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3. Undergraduate Topics in Computer
Science
Series Editor
Ian Mackie, University of Sussex, Brighton, UK
Advisory Editors
Samson Abramsky , Department of Computer Science, University of Oxford,
Oxford, UK
Chris Hankin , Department of Computing, Imperial College London, London, UK
Mike Hinchey , Lero – The Irish Software Research Centre, University of
Limerick, Limerick, Ireland
Joseph Migga Kizza, The University of Tennessee–Chattanooga, College of
Engineering and Computer Science, Chattanooga, Tennessee, USA
Dexter C. Kozen, Department of Computer Science, Cornell University, Ithaca,
NY, USA
Andrew Pitts , Department of Computer Science and Technology, University of
Cambridge, Cambridge, UK
Hanne Riis Nielson , Department of Applied Mathematics and Computer Science,
Technical University of Denmark, Kongens Lyngby, Denmark
Steven S. Skiena, Department of Computer Science, Stony Brook University, Stony
Brook, NY, USA
Iain Stewart , Department of Computer Science, Durham University, Durham,
UK
4. ‘Undergraduate Topics in Computer Science’ (UTiCS) delivers high-quality
instructional content for undergraduates studying in all areas of computing and
information science. From core foundational and theoretical material to final-year
topics and applications, UTiCS books take a fresh, concise, and modern approach
and are ideal for self-study or for a one- or two-semester course. The texts are all
authored by established experts in their fields, reviewed by an international advisory
board, and contain numerous examples and problems, many of which include fully
worked solutions.
The UTiCS concept relies on high-quality, concise books in softback format, and
generally a maximum of 275–300 pages. For undergraduate textbooks that are
likely to be longer, more expository, Springer continues to offer the highly regarded
Texts in Computer Science series, to which we refer potential authors.
7. To
Past and present members of the Formal
Methods Group (Foundations and Methods
Group) at Trinity College Dublin, Ireland.
8. vii
Preface
Overview
The objective of this book is to provide a concise introduction to the software
engineering field to students and practitioners. The principles of software engi-
neering are discussed, and the goal is to give the reader a grasp of the fundamentals
of the software engineering field, as well as guidance on how to apply the theory in
an industrial environment.
Organization and Features
Chapter 1 presents a broad overview of software engineering and discusses various
software lifecycles and the activities in software development. We discuss
requirements gathering and specification, software design, implementation, testing
and maintenance. The lightweight Agile methodology is introduced, and it has
become very popular in industry.
Chapter 2 discusses the professional responsibilities of software engineers.
Engineers have a responsibility to ensure that the products that they design and
develop are built to the highest possible standards and are safe for the public to use.
Engineers must behave ethically in their dealings with their clients, and they need to
adhere to the code of ethics of the professional engineering body.
Chapter 3 discusses ethical software engineering where the ethical software
engineer needs to examine both the technical and the ethical dimensions of deci-
sions that affect wider society. We discuss the Volkswagen emissions scandal
where engineers installed a “defeat device” to enable cars to pass an emissions test.
Chapter 4 introduces project management for traditional software engineering,
and we discuss project estimation, project planning and scheduling, project moni-
toring and control, risk management, managing communication and change, and
managing project quality.
Chapter 5 discusses requirements engineering and discusses activities such as
requirements gathering, requirements elicitation, requirements analysis, require-
ments management, and requirements verification and validation.
9. viii Preface
Chapter 6 discusses software design and development, where software design is
the blueprint of the solution to be developed. It is concerned with the high-level
architecture of the system, as well as the detailed design that describes the algo-
rithms and functionality of the individual programs. The detailed design is then
implemented in a programming language such as C++ or Java. We discuss software
development topics such as software reuse, customized-off-the-shelf software
(COTS), and open-source software development.
Chapter 7 discusses software inspections, which play an important role in
building quality into a product. The well-known Fagan inspection process that was
developed at IBM in the 1970s is discussed, as well as lighter review and walk-
through methodologies.
Chapter 8 is concerned with software testing and discusses the various types of
testing that may be carried out during the project. We discuss test planning, test case
definition, test environment set-up, test execution, test tracking, test metrics, test
reporting, and testing in an e-commerce environment.
