answer using our ruler is:
height of John - height of Susan 160 cm 150 cm 10 cm= = .
If we do this using the actual heights, we arrive at the same answer:
height of John - height of Susan 158 cm 148 cm 10 cm= = .
The most useful feature of using differences to account for systematic error is that it works even
when you do not know the magnitude of the systematic error! Consider our above example.
Suppose we just knew that the systematic error was some value E, and that John had a real
height that we will call jH and Susan had a real height that we call sH . Then what we know is
the following:
measured height of John - measured height of Susan 160 cm 150 cm 10 cm= =
Rewriting this using our variables and the fact that4:
measured height of John ( )
measured height of Susan ( )
j
s
H E
H E
= +
= +
4 Refer to Appendix A to review the use of variables.
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( ) ( ) ( ) ( ) ( ) 10 cmj s j s j s
H E H E H H E E H H+ + = + = = ,
we see that the common systematic error always cancels out, and we get the actual height
difference. We put actual in quotes because there may be other errors that do not cancel; these
are the statistical errors discussed next.
Statistical errors occur if conditions in a measurement fluctuate randomly. There are two basic
types of fluctuations in measurements. The first type comes from variations in the measurement
technique. For example, consider measuring the diameter of a uniform cylindrical bar with a high
precision micrometer. The measuring tool will not always return to exactly the same spot on the
bar, and the diameter of the cylinder will not be perfectly uniform. Also, it is impossible to use
the micrometer in exactly the same way every time; and this may produce a random fluctuation
in the measured value. (Note that it could also produce a systematic error that is not random.)
The second class of statistical error comes from intrinsic fluctuations. There are many physical
quantities that are inherently fluctuating in time or position. For example, consider the weight of
a person. If you were to measure it throughout the day, it would fluctuate based on whole host
of factors such as, how much the person just ate, how recently the exercised, etc. The interesting
thing about intrinsic fluctuations is that sometimes they need to be treated as a source of error and
sometimes they are the thing you want to measure! Consider our weight example. Usually, you
just want to know the average change in your weight on a daily or weekly basis. In this case, the
fluctuations mentioned here are potential sources of error because they can lead to you
concluding that your average weight changed between two days when what really changed was
the time you weighed yourself! However, if you are interested in how quickly eating and
exercises changes your weight, these are the quantities you would want to measure!
In physics, we have learned that there are even different classes of intrinsic fluctuations. A
particular important breakthrough that we will return to in later chapter is the idea of quantum
fluctuations. These are fluctuations in systems that exist no matter what you do to get rid of them!Another important class of fluctuations that will be discussed in the content chapters is
associated with large numbers of objects acting together, such as molecules in a gas. In this case,
it is easier to treat the fluctuations in a statistical sense then to track the motion of every particle!
Because of this (and other important phenomena), statistics is a critical area of mathematics for
the serious science spectator, and we will spend an entire section reviewing some key concepts in
statistics. But, lets quickly consider two more examples of fluctuations, the types that occur, and
why they are important.
Physical Example: We have already addressed some of the issues with measuring the average
temperature of the Earth when we looked at operational definitions. The temperature is an excellentexample of a physical process with intrinsic fluctuations. Just think about your daily experience.
The temperature fluctuates throughout the day in fairly regular way. It warms up as the sun is
out, and then cools down once the sun goes down. But, on top of that regular variation, it can
fluctuate as clouds come and go, or as you move in an out of the shade, or as the wind moves the
hot and cold air around from different places. If you spent the day walking around with a
thermometer, you would see all of these variations as fluctuations in your measurement. Some of
these fluctuations are what we would consider actual changes in temperature (such as the variation
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from day to night) and others might be viewed as sources of statistical error (such as the wind
moving the air around your thermometer). However, understanding and correctly accounting for
these fluctuations and determining under what conditions they represent a measurement of a
real change or an error is one of the major challenges of doing careful experiments.
