We use cookies to distinguish you from other users and to provide you with a better experience on our websites. Close this message to accept cookies or find out how to manage your cookie settings.
To save content items to your account,
please confirm that you agree to abide by our usage policies.
If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account.
Find out more about saving content to .
To save content items to your Kindle, first ensure no-reply@cambridge.org
is added to your Approved Personal Document E-mail List under your Personal Document Settings
on the Manage Your Content and Devices page of your Amazon account. Then enter the ‘name’ part
of your Kindle email address below.
Find out more about saving to your Kindle.
Note you can select to save to either the @free.kindle.com or @kindle.com variations.
‘@free.kindle.com’ emails are free but can only be saved to your device when it is connected to wi-fi.
‘@kindle.com’ emails can be delivered even when you are not connected to wi-fi, but note that service fees apply.
The material in this book is an enlarged version of a highly successful, short course of lectures given to graduate students in the Nuclear Physics Laboratory, Oxford. The course was designed to interest both nuclear structure and elementary particle physicists.
I am an experimental high energy physicist, and although as an undergraduate I suffered a course in statistics, it was only later during my research work, when I had to deduce something from my own data, that I learned how to use statistics. I also discovered that there were many things that one learned by experience and which were not explicitly mentioned in text-books; I tried to incorporate these aspects of the subject in my lectures. The emphasis of my lectures was thus not on formal proofs or on a rigorous treatment of the subject, but rather on practical applications and on how to use statistics to obtain the best results from one's data and to know the limitations of the results. In short, this was a course given by a non-statistician to non-statisticians.
My course did not attempt to cover every single example of statistics problems that can arise in nuclear and particle physics. The aim was rather to explain as fully as possible the different techniques that are available for attacking data analysis problems, to explain their relative merits and drawbacks, and to try to give the students sufficient confidence in their own ability to tackle any new problems that they might encounter. The book has maintained this approach.
There are basically two different types of results of experiments that scientists perform in order to learn about the physical world. In one type, we set out to determine the numerical value of some physical quantity, while in the second we are testing whether a particular theory is consistent with our data. These two types are referred to as ‘parameter determination’ and ‘hypothesis testing’ respectively. (Of course, in real life situations there is a degree of overlap between the two: a parameter determination may well involve the assumption that a specific theory is correct, while a particular theory may predict the value of a parameter.) For example, a parameter determination experiment could consist of measuring the velocity of light, while a hypothesis testing experiment could check whether the velocity of light has suddenly increased by several percent since the beginning of this year.
In this chapter, we are mainly concerned with various aspects of calculating the accuracy of parameter determination type experiments. We will have more to say about hypothesis testing experiments in Chapter 2.
Why estimate errors?
When we performed parameter determination experiments at school, we considered that the job was over once we obtained a numerical value for the quantity we were trying to measure. At university, and even more so in every-day situations in the laboratory, we are concerned not only with the answer but also with its accuracy.
Another question concerns the oscillations of pendulums, and it falis into two parts. One is whether all oscillations, large, medium, and small, are truly and precisely made in equal times. The other concerns the ratio of times for bodies hung from unequal threads; the times of their vibrations, I mean…. As to the prior question, whether the same pendulum makes all its oscillations – the largest, the average, and the smallest – in truly and exactly equal times, I submit myself to that which I once heard from our Academician [Galileo]. He demonstrated that the moveable which falls along chords subtended by every arc [of a given circle] necessarily passes over them all in equal times….
As to the ratio of times of oscillations of bodies hanging from strings of different lengths, those times are as the square roots of the string lengths; or should we say that the lengths are as the doubled ratios, or squares, of the times.
Galileo Galilei, Two New Sciences (1638)
FINDING A CLOCK THAT WOULDN'T GET SEASICK
Navigation has provided one of the most persistent motives for measuring time accurately. All navigators depend on continuous time information to find out where they are and to chart their course. But until about two centuries ago, no one was able to make a clock that could keep time accurately at sea.