Chapter 9 discusses ethics and privacy where professional ethics are a code of
conduct that governs how members of a profession deal with each other and with
third parties. It expresses ideals of human behaviour, and the fundamental values
of the organization, and is an indication of its professionalism. Privacy is defined as
“the right to be left alone,” and specifies there should be no intrusion upon
seclusion, and no public disclosure of private facts or false information.
Chapter 10 is concerned with metrics and problem-solving, and this includes a
discussion of the balanced score card which assists in identifying appropriate
metrics for the organization. The goal, question, metrics (GQM) approach is dis-
cussed, and this allows appropriate metrics related to the organization goals to be
defined. A selection of sample metrics for an organization is presented, and
problem-solving tools such as fishbone diagrams, Pareto charts, trend charts are
discussed.
Chapter 11 is concerned with the selection and management of a software
supplier. It discusses how candidate suppliers may be identified, formally evaluated
against defined selection criteria, and how the appropriate supplier is selected. We
discuss how the selected supplier is managed during the project.
Chapter 12 discusses software configuration management and discusses the
fundamental concept of a baseline. Configuration management is concerned with
identifying those deliverables that must be subject to change control and controlling
changes to them.
Chapter 13 discusses software quality assurance and the importance of process
quality. It is a premise in the quality field that good processes and conformance to
them is essential for the delivery of high-quality product, and this chapter discusses
audits, and describes how they are carried out.
Chapter 14 discusses the Agile methodology which is a popular lightweight
approach to software development. Agile provides opportunities to assess the
direction of a project throughout the development lifecycle and ongoing changes to
requirements are considered normal in the Agile world. It has a strong collaborative
style of working, and it advocates adaptive planning and evolutionary development.
10. Preface ix
Chapter 15discusses software reliability and dependability and covers topics suchas
software reliability and software reliability models; the cleanroom methodology, sys-
tem availability; safety and security critical systems; and dependability engineering.
Chapter 16 discusses formal methods, which consist of a set of mathematical
techniques to specify and derive a program from its specification. Formal methods
may be employed to rigorously state the requirements of the proposed system. They
may be employed to derive a program from its mathematical specification, and they
may be used to provide a rigorous proof that the implemented program satisfies its
specification. They have been mainly applied to the safety critical field.
Chapter 17 presents the Z specification language, which is one of the more
popular formal methods. It was developed at the Programming Research Group at
Oxford University in the early 1980s. Z specifications are mathematical, and the use
of mathematics ensures precision and allows inconsistencies and gaps in the
specification to be identified. Theorem provers may be employed to demonstrate
that the software implementation meets its specification.
Chapter 18 presents the unified modelling language (UML), which is a visual
modelling language for software systems, and I used to present several views of the
system architecture. It was developed at Rational Corporation as a notation for
modelling object-oriented systems. We present various UML diagrams such as use
case diagrams, sequence diagrams, and activity diagrams.
Chapter 19 discusses software process improvement. It begins with a discussion
of a software process and discusses the benefits that may be gained from a software
process improvement initiative. Various models that support software process
improvement are discussed, and these include the Capability Maturity Model
Integration (CMMI), ISO 9000, Personal Software Process (PSP), and Team
Software Process (TSP).
Chapter 20 gives an overview of the CMMI model and discusses its five
maturity levels and their constituent process areas. We discuss both the staged and
continuous representations of the CMMI and SCAMPI appraisals that indicate the
extent to which the CMMI has been implemented in the organization, as well as
identifying opportunities for improvement.
Chapter 21 discusses various tools to support the various software engineering
activities. The focus is first to define the process, and then to find tools to support
the process. Tools to support project management are discussed as well as tools to
support requirements engineering, configuration management, design and devel-
opment activities, and software testing.
Chapter 22 discusses innovation in the software field including miscellaneous
topics such as distributed systems, service-oriented architecture, software as a
service, cloud computing and embedded systems. We discuss the need for inno-
vation in software engineering and discuss some recent innovations such as
aspect-oriented software engineering.
Chapter 23 is concerned with the application of the legal system to the com-
puting field. This includes the protection of intellectual property such as patents,
copyright, trademarks and trade secrets, and the resolution of disputes between
parties.
11. x Preface
Chapter 24 discusses cybersecurity and cybercrime. Cybercrime is a crime that
involves a computer and a network. The computer may be the vehicle by which the
crime was conducted, or it may be the target of the crime. Cybersecurity is con-
cerned with the ability of a computer system to protect itself from attacks, and there
are several characteristics of security such as confidentiality, integrity, and
availability.