Fiscal Example: Suppose you are planning to invest in the stock market. The prices on the stock
market vary in time: they fluctuate. There are two types of fluctuations. There are short term
fluctuations that really are random chance due to the fact that large numbers of people are
buying and selling stock at any given moment, causing small fluctuations in prices. There are
long term fluctuations. These tend to be more deterministic. They are not completely
predictable in detail because are models are still limited. But, one can always count on an
eventual downturn after an excessive increase in prices that are associated with a bubble in the
market. Finally, there is the long term average trend which is consistently increasing.
Depending on your goals and the time you plan to invest for, you are going to worry more or less
about the short term random fluctuations, longer variations, or even longer long-term average
behavior.
3-B.3. Sources of Error
Figure illustrating some potential sources of error with a meter stick.
Before focusing on characterizing fluctuations, it is worth taking a tour of potential sources of
error. Consider the measurement of the diameter of a penny. It can be done with a meter stick or
a micrometer. Both are referenced to the same standard, but with different degrees of precision.
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Both contain some inherent physical imperfections, again with different degrees of precision.
Each has different limitations. Both can be used with bad technique. The penny also must be
considered. It will not be perfectly round; thus the diameter is not the same taken in different
locations. Any given penny will have its dimensions change with temperature. And every
penny is slightly different from every other penny, so measurements of one penny are not
perfectly representative of all others. This simple example is typical of the type of error
considerations that are encountered in every experiment. There are several sources of uncertainty
in measurements, and we will take a brief look at each of these.
1. Uncertainty in the standard used to define the unit of measure. For example, the kilogram used to
be defined as the mass of a reference object that was kept in Paris. This object could be compared
with other objects by using a pan balance. The error that would arise from such comparisons was
fairly small for most applications. Today, the basic unit of mass is referenced to the hydrogen
atom. When standards are poorly defined, considerable error can occur. An example of this
problem may arise because the standard is not constant. The foot, an English length unit, was
initially defined as the length of the foot of a certain English king. (This may be why English
monarchs are often referred to as rulers.) The kings foot also was not of constant length from
morning to night or from day to day (or even as the temperature changed). The kings foot alsomight change over longer time periods due to growth or shrinkage (or because of gout, etc.).
These days, however, the foot is defined in terms of the metric system (1 foot = 0.3048 meters); the
meter is referenced to the wavelength of light emitted by an atom when it changes from one
energy level to another energy level.
2. Imperfections in the equipment being used. No measuring equipment can operate perfectly. For
example, if I use a meter stick on an extremely cold day, it will shrink slightly, increasing the
errors in its readings. Of course, a correction can be made to account for expansion or
contraction. This implies that we need to know at what temperature the meter stick is accurate,
and that we know how the length of the meter stick changes with temperature.
Figure of different types of equipment for measuring the mass of
objects. Each of these has different sources and types of errors.
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3. Limitations in the equipment being used. When I measure my weight on a bathroom scale, I
might get 157 pounds. But I wouldnt get 157.357 pounds, because the scale is not capable of
measuring to this precision, although some other scale might be. When my bathroom scale says
157 pounds, the precision is probably about one pound, because I can tell it doesnt mean 158
pounds, but I would have a hard time measuring precisely 157.5 pounds. However, it is also
possible (perhaps even likely) that the scale could be in error by as much as two or three pounds.
4. Inaccurate techniques in using equipment. When I stand on the bathroom scale some mornings, I
get 173 pounds. But then I notice that the scale says 11 pounds even when I am off it. This means
that someone has tinkered with the knob that sets the zero reading. If I had relied on the value
173 pounds, I would have gotten my inaccurate result because of improper technique. Making
sure that the equipment is properly calibrated is standard procedure when setting up experiments,
and it prevents the above problem. Other flawed techniques are also possible. Someone
standing near me might get a different reading than I do because they are looking at the scale
from an angle, changing the geometrical relationship between the numbers and the indicator
pointing at them. This is like the difficulty encountered when trying to read a car speedometer from the
passenger seat next to the right front window. The driver has a better (more accurate) viewpoint.
