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.
We study the equation a2−2b6=cp and its specialization a2−2=cp, where p is a prime, using the modular method. In particular, we use a ℚ-curve defined over for which the solution (a,b,c)=(±1,±1,−1) gives rise to a CM-form. This allows us to apply the modular method to resolve the equation a2−2b6=cp for p in certain congruence classes. For the specialization a2−2=cp, we use the multi-Frey technique of Siksek to obtain further refined results.
We perform an almost sure linear stability analysis of the θ-Maruyama method, selecting as our test equation a two-dimensional system of Itô differential equations with diagonal drift coefficient and two independent stochastic perturbations which capture the stabilising and destabilising roles of feedback geometry in the almost sure asymptotic stability of the equilibrium solution. For small values of the constant step-size parameter, we derive close-to-sharp conditions for the almost sure asymptotic stability and instability of the equilibrium solution of the discretisation that match those of the original test system. Our investigation demonstrates the use of a discrete form of the Itô formula in the context of an almost sure linear stability analysis.
Let p and r be two primes, and letn and m be two distinct divisors ofpr. Consider Φn and Φm, the nth and mth cyclotomicpolynomials. In this paper, we present lower and upper bounds for thecoefficients of the inverse of Φn modulo Φm and discuss an application to torus-based cryptography.
The existence of products of three pairwise coprime integers is investigated in short intervals of the form . A general theorem is proved which shows that such integer products exist provided there is a bound on the product of any two of them. A particular case of relevance to elliptic curve cryptography, where all three integers are of order , is presented as a corollary to this result.
We test R. van Luijk’s method for computing the Picard group of a K3 surface. The examples considered are the resolutions of Kummer quartics in ℙ3. Using the theory of abelian varieties, the Picard group may be computed directly in this case. Our experiments show that the upper bounds provided by van Luijk’s method are sharp when sufficiently many primes are used. In fact, there are a lot of primes that yield a value close to the exact one. However, for many but not all Kummer surfaces V of Picard rank 18, we have for a set of primes of density at least 1/2.
Let G be a group generated by k elements, G=〈g1,…,gk〉, with group operations (multiplication, inversion and comparison with identity) performed by a black box. We prove that one can test whether the group G is abelian at a cost of O(k) group operations. On the other hand, we show that a deterministic approach requires Ω(k2) group operations.
The ability to summarise data, compare models and apply computer-based analysis tools are vital skills necessary for studying and working in the physical sciences. This textbook supports undergraduate students as they develop and enhance these skills. Introducing data analysis techniques, this textbook pays particular attention to the internationally recognised guidelines for calculating and expressing measurement uncertainty. This new edition has been revised to incorporate Excel® 2010. It also provides a practical approach to fitting models to data using non-linear least squares, a powerful technique which can be applied to many types of model. Worked examples using actual experimental data help students understand how the calculations apply to real situations. Over 200 in-text exercises and end-of-chapter problems give students the opportunity to use the techniques themselves and gain confidence in applying them. Answers to the exercises and problems are given at the end of the book.
In chapter 3 we considered the normal distribution largely due to its similarityto the distribution of data observed in many experiments involving repeatmeasurements of a quantity. In particular, the normal distribution is useful fordescribing the spread of values when continuous quantities such as temperatureor time interval are measured.
Another important category of experiment involves counting. As examples, we maycount the number of electrons scattered by a gas, the number of charge carriersthermally generated in an electronic device, or the number of beta particlesemitted by a radioactive source. In these situations, distributions thatdescribe discrete quantities must be considered. In this chapter we consider twosuch distributions important in science: the binomial and Poissondistributions.
The binomial distribution
One type of experiment involving discrete variables entails removing an objectfrom a population and classifying that object in one of a finite number of ways.For example, we might test an electrical component and classify it‘within specification’ or ‘outside specification’.Owing to the underlying (and possibly unknown) processes causing components tofail to meet the specification, we can only give a probability that anyparticular component tested will satisfy the specification. Whenn objects are removed from a population and tested, or whena coin is tossed n times, we speak of performingn trials. The result of a test (e.g. ‘pass’)or the result of a coin toss (e.g. ‘head’) is referred to as anoutcome.
I thank Cambridge University Press, and in particular Simon Capelin, for the opportunity to revisit Data Analysis with Excel. I have revised sections of the book to include topics of contemporary relevance to undergraduate students, particularly in the area of uncertainty in measurement. I hope the book will continue to assist in developing the quantitative skills of students destined to graduate in the physical sciences. There is little doubt that the demand for such skills will continue to grow in society in general and particularly within industry, research, education and commerce.
This edition builds on the first with a new chapter added and others undergoing major or minor modifications (for example, to remedy mistakes, update references or include more end of chapter exercises).
We may believe that the ‘laws of chance’ that apply when tossing a coin or rolling dice have little to do with experiments carried out in a laboratory. Rolling dice and tossing coins are the stuff of games. Surely, well planned and executed experiments provide precise and reliable data, immune from the laws of chance. Not so. Chance, or what we refer to more formally as probability, has rather a large role to play in every experiment. This is true whether an experiment involves counting the number of beta particles detected by nuclear counting apparatus in one minute, measuring the time a ball takes to fall a distance through a liquid or determining the values of resistance of 100 resistors supplied by a component manufacturer. Because it is not possible to predict with certainty what value will emerge when a measurement is made of a quantity, say of the time for a ball to fall a fixed distance through liquid, we are in a similar position to a person throwing several dice, who cannot know in advance which numbers will appear ‘face up’. If we are not to give up in frustration at our inability to discover the ‘exact’ value of a quantity experimentally, we need to find out more about probability and how it can assist rather than hamper our experimental studies.
In many situations a characteristic pattern or distribution emerges in data gathered when repeat measurements are made of a quantity. A distribution of values indicates that there is a probability associated with the occurrence of any particular value. Related to any distribution of ‘real’ data there is a probability distribution which allows us to calculate the probability of the occurrence of any particular value. Real probability distributions can often be approximated by a ‘theoretical’ probability distribution. Though it is possible to devise many theoretical probability distributions, it is the so called ‘normal’ probability distribution (also referred to as the Gaussian distribution) that is most widely used. This is because histograms of data obtained in many experiments have shapes that are very similar to that of the normal distribution. An attraction of the normal and other distributions is that they provide a way of describing data in a quantitative manner which complements and extends visual representations of data such as the histogram. Using the properties of the normal distribution we are usually able to summarise a whole data set, which may consist of many values, by one or two carefully chosen numbers.
Establishing and understanding the relationship between quantities are principal goals in the physical sciences. As examples, we might be keen to know how the:
size of a crystal depends on the growth time of the crystal;
output intensity of a light emitting diode varies with the emission wavelength;
amount of light absorbed by a chemical species depends on the species concentration;
electrical power supplied by a solar cell varies with optical power incident on the cell;
viscosity of an engine oil depends upon the temperature of the oil;
rate of flow of a fluid through a hollow tube depends on the internal diameter of the tube.
Once an experiment is complete and the data presented in the form of an x–y graph, an examination of the data assists in answering important qualitative questions such as: Is there evidence of a clear trend in the data? If so, is that trend linear, and do any of the data conflict with the general trend? A qualitative analysis often suggests which quantitative methods of analysis to apply.
There are many situations in the physical sciences in which prior knowledge or experience suggests a relationship between measured quantities. Perhaps we are already aware of an equation which predicts how one quantity depends on another. Our goal in this situation might be to discover how well the equation can be made to ‘fit’ the data.