Chapter 25 is the concluding chapter in which we summarize the journey that we
have travelled in this book.
Audience
The main audience of this book is computer science students who are interested in
learning about software engineering and in learning on how to build high-quality
and reliable software on time and on budget. It will also be of interest to indus-
trialists including software engineers, quality professionals and software managers,
as well as the motivated general reader.
Acknowledgments
I am deeply indebted to family and friends who supported my efforts in this
endeavour, and my thanks, as always, to the team at Springer. This book is dedi-
cated to present and past members of the Formal Methods Group (Foundations and
Methods Group) at Trinity College Dublin where the author spent several happy
years. I would especially like to thank Dr. Mícheál Mac An Airchinnigh,
Dr. Andrew Butterfield, Dr. Hugh Gibbons, Dr. Arthur Hughes, Alexis Donnelly,
Dara Gallagher, Eoin McDonnell, Gradamir Starovic, and Glenn Strong.
Cork, Ireland Gerard O’Regan
18. He says, moreover, “I am almost confident by circumstances, that Sir
Christopher Wren knew the duplicate proportion when I gave him a
visit; and then Mr. Hooke, by his book Cometa, will prove the last of
us three that knew it.” Hooke’s Cometa was published in 1678.
These inferences were all connected with Kepler’s law, that the times
are in the sesquiplicate ratio of the major axes of the orbits. But
Halley had also been led to the duplicate proportion by another train
of reasoning, namely, by considering the force of the sun as an
emanation, which must become more feeble in proportion to the
increased spherical surface over which it is diffused, and therefore in
the inverse proportion of the square of the distances.24
In this view
of the matter, however, the difficulty was to determine what would be
the motion of a body acted on by such a force, when the orbit is not
circular but oblong. The investigation of this case was a problem
which, we can 398 easily conceive, must have appeared of very
formidable complexity while it was unsolved, and the first of its kind.
Accordingly Halley, as his biographer says, “finding himself unable to
make it out in any geometrical way, first applied to Mr. Hooke and Sir
Christopher Wren, and meeting with no assistance from either of
them, he went to Cambridge in August (1684), to Mr. Newton, who
supplied him fully with what he had so ardently sought.”
23 Biog. Brit., art. Hooke.
24 Bullialdus, in 1645, had asserted that the force by which the
sun “prehendit et harpagat,” takes hold of and grapples the
planets, must be as the inverse square of the distance.
A paper of Halley’s in the Philosophical Transactions for January,
1686, professedly inserted as a preparation for Newton’s work,
contains some arguments against the Cartesian hypothesis of
gravity, which seem to imply that Cartesian opinions had some
19. footing among English philosophers; and we are told by Whiston,
Newton’s successor in his professorship at Cambridge, that
Cartesianism formed a part of the studies of that place. Indeed,
Rohault’s Physics was used as a classbook at that University long
after the time of which we are speaking; but the peculiar Cartesian
doctrines which it contained were soon superseded by others.
With regard, then, to this part of the discovery, that the force of the
sun follows the inverse duplicate proportion of the distances, we see
that several other persons were on the verge of it at the same time
with Newton; though he alone possessed that combination of
distinctness of thought and power of mathematical invention, which
enabled him to force his way across the barrier. But another, and so
far as we know, an earlier train of thought, led by a different path to
the same result; and it was the convergence of these two lines of
reasoning that brought the conclusion to men’s minds with irresistible
force. I speak now of the identification of the force which retains the
moon in her orbit with the force of gravity by which bodies fall at the
earth’s surface. In this comparison Newton had, so far as I am
aware, no forerunner. We are now, therefore, arrived at the point at
which the history of Newton’s great discovery properly begins.
~Additional material in the 3rd edition.~ 399
20. I
CHAPTER II.
The Inductive Epoch of Newton.—Discovery of the Universal Gravitation
of Matter, according to the Law of the Inverse Square of the Distance.