5. Improperassumptions concerning the system being measured. If you measured my height early in
the morning, you would get 69.5 inches. But if you assume that this is always my height, you are
wrong, because you would be assuming that a person always has the same height, which is not
true. In fact, when you measure my height in the evening, you would get a number like 69.2
inches. The reason I and other people usually get shorter during the day is that the vertebrae in
our backbones are separated by pads called discs, which tend to compress during the day. At
night, when we sleep, the discs are not under stress, and so they expand slightly, making us a
little taller when we get up in the morning.
Here is another example of an improper assumption about the system being studied. Suppose
you wanted to study the influence of gravity on falling pieces of paper. So you design anexperiment in which you time the fall of pieces of paper from different heights above the ground.
Your results would be inaccurate because falling paper is influenced not only by gravity but by
air resistance. So your claim that the results showed the influence only of gravity would be
wrong. The proper way to study the effect of gravity of falling pieces of paper is to drop them in
a vacuum chamber, eliminating or greatly reducing the influence of air resistance. This illustrates
a significant challenge in science. Scientist must develop models describing a system which are
simple and yet complete enough to predict the behavior of the system.
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Figure showing your height changing with the time of day. Humans are slightly
taller in the morning than in the evening because of the compression that spinal
disks are exposed to during the day because we are primarily vertical.
6. Variations in the system being measured . If you were to measure how tall people in a class are,
you would find considerable variation. These are actual variations; they are not the result of how
we use our equipment. So, if you were to measure the height of only one student, you would not
be able to draw any reliable conclusions about the range of heights in the class.
Thought Experiment: If I step on a scale in Death Valley, my weight may be
different than when I step on the same scale at the top of Pikes Peak. This could
be due to almost any of the 6 preceding categories of uncertainties. How couldthis be?
A number of important mathematical methods have been developed to study systems
with natural variations or fluctuations. It is this last example that we will turn our
attention to now how to understand and think about fluctuations and uncertainties that
are either intrinsic in the system, due to randomness, or due to some lack of information
on our part.
3-B.4 Error bars and notation
When we want to tell someone what our expected error is for a given measurement, we already
saw in our discussion of precision that we write our answer as:
6.45 0.5 m
This expression has three parts:
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1) 6.45: this is our best estimate of our measurement, or the average value of our
measurement. The last digit gives a good indication of our precision. Though as we
mentioned, sometimes our precision is a little worse than this digit, but not as bad as the
next digit!
2) 0.5: this is our best estimate of the error in our measurement. Notice that this will often
include both the accuracy and the precision. Because in this case, the result is quoted to
the nearest 0.01 and the error is given as 0.5, there is probably a statement being made
about precision and accuracy. Often, if the accuracy is as bad as this error indicates, the
precision is no longer relevant, and you would write the measurement as 6.5 0.5 m .
3) The final piece is the units. In this case, the unit is meters.
There are a few other issues to be aware of with this notation. In some types of measurements,
the number after the is the standard deviation, a quantity we will review in the next section. This
is not always the true expected error in the measurement, but it is often a way to communicate the
expected range of values, which is very closely related to error. From a science spectator point of
view, the main goal is to see that a reasonable effort was made regarding the general precision
and accuracy of the measurement, and to report it. Subtle distinctions involving propagation of
errors, standard deviation versus standard error, etc., are things you can explore more if
interested, but not essential.
It is worth noting that sometimes the error is not symmetrical. Maybe there is a iron-clad reason
the number can not be negative for example. So, you might get a situation where the answer is:
1
0.50.5 m+
.
This reflects the fact that even though your error may be 1 m, the answer can not possibly go
below zero, so 0.5 1 m makes no sense.
Finally, it is worth pointing out that when graphing data, the error is indicated by error bars that
represent the range of values suggested by the error. This is illustrated in the following figure:
Figure illustrating the use of error bars. For each of the measurements of
height in this plot, the error is 0.1 cm .