We have seen that the gaseous and liquid states are only distant stages of the same condition of matter, and are capable of passing into one another by a process of continuous change. A problem of far greater difficulty yet remains to be solved, the possible continuity of the liquid and solid states of matter. The fine discovery made some years ago by James Thomson, of the influence of pressure on the temperature at which liquefaction occurs, and verified experimentally by Sir. W. Thomson, points, as it appears to me, to the direction this inquiry must take; and in the case at least of those bodies which expand in liquefying, and whose melting-points are raised by pressure, the transition may possibly be effected. But this must be a subject for future investigation; and for the present I will not venture to go beyond the conclusion I have already drawn from direct experiment, that the gaseous and liquid forms of matter may be transformed into one another by a series of continuous and unbroken changes.
Thomas Andrews, Philosophical Transactions of 1869
COOLING OFF
How do you make something colder? Making something hotter is easy. For example, if you need to warm yourself on a chilly night, you can build a fire with little or no technology. But to cool yourself on a hot day is quite another matter.
Hitherto we have explained the phenomena of the heavens and of our sea by the power of gravity, but have not yet assigned the cause of this power. This is certain, that it must proceed from a cause that penetrates to the very centres of the sun and planets, without suffering the least diminution of its force; that operates not according to the quantity of the surfaces of the particles upon which it acts (as mechanical causes used to do), but according to the quantity of the solid matter which they contain, and propagates its virtue on all sides to immense distances, decreasing always as the inverse square of the distances.
Isaac Newton, Printipia (1686)
THE GENESIS OF AN IDEA
The year was 1665, the month was August, and Cambridge, England, was besieged by bubonic plague. Isaac Newton, then a 23-year-old university student, retired to the solitude of his family's farm in Lincolnshire until the plague subsided and the university reopened. Not taking kindly to inactivity, Newton composed 22 questions for himself to tackle, ranging from geometric constructions to Galileo's new mechanics to Kepler's planetary laws. During the next 18 months, he immersed himself in the search for answers and along the way discovered calculus, the laws of motion, and the universal law of gravity.
And with respect to the general cause, it seems manifest to me that it is none other than God himself, who, in the beginning, created matter along with motion and rest, and now by his ordinary concourse alone preserves in the whole the same amount of motion and rest that he placed in it. For although motion is nothing in the matter moved but its mode, it has yet a certain and determinate quantity, which we easily see may remain always the same in the whole universe, although it changes in each of the parts of it.
René Descartes, Principles of Philosophy (1644)
THE UNIVERSE AS A MACHINE
In the seventeenth century science assumed its modern form and the scientific spirit infected Europe. It was then that Aristotle's view of nature was rejected and Galileo's great book of the universe was adopted. The new science was nourished by an optimism that mankind could discover the laws of nature.
One of the most significant and influential figures in seventeenth-century natural philosophy was René Descartes. Early in his life, Descartes rebelled against the traditions in which he had been thoroughly educated. He sought new foundations for knowledge, foundations which could underpin confidence in our understanding of nature. Convinced of the indubitable logic of mathematics, Descartes chose to identify mathematics with physics.
Descartes is credited with having been the first person to state the law of inertia correctly.
The initial shock [of acceleration] is the worst part of it, for he is thrown upward as if by an explosion of gun powder…. Therefore he must be dazed by opiates beforehand; his limbs must be carefully protected so that they are not torn from him and the recoil is spread over all parts of his body. Then he will meet new difficulties: immense cold and inhibited respiration…. When the first part of the journey is completed, it becomes easier because on such a long journey the body no doubt escapes the magnetic force of the earth and enters that of the moon, so that the latter gets the upper hand. At this point we set the travellers free and leave them to their own devices: like spiders they will stretch out and contract, and propel themselves forward by their own force – for, as the magnetic forces of the earth and moon both attract the body and hold it suspended, the effect is as if neither of them were attracting it – so that in the end its mass will by itself turn toward the moon.
–Johannes Kepler, Somnium, published posthumously in 1634
FREEWAYS IN THE SKY
Not many years ago, the only conceivable use of the beautiful celestial mechanics developed over hundreds of years was to compute the positions of bodies in the heavens. Today that situation has changed radically.