N order that we may the more clearly consider the bearing of this,
the greatest scientific discovery ever made, we shall resolve it into
the partial propositions of which it consists. Of these we may
enumerate five. The doctrine of universal gravitation asserts,
1. That the force by which the different planets are attracted to the
sun is in the inverse proportion of the squares of their distances;
2. That the force by which the same planet is attracted to the sun,
in different parts of its orbit, is also in the inverse proportion of the
squares of the distances;
3. That the earth also exerts such a force on the moon, and that
this force is identical with the force of gravity;
4. That bodies thus act on other bodies, besides those which
revolve round them; thus, that the sun exerts such a force on the
moon and satellites, and that the planets exert such forces on one
another;
5. That this force, thus exerted by the general masses of the sun,
earth, and planets, arises from the attraction of each particle of these
masses; which attraction follows the above law, and belongs to all
matter alike.
21. The history of the establishment of these five truths will be given in
order.
1. Sun’s Force on Different Planets.—With regard to the first of the
above five propositions, that the different planets are attracted to the
sun by a force which is inversely as the square of the distance,
Newton had so far been anticipated, that several persons had
discovered it to be true, or nearly true; that is, they had discovered
that if the orbits of the planets were circles, the proportions of the
central force to the inverse square of the distance would follow from
Kepler’s third law, of the sesquiplicate proportion of the periodic
times. As we have seen, Huyghens’ theorems would have proved
this, if they had been so applied; Wren knew it; Hooke not only knew
it, but claimed a prior knowledge to Newton; and Halley had satisfied
himself that it was at 400 least nearly true, before he visited Newton.
Hooke was reported to Newton at Cambridge, as having applied to
the Royal Society to do him justice with regard to his claims; but
when Halley wrote and informed Newton (in a letter dated June 29,
1686), that Hooke’s conduct “had been represented in worse colors
than it ought,” Newton inserted in his book a notice of these his
predecessors, in order, as he said, “to compose the dispute.”25
This
notice appears in a Scholium to the fourth Proposition of the
Principia, which states the general law of revolutions in circles. “The
case of the sixth corollary,” Newton there says, “obtains in the
celestial bodies, as has been separately inferred by our countrymen,
Wren, Hooke, and Halley;” he soon after names Huyghens, “who, in
his excellent treatise De Horologio Oscillatorio, compares the force
of gravity with the centrifugal forces of revolving bodies.”
25 Biog. Brit. folio, art. Hooke.
22. The two steps requisite for this discovery were, to propose the
motions of the planets as simply a mechanical problem, and to apply
mathematical reasoning so as to solve this problem, with reference
to Kepler’s third law considered as a fact. The former step was a
consequence of the mechanical discoveries of Galileo and his
school; the result of the firm and clear place which these gradually
obtained in men’s mind, and of the utter abolition of all the notions of
solid spheres by Kepler. The mathematical step required no small
mathematical powers; as appears, when we consider that this was
the first example of such a problem, and that the method of limits,
under all its forms, was at this time in its infancy, or rather, at its birth.
Accordingly, even this step, though much the easiest in the path of
deduction, no one before Newton completely executed.
2. Force in different Points of an Orbit.—The inference of the law
of the force from Kepler’s two laws concerning the elliptical motion,
was a problem quite different from the preceding, and much more
difficult; but the dispute with respect to priority in the two propositions
was intermingled. Borelli, in 1666, had, as we have seen,
endeavored to reconcile the general form of the orbit with the notion
of a central attractive force, by taking centrifugal force into the
account; and Hooke, in 1679, had asserted that the result of the law
of the inverse square in the force of the earth would be an ellipse,26
or a curve like an ellipse.27
But it does not appear that this was any
thing more than 401 a conjecture. Halley says28
that “Hooke, in 1683,
told him he had demonstrated all the laws of the celestial motions by
the reciprocally duplicate proportion of the force of gravity; but that,
being offered forty shillings by Sir Christopher Wren to produce such
a demonstration, his answer was, that he had it, but would conceal it
for some time, that others, trying and failing, might know how to
value it when he should make it public.” Halley, however, truly
23. observes, that after the publication of the demonstration in the
Principia, this reason no longer held; and adds, “I have plainly told
him, that unless he produce another differing demonstration, and let
the world judge of it, neither I nor any one else can believe it.”
26 Newton’s Letter, Biog. Brit., Hooke, p. 2660.
27 Birch’s Hist. R. S., Wallis’s Life.
28 Enc. Brit., Hooke, p. 2660.
Newton allows that Hooke’s assertions in 1679 gave occasion to
his investigation on this point of the theory. His demonstration is
contained in the second and third Sections of the Principia. He first
treats of the general law of central forces in any curve; and then, on
account, as he states, of the application to the motion of the
heavenly bodies, he treats of the case of force varying inversely as
the square of the distance, in a more diffuse manner.