0 2 4 6 8 100.0
0.2
0.4
0.6
0.8
1.0
1.2
Height(cm)
time (days)
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3-C Fluctuations, Statistics, and Probability
In this section, we will be tackling two of the most important, and perhaps the most challenging
topics in mathematics that is relevant to science literacy: probability and statistics. The challenge
with these topics is that to apply them correctly often involves subtle ideas that can be easily
overlooked by the non-expert. This is coupled with the fact that our intuition of these topics isoften unreliable. We will consider these two topics in the context of an important physical
phenomenon:fluctuations. To help with this discussion, we will focus on two examples for which
people do have some intuition: financial issues (money) and weather.
Given the inherent difficulty of these topics, it is worth explicitly recalling that the goal of our
discussion is to provide essential tools for basic science spectatorship. To return to our sports
analogy, to be a science spectator, it is not necessary to go into all the subtle aspects of using an
off-side trap in a game of soccer. But, you need to know the basic facts about off-sides to
intelligently watch the game. As we deal with the concepts of randomness, probability, statistics,
and fluctuations, the reader needs to understand that this is really the subject for whole textbooks
and there are many details we will gloss over by necessity. We will focus on key conceptual
ideas and a few central calculations that are handy to have for analysis of scientific reports (and
occasionally daily life).
3-C.1 Definitions
Fluctuations in a quantity are changes in time or space. There are two basic types of fluctuations:
random and predictable. The day to day fluctuations in temperature and the price of the
stock market are basically random. We might have some ability to predict their general trends,
but detail prediction is not possible. However, the long term fluctuations are predictable
summer is hotter on average then winter in Northern latitudes! Another example of a predictable
fluctuation is given by the voltage in an alternating current system. The voltage fluctuates from
positive to negative in a smooth and predictable manner. Generally, predictable fluctuationsoccur in systems that are periodic. In fact, once it has been determined that the variations in a
quantity are sufficiently regular and periodic, one generally does not use the term fluctuation,
but the more specific term of periodic. Periodic variations are generally well described by
sinusoidal functions, a topic we will review in Chapter 4. So, for most of this section, we focus on
random fluctuations, and just use the term fluctuation.
Distributions refer to the collection of numbers that are the result of a series of measurements.
These can take many forms. They can be measurements of a single quantity taking over time. For
example, a set temperature measurements that is taken every hour forms a distribution. If one
measures the height of individuals in a group, this will also be a distribution. These are examples
of discrete distributions where you have measured a countable number of objects. A challenge for
these types of distributions is determining how best tograph them. This is best illustrated with asimple example.
Example: Consider measuring the heights of a group of people. (Names have been removed to
protect their identity!) Here are the results in the form of a table:
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Person Height
A 1.2 m
B 0.9 m
C 1.3 m
D 0.7 m
E 1.5 mF 1.2 m
G 1.4 m
H 1.0 m
I 1.1 m
If we want to look at the distribution of the results, we need to count how many times we get the
measurement of the height in a certain range or bin. We will show the results of using three
different choices:
All three of these graphs are of the same data from the table. The first one plots the number of
heights in bins of width 0.3 m. So, there are two people with a height between 0.6 m and 0.9 m,
the first bin in the plot. The second plot uses bins of 0.2 m, and the last one uses bins of 0.1 m.
In the last case, one of the bins goes from 1.1 m to 1.2 m, and this is the bin with three people in it.
Notice how the visual impression of the distribution can vary with the choice of bin size. This is a
key feature of reporting data, and something to be extremely aware of as a science spectator!Make sure that the person presenting the data is not using their bin choice to convey a falseimpression!
Probabilistic event is one where the outcome is a matter of random chance. Consider a box filled
with half red balls and half blue balls. Putting your hand in without looking and grabbing a ball
gives you a 50% of getting a red ball and a 50% chance of getting a blue ball. Similarly, the case
flipping a perfectly balanced coin is a 50-50 situation5. There is a 50% chance of getting heads and
a 50% chance of getting tails. In this case, any model used to describe the behavior predicts the
chance of particular outcomes occurring and not the outcome itself. The field of probability deals
5 There is a subtle issue here that the careful reader will notice. For a single coin flip, if we truly tracked every elementof launching the coin, we could predict whether or not it would come up heads or tails. For the ball example, if wetracked every motion of the balls and the exact location of your hand, we could predict your outcome. So, strictlyspeaking it is deterministic. However, in practice, there are so many variables involved, we can consider it
probabilistic. In contrast, quantum mechanics is a truly intrinsically probabilistic theory in many ways. We will revisitthis in the content chapters.
0.6 0.7 0.8 0.9 1.0 1.1 1.2 1.3 1.4 1.50.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
Numberofpeople
Height (m)
0.6 0.8 1.0 1.2 1.4 1.60.0
0.5
1.0
1.5
2.0
2.5
3.0
um
erop
eople
Height (m)
0.6 0.8 1.0 1.2 1.40.0
0.5
1.0
1.5
2.0
2.5
3.0
umberop
eople
Height (m)
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with the rules for predicting various combinations of random events. For example, if you wish toknow the probability of getting four heads in a row when flipping a balanced coin, you woulduse probability theory to compute this. This is one area where our intuition is often flawed.
Intuition Test: Write down on a piece of paper what you might expect to get if you flipped a coin50 times in a row. Use H to indicate heads and T to indicate tails. After writing down this series,try flipping an actual coin 50 times. One thing to look for is the longest streak of head or tails inyour fake series (most number of heads or tails in a row) and the longest one in the real series ofheads and tails. Also, compare the number of times you gets streaks of 3, 4, 5, 6, etc., this will letyou know how good your intuition is. Hint: This exercise works best if you can get a group offriends to do it independently from each other and compare notes. Then the differences reallyshow up!
A deterministic event is one in which the outcome itselfis predictable (within the stated precision)
with the use of a mathematical model, and not just the probability of different outcomes. Thiswould be the case of throwing a ball. Given the initial speed and direction of the throw (and a
few other variables, such as wind and air-resistance), a person can reasonably predict where the
ball will land. There is some error associated with the prediction, but this can be characterized as
well.
Statistical events refer to the analysis of the properties of many events. One challenge in looking at
the outcome of different systems and behaviors is that when considering a large number ofevents, the results can be random even when the individual events are deterministic. In this
case, it is often best to use a statistical description of the system. For example, if we throw a ball
many times, each individual throw is deterministic. But, we do not have the ability to throw the
ball with the same initial angle and velocity every time. So, if we measure the landing spots, we
will get a distribution of locations. We will treat this problem in a probabilistic fashion, where therandomness is due to unknown information (initial angle and speed of the throw) in an otherwisedeterministic process (throwing the ball). In this case, we can analyze the statistical properties of
the landing locations, and learn useful information about our throwing process. On the otherhand, if we flip our coin many different times, we will get a distribution of heads and tails. In thiscase, the distribution is from an intrinsically random process. We will use the same statisticalmethods in these two cases, but often we will be asking different questions. Therefore, justbecause you see the same words like mean or standard deviation, it is important to understand thecontext I which they are being used to fully understand what they mean!
Generic fluctuations would be ones that are not easy to classify as strictly speaking probabilistic ordeterministic. One example is cases where the quantity of interest is being studied for different
objects. For example, we already mentioned looking at the height of different people in a room.Depending on your perspective, you might think of this as probabilistic (the heights are randombecause you do not know anything about the people) or deterministic with a degree of error (youknow something about the genetics and history of the people in the room). Another way to thinkof these categories is that the distinction betweenprobabilistic and deterministic is often an issue ofinformation regarding the system. As with anything, there are clear-cut cases where theinformation required is so overwhelming, we declare the situationprobabilistic, as we did for our
ball and coin examples. However, consider the case of the amount of money I have in my pockets
from day to day. This is not strictly speaking random it occurs because I take money in and out
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for specific reasons. To the degree that I can track and predict these reasons, the process is
deterministic. But, there always seem to be surprise events that occur that prevent the
development of a fully predictive model for the behavior (yet!). Therefore, these fluctuations are
often best described in aprobabilistic model.