In this, as in the former portion of his discovery, the two steps
were, the proposing the heavenly motions as a mechanical problem,
and the solving this problem. Borelli and Hooke had certainly made
the former step, with considerable distinctness; but the mathematical
solution required no common inventive power.
Newton seems to have been much ruffled by Hooke’s speaking
slightly of the value of this second step; and is moved in return to
deny Hooke’s pretensions with some asperity, and to assert his own.
He says, in a letter to Halley, “Borelli did something in it, and wrote
modestly; he (Hooke) has done nothing; and yet written in such a
way as if he knew, and had sufficiently hinted all but what remained
to be determined by the drudgery of calculations and observations;
excusing himself from that labor by reason of his other business;
24. whereas he should rather have excused himself by reason of his
inability; for it is very plain, by his words, he knew not how to go
about it. Now is not this very fine? Mathematicians that find out,
settle, and do all the business, must content themselves with being
nothing but dry calculators and drudges; and another that does
nothing but pretend and grasp at all things, must carry away all the
inventions, as well of those that were to follow him as of those that
402 went before.” This was written, however, under the influence of
some degree of mistake; and in a subsequent letter, Newton says,
“Now I understand he was in some respects misrepresented to me, I
wish I had spared the postscript to my last,” in which is the passage
just quoted. We see, by the melting away of rival claims, the
undivided honor which belongs to Newton, as the real discoverer of
the proposition now under notice. We may add, that in the sequel of
the third Section of the Principia, he has traced its consequences,
and solved various problems flowing from it with his usual fertility
and beauty of mathematical resource; and has there shown the
necessary connection of Kepler’s third law with his first and second.
3. Moon’s Gravity to the Earth.—Though others had considered
cosmical forces as governed by the general laws of motion, it does
not appear that they had identified such forces with the force of
terrestrial gravity. This step in Newton’s discoveries has generally
been the most spoken of by superficial thinkers; and a false kind of
interest has been attached to it, from the story of its being suggested
by the fall of an apple. The popular mind is caught by the character
of an eventful narrative which the anecdote gives to this occurrence;
and by the antithesis which makes a profound theory appear the
result of a trivial accident. How inappropriate is such a view of the
matter we shall soon see. The narrative of the progress of Newton’s
thoughts, is given by Pemberton (who had it from Newton himself) in
25. his preface to his View of Newton’s Philosophy, and by Voltaire, who
had it from Mrs. Conduit, Newton’s niece.29
“The first thoughts,” we
are told, “which gave rise to his Principia, he had when he retired
from Cambridge, in 1666, on account of the plague (he was then
twenty-four years of age). As he sat alone in a garden, he fell into a
speculation on the power of gravity; that as this power is not found
sensibly diminished at the remotest distance from the centre of the
earth to which we can rise, neither at the tops of the loftiest
buildings, nor even on the summits of the highest mountains, it
appeared to him reasonable to conclude that this power must extend
much further than was usually thought: Why not as high as the
moon? said he to himself; and if so, her motion must be influenced
by it; perhaps she is retained in her orbit thereby.”
29 Elémens de Phil. de Newton, 3me partie, chap. iii.
The thought of cosmical gravitation was thus distinctly brought into
being; and Newton’s superiority here was, that he conceived the 403
celestial motions as distinctly as the motions which took place close
to him;—considered them as of the same kind, and applied the same
rules to each, without hesitation or obscurity. But so far, this thought
was merely a guess: its occurrence showed the activity of the
thinker; but to give it any value, it required much more than a “why
not?”—a “perhaps.” Accordingly, Newton’s “why not?” was
immediately succeeded by his “if so, what then?” His reasoning was,
that if gravity reach to the moon, it is probably of the same kind as
the central force of the sun, and follows the same rule with respect to
the distance. What is this rule? We have already seen that, by
calculating from Kepler’s laws, and supposing the orbits to be circles,
the rule of the force appears to be the inverse duplicate proportion of
the distance; and this, which had been current as a conjecture
26. among the previous generation of mathematicians, Newton had
already proved by indisputable reasonings, and was thus prepared
to proceed in his train of inquiry. If, then, he went on, pursuing his
train of thought, the earth’s gravity extend to the moon, diminishing
according to the inverse square of the distance, will it, at the moon’s
orbit, be of the proper magnitude for retaining her in her path? Here
again came in calculation, and a calculation of extreme interest; for
how important and how critical was the decision which depended on
the resulting numbers? According to Newton’s calculations, made at
this time, the moon by her motion in her orbit, was deflected from the
tangent every minute through a space of thirteen feet. But by
noticing the space through which bodies would fall in one minute at
the earth’s surface, and supposing this to be diminished in the ratio
of the inverse square, it appeared that gravity would, at the moon’s
orbit, draw a body through more than fifteen feet. The difference
seems small, the approximation encouraging, the theory plausible; a
man in love with his own fancies would readily have discovered or
invented some probable cause of this difference. But Newton
acquiesced in it as a disproof of his conjecture, and “laid aside at
that time any further thoughts of this matter;” thus resigning a
favorite hypothesis, with a candor and openness to conviction not
inferior to Kepler, though his notion had been taken up on far
stronger and sounder grounds than Kepler dealt in; and without
even, so far as we know, Kepler’s regrets and struggles. Nor was
this levity or indifference; the idea, though thus laid aside, was not
finally condemned and abandoned. When Hooke, in 1679,
contradicted Newton on the subject of the curve described by a
falling body, and asserted it to be an ellipse, Newton 404 was led to
investigate the subject, and was then again conducted, by another
road, to the same law of the inverse square of the distance. This
27. naturally turned his thoughts to his former speculations. Was there
really no way of explaining the discrepancy which this law gave,
when he attempted to reduce the moon’s motion to the action of
gravity? A scientific operation then recently completed, gave the
explanation at once. He had been mistaken in the magnitude of the
earth, and consequently in the distance of the moon, which is
determined by measurements of which the earth’s radius is the base.
He had taken the common estimate, current among geographers
and seamen, that sixty English miles are contained in one degree of
latitude. But Picard, in 1670, had measured the length of a certain
portion of the meridian in France, with far greater accuracy than had
yet been attained and this measure enabled Newton to repeat his
calculations with these amended data. We may imagine the strong
curiosity which he must have felt as to the result of these
calculations. His former conjecture was now found to agree with the
phenomena to a remarkable degree of precision. This conclusion,
thus coming after long doubts and delays, and falling in with the
other results of mechanical calculation for the solar system, gave a
stamp from that moment to his opinions, and through him to those of
the whole philosophical world.
[2d Ed.] [Dr. Robison (Mechanical Philosophy, p. 288) says that
Newton having become a member of the Royal Society, there
learned the accurate measurement of the earth by Picard, differing
very much from the estimation by which he had made his
calculations in 1666. And M. Biot, in his Life of Newton, published in
the Biographie Universelle, says, “According to conjecture, about the
month of June, 1682, Newton being in London at a meeting of the
Royal Society, mention was made of the new measure of a degree of
the earth’s surface, recently executed in France by Picard; and great
28. praise was given to the care which had been employed in making
this measure exact.”
I had adopted this conjecture as a fact in my first edition; but it has
been pointed out by Prof. Rigaud (Historical Essay on the First
Publication of the Principia, 1838), that Picard’s measurement was
probably well known to the Fellows of the Royal Society as early as
1675, there being an account of the results of it given in the
Philosophical Transactions for that year. Newton appears to have
discovered the method of determining that a body might describe an
ellipse when acted upon by a force residing in the focus, and varying
405 inversely as the square of the distance, in 1679, upon occasion
of his correspondence with Hooke. In 1684, at Halley’s request, he
returned to the subject, and in February, 1685, there was inserted in
the Register of the Royal Society a paper of Newton’s (Isaaci
Newtoni Propositiones de Motu) which contained some of the
principal Propositions of the first two Books of the Principia. This
paper, however, does not contain the Proposition “Lunam gravitare in
terram,” nor any of the other propositions of the third Book. The
Principia was printed in 1686 and 7, apparently at the expense of
Halley. On the 6th of April, 1687, the third Book was presented to the
Royal Society.]