Errors in measurement techniques often produce a distribution of results that are well described
by statistical methods. In fact, sources of error can create fluctuations even when the quantity
appears to be constant. For example, the length of a rod might be unchanging; but the measured
value of the length may fluctuate due to variations in the process of measurement. This could
include the case where different measurement tools are used.
3-C.2 Mathematical Formulas
Given the importance of statistical analysis, it is the one area of mathematics where it is worth
reviewing the relevant formulas and doing a few computational examples. To make this easier, it
is important to introduce some notation. To help with the abstract notation, we will use the
specific example discussed with regard to distributions of the students heights in a class. The
first step is to define a variable that represents each measurement. It is common to use x, but wecould just as easily use any other letter. Often, we pick the first letter of the quantity that we are
measuring. The next step is to number the different measurements and use that as a subscript on
are variable to keep track of each element. We can do that in our table of heights:
Person Height
1x 1.2 m
2x 0.9 m
3x 1.3 m
4x 0.7 m
5x 1.5 m
6x 1.2 m
7x 1.4 m
8x 1.0 m
9x 1.1 m
We generally refer to the number of the measurements as N or n, which for our example is
9n = . A final notation point: if we want to refer to ageneric measurement and a specific one, we
will use the notation ix where the variable i as a subscript tells us that we want one of the 9measurements that we made, but at this point, we do not care which one!
Here is where for many readers their math fear kicks in just take a deep breath and relax!
Remember, we are learning the essential features of a new language. This is a chance to start
practicing converting between symbols and English.
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There are two main terms that we want to be able to computes: average (or mean) and standarddeviation.
We define the average (or mean) xave of our measurements to be
1
1 n
ave i
i
x x x x
n =
= = = .
Hereavex , x and x are just different symbols that can be used for the average value of x, and
is a symbol that indicates an operation that adds all the values of x together, where i indicates
each separate value and takes on all values from 1 to n. You can see how this takes significantly
more space in English to write then it does in math symbols. Remember, if you are not happy
with the symbols, go with the English: The average is the sum of all the measured values divided
by the number of measurements that were made. So for our example, it looks like this:
9
1 1
1 1
9
1.2 m 0.9 m 1.3 m 0.7 m 1.5 m 1.2 m 1.4 m 1.0 m 1.1 m1.14 m
9
n
ave i i
i i
x x xn = =
= =
+ + + + + + + += =
One feature to notice about the calculation is that we followed our rules for units. We only added
numbers with the same units, meters! Also, because the number of measurement does not have
any units, the final answer has the same units as the measurements, as we would expect for the
average height.
We often want to have a measure of the spread or the width of the distribution of the measured
values. You could just compute the difference between the highest and lowest values, but this
does not capture the fact that you often have many measurements grouped around a central
value with just a few values that are very large or very small. For this case, we define the
standarddeviation and use it to estimate the width of the distribution. This is illustrated in the
figure that represents the measurement of a large number of heights.
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Figure illustrating a distribution of heights. This distribution is plotted as aprobability
distribution where the number of results for each height has been divided by the total
number of heights. The red arrows represents the width as measured by thestandard deviation: the width is given as twice the standard deviation and represents
the mean plus and minus the standard deviation. Notice, this captures most of the
measurements, though certainly not the full range. It is common to use this as the
estimate of the range of likely values. In this case, the range given by the red arrow
represents approximately 65% of the data. If we went to plus and minus twice the
standard deviation, we would be at 95% of the data.
For our purposes, we will define the standard deviation x (called the standard deviation of x)
by the following formula6:
2
1
1( )
n
x i
i
x xn
=
=
Again, the formula may appear scary, but the English is more complicated in some ways:
Take each measurement that you made and subtract the mean from it. Take each of these
numbers and square them. Now, take all these new numbers and add them up (that is the symbol again). Now divide this number by the number of measurements and take the square
root of this number.
Here is an example showing how to calculate the standard deviation of the height of fourstudents (we use a small number to focus on the arithmetic involved):
6 Strictly speaking this is an approximation. Because our focus is on the concept that numbers have uncertainties, and the
different physical meanings associated with the standard deviation, we will use this approximation for all problem
examples that we discuss in this text. This does ignore some subtle issues in a rigorous study of statistics, but these do not
impact the main conclusions we will be making. If you are interested in a more detailed discussion, you can refer to any
basic book on statistics.