It does not appear, I think, that before Newton, philosophers in
general had supposed that terrestrial gravity was the very force by
which the moon’s motions are produced. Men had, as we have seen,
taken up the conception of such forces, and had probably called
them gravity: but this was done only to explain, by analogy, what
kind of forces they were, just as at other times they compared them
with magnetism; and it did not imply that terrestrial gravity was a
force which acted in the celestial spaces. After Newton had
29. discovered that this was so, the application of the term “gravity” did
undoubtedly convey such a suggestion; but we should err if we
inferred from this coincidence of expression that the notion was
commonly entertained before him. Thus Huyghens appears to use
language which may be mistaken, when he says,30
that Borelli was
of opinion that the primary planets were urged by “gravity” towards
the sun, and the satellites towards the primaries. The notion of
terrestrial gravity, as being actually a cosmical force, is foreign to all
Borelli’s speculations.31
But Horrox, as early as 1635, appears to
have entertained the true view on this subject, although vitiated by
Keplerian errors concerning the connection between the rotation of
the central body and its effect on the body which revolves about it.
Thus he says,32
that the emanation of the earth carries a projected
stone along with the motion of the earth, just in the same way as it
carries the moon in her orbit; and that this force is greater on the
stone than on the moon, because the distance is less.
30 Cosmotheoros, l. 2. p. 720.
31 I have found no instance in which the word is so used by him.
32 Astronomia Kepleriana defensa et promota, cap. 2. See further
on this subject in the Additions to this volume.
The Proposition in which Newton has stated the discovery of
which we are now speaking, is the fourth of his third Book: “That the
moon gravitates to the earth, and by the force of gravity is
perpetually 406 deflected from a rectilinear motion, and retained in
her orbit.” The proof consists in the numerical calculation, of which
he only gives the elements, and points out the method; but we may
observe, that no small degree of knowledge of the way in which
astronomers had obtained these elements, and judgment in
30. selecting among them, were necessary: thus, the mean distance of
the moon had been made as little as fifty-six and a half
semidiameters of the earth by Tycho, and as much as sixty-two and
a half by Kircher: Newton gives good reasons for adopting sixty-one.
The term “gravity,” and the expression “to gravitate,” which, as we
have just seen, Newton uses of the moon, were to receive a still
wider application in consequence of his discoveries; but in order to
make this extension clearer, we consider it as a separate step.
~Additional material in the 3rd edition.~
4. Mutual Attraction of all the Celestial Bodies.—If the preceding
parts of the discovery of gravitation were comparatively easy to
conjecture, and difficult to prove, this was much more the case with
the part of which we have now to speak, the attraction of other
bodies, besides the central ones, upon the planets and satellites. If
the mathematical calculation of the unmixed effect of a central force
required transcendent talents, how much must the difficulty be
increased, when other influences prevented those first results from
being accurately verified, while the deviations from accuracy were far
more complex than the original action! If it had not been that these
deviations, though surprisingly numerous and complicated in their
nature, were very small in their quantity, it would have been
impossible for the intellect of man to deal with the subject; as it was,
the struggle with its difficulties is even now a matter of wonder.
The conjecture that there is some mutual action of the planets,
had been put forth by Hooke in his Attempt to prove the Motion of
the Earth (1674). It followed, he said, from his doctrine, that not only
the sun and moon act upon the course and motion of the earth, but
that Mercury, Venus, Mars, Jupiter, and Saturn, have also, by their
31. attractive power, a considerable influence upon the motion of the
earth, and the earth in like manner powerfully affects the motions of
those bodies. And Borelli, in attempting to form “theories” of the
satellites of Jupiter, had seen, though dimly and confusedly, the
probability that the sun would disturb the motions of these bodies.
Thus he says (cap. 14), “How can we believe that the Medicean
globes are not, like other planets, impelled with a greater velocity
when they approach the sun: and thus they are acted upon by two
moving forces, one of 407 which produces their proper revolution
about Jupiter, the other regulates their motion round the sun.” And in
another place (cap. 20), he attempts to show an effect of this
principle upon the inclination of the orbit; though, as might be
expected, without any real result.
The case which most obviously suggests the notion that the sun
exerts a power to disturb the motions of secondary planets about
primary ones, might seem to be our own moon; for the great
inequalities which had hitherto been discovered, had all, except the
first, or elliptical anomaly, a reference to the position of the sun.