0.5 1.0 1.5 2.0 2.5 3.00.00
0.02
0.04
0.06
0.08
0.10
mean minus one
standard deviationmean plus one
standard deviation
Mean =1.5 m
Probabilityof
height
Height (m)
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i xii
x x 2( )
ix x
1 1.50 0.10 m 0.0100 m2
2 1.55 0.05 m 0.0025 m2
3 1.60 0.00 m 0.0000 m2
4 1.75 +0.15 m 0.0225 m2
2
1
( )n
i
i
x x=
= (0.0100 + 0.0025 + 0.0000 + 0.0225) m2
= 0.0350 m2 ,
and so the standard deviation is
2 2
1
1 1( ) (0.0350m ) 0.09 m
4
n
x i
i
x xn
=
= = =
As with our earlier example, we can also compute the average height of these four students. You
should check that it is 1.60 m. In this case, if we ask the question what is the average height of a
student in the class, we might present the answer as:
Student height = 1.60 0.09 m.
This is a statement about two facts that we have determined: (1) The mean or average height is
1.60 m and (2) the standard deviation is 0.09 m. In this case, the standard deviation is telling us
about the spread or range of heights in the class. One might think of it as an error in the sense of
how accurately the mean reflects a true measurement of height in the following sense. For a
class where the students are all essentially the same height, the standard deviation will be reallysmall and the average height will provide an accurate picture of the height of a student in the
class. For a class with a wide range of heights, the standard deviation will be large, and the
mean will not necessarily provide an accurate picture of a typical height because such a quantity
does not exist!
ASIDE:
Another important issue is one of judgment. Sometimes data sets contain values that simply do not seem
credible. What is to be done in such cases? Consider the heights of four students that were presented previously,
and suppose that a fifth height had been recorded of 16.1 meters. This means that one of the students was about
as tall as a five-story building! Surely this is ridiculous, and the value should be discarded. But on second thought,it looks like a decimal was misplaced. Do we simply move the decimal? Do we repeat all five measurements?
If we have names associated with the heights, then it would only be necessary to re-measure one student.
Suppose that the measurementcould not be repeated, what would be done then? The point of this paragraph issimple. Sometimes it is necessary to reject data, and this is a matter of judgment. There is no general rule ofthumb that applies other than vigilance by the experimenter.
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In contrast to measuring four different people, we can consider the following interesting twist.
Suppose the four heights in the table were four measurements of the height of the same person
taken four different times. In this case, we would compute the same mean and standard
deviation. We would still say that the standard deviation represents the accuracy of the
measurement. But, notice there is now a different sense to this accuracy it is the accuracy with
which were able to make the particular measurement! It might represent the variation in the
persons height with the time of day; it might be our ability to use a ruler; or it might be some
other error. Though very similar to the interpretation of standard deviation for the heights of the
different people in the class, it is useful to note the subtle differences. For people in the class,
there is clearly a real distribution of heights even when our measurement technique is perfect! The
standard deviation is a way to measure how wide this distribution is. For a single person, it is
conceivable that the measurements should represent a single value and the only reason for the
variation in measurements is some source of error in the measurement.
We can see from this example that a blind use of calculational formulas should be avoided.
When we interpret the standard deviation in the above equations as a measure of the accuracy of
the mean, we assume that the x values are reliable. But we know that an individuals height
changes during the day. Students may also be wearing shoes of differing thicknesses, or mighthave differing posture. All of these conditions affect the final result. Could a standard system be
adapted for obtaining this quantity of average height? Would it be sensible (or worth the trouble
and expense) to do so?
The mathematics of statistical processes is a highly developed and sophisticated branch of
mathematics, and perhaps of the most poorly understood and misused! Given this, our example
provides a good idea of what you should take away from our discussion of averages and
standard deviation. At its most basic level, the fact that an average and standard deviation is
being reported tells you that there is a range of possible values for the measurement. The
standard deviation provides a good estimate for how wide the range of values is. If you want to
be even more specific, the results of mathematical studies of systems that fluctuate in this wayimply that two thirds of the samples will fall within one standard deviation of the average when
the resulting distribution of results agrees with a normal curve of error. This is also called a
Gaussian distribution or a bell-shaped distribution. Surprisingly, many things in the physical
world are described by such a curve, and so this is a good rule of thumb to use for the
quantitative meaning of standard deviation. The next figure displays these properties.
3-C.3 Statistics of Basic Probability
There is another characteristic of a set of fluctuating or random data that plays an important role
in scientific literacy the most likely or most probable value. Often, this is also the average of the
set of numbers, but this is not always true. This introduces the idea of probability. Probabilities
are represented as fractions, because a probability of one is considered an event that isguaranteed to happen. In general, the public is presented with probabilities all the time,
especially in the context of risk. As with the more general issue of statistics, probabilities are often
poorly understood and even completely misused at times. For simple cases, the probability is
straightforward to compute (or estimate) by taking the number of ways you can get your result
and dividing by the total number of outcomes. Unfortunately, one quickly finds that it can be
difficult to correctly count things like the number of possible outcomes, even when it looks easy!
Also, this argument relies on all the outcomes being equally likely.
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Warning Examples: Consider the challenge of computing the probability that an asteroid will hit
the Earth. An incorrect and nave argument would say: There are two possibilities, it hits or it
does not, so the chance of being hit by an asteroid is 50% (1 out of 2). The errors in this argumentshould be reasonably obvious, as the probability of the asteroid hitting the Earth involves a
number of factors, starting with the question of the time frame you want to consider! Another way
in which counting can cause problems is highlighted by the following example. Suppose you
determined the probability of a US citizen dying from a shark attack in a year by taking the
number of US citizens killed by sharks last year and dividing by the total number of US citizens.
What is one obvious problem with using this probability to assess your risk? I doubt anyone was
killed by sharks further than 1 mile from the water. So, if you are never within a mile of the
water, this calculation makes no sense.
As with statistics, probability is full of subtle issues. We can get a sense of some of the issues by
considering four standard cases, but as with statistics, it is most useful to know what you do not
understand, and then to seek expert help when it really matters!
CASE 1: Flipping a coin: In this case, there are two possible outcomes (heads or tails), and each
outcome can be achieved in a single way. So, the probability of each outcome is or 50%. Also,
in this case, the two outcomes are equally likely. So, this is the classic case where counting works
because each outcome is equally likely.
CASE 2: Rolling two normal six-sided dice: In this case, the outcomes are a one to six on one
dice and a one to six on the other dice. In this case, there are 36 different outcomes (6 x 6). The
argument is as follows. A one on the first dice can goes with any of the six values on the seconddice, and the same with a two, and so on, until you reach 36 possibilities. Now, compare the
probability of rolling a two, a three or a six. There is only one way to roll a two, so this has a
probability of 1/36. There are two ways to roll a three a two on one dice and a one on the other,
or vice versa. So this has a probability of 2/36, or 1/18. So, a three is twice a likely as rolling a two.
Finally, for a six, you can have the pairs (5,1), (1,5), (4, 2), (2, 4) and (3, 3). So there are five
possible outcomes, for a probability of 5/36. If you do this for all the values between two and
twelve, you will find that the outcome with the highest probability is seven (6/36 = 1/6). Also, this
is an example of a symmetric case. For example, the probability of getting six is the same as
getting eight. It turns out, for a case like this, if you rolled the dice enough times and took an
average of your results, it would also equal seven! This is an example of the average and most
likely result being the same.
CASE 3: Consider a room with 10 people in it with the following ages: 15, 15, 20, 25, 25, 25, 30, 50,
74. The average age is 31. This is not even one of the choices! But, if you were to pick a person at
random, the most likely age you would get is 25, something very different from the average. You
should notice that this case is very asymmetric. There are a few very large ages (50 and 74), that