Nevertheless, I do not know that any one had attempted thus to
explain the curiously irregular course of the earth’s attendant. To
calculate, from the disturbing agency, the amount of the
irregularities, was a problem which could not, at any former period,
have been dreamt of as likely to be at any time within the verge of
human power.
Newton both made the step of inferring that there were such
forces, and, to a very great extent, calculated the effects of them.
The inference is made on mechanical principles, in the sixth
Theorem of the third Book of the Principia;—that the moon is
attracted by the sun, as the earth is;—that the satellites of Jupiter
32. and Saturn are attracted as the primaries are; in the same manner,
and with the same forces. If this were not so, it is shown that these
attendant bodies could not accompany the principal ones in the
regular manner in which they do. All those bodies at equal distances
from the sun would be equally attracted.
But the complexity which must occur in tracing the results of this
principle will easily be seen. The satellite and the primary, though
nearly at the same distance, and in the same direction, from the sun,
are not exactly so. Moreover the difference of the distances and of
the directions is perpetually changing; and if the motion of the
satellite be elliptical, the cycle of change is long and intricate: on this
account alone the effects of the sun’s action will inevitably follow
cycles as long and as perplexed as those of the positions. But on
another account they will be still more complicated; for in the
continued action of a force, the effect which takes place at first,
modifies and alters the effect afterwards. The result at any moment
is the sum of the results in preceding instants: and since the terms,
in this series of instantaneous effects, follow very complex rules, the
sums of such series will be, it might be expected, utterly incapable of
being reduced to any manageable degree of simplicity.
It certainly does not appear that any one but Newton could make
408 any impression on this problem, or course of problems. No one
for sixty years after the publication of the Principia, and, with
Newton’s methods, no one up to the present day, had added any
thing of any value to his deductions. We know that he calculated all
the principal lunar inequalities; in many of the cases, he has given us
his processes; in others, only his results. But who has presented, in
his beautiful geometry, or deduced from his simple principles, any of
the inequalities which he left untouched? The ponderous instrument
33. of synthesis, so effective in his hands, has never since been grasped
by one who could use it for such purposes; and we gaze at it with
admiring curiosity, as on some gigantic implement of war, which
stands idle among the memorials of ancient days, and makes us
wonder what manner of man he was who could wield as a weapon
what we can hardly lift as a burden.
It is not necessary to point out in detail the sagacity and skill which
mark this part of the Principia. The mode in which the author obtains
the effect of a disturbing force in producing a motion of the apse of
an elliptical orbit (the ninth Section of the first Book), has always
been admired for its ingenuity and elegance. The general statement
of the nature of the principal inequalities produced by the sun in the
motion of a satellite, given in the sixty-sixth Proposition, is, even yet,
one of the best explanations of such action; and the calculations of
the quantity of the effects in the third Book, for instance, the variation
of the moon, the motion of the nodes and its inequalities, the change
of inclination of the orbit,—are full of beautiful and efficacious
artifices. But Newton’s inventive faculty was exercised to an extent
greater than these published investigations show. In several cases
he has suppressed the demonstration of his method, and given us
the result only; either from haste or from mere weariness, which
might well overtake one who, while he was struggling with facts and
numbers, with difficulties of conception and practice, was aiming also
at that geometrical elegance of exposition, which he considered as
alone fit for the public eye. Thus, in stating the effect of the
eccentricity of the moon’s orbit upon the motion of the apogee, he
says,33
“The computations, as too intricate and embarrassed with
approximations, I do not choose to introduce.”
33 Schol. to Prop. 35, first edit.
34. The computations of the theoretical motion of the moon being thus
difficult, and its irregularities numerous and complex, we may ask 409
whether Newton’s reasoning was sufficient to establish this part of
his theory; namely, that her actual motions arise from her gravitation
to the sun. And to this we may reply, that it was sufficient for that
purpose,—since it showed that, from Newton’s hypothesis,
inequalities must result, following the laws which the moon’s
inequalities were known to follow;—since the amount of the
inequalities given by the theory agreed nearly with the rules which
astronomers had collected from observation;—and since, by the very
intricacy of the calculation, it was rendered probable, that the first
results might be somewhat inaccurate, and thus might give rise to
the still remaining differences between the calculations and the facts.
A Progression of the Apogee; a Regression of the Nodes; and,
besides the Elliptical, or first Inequality, an inequality, following the
law of the Evection, or second inequality discovered by Ptolemy;
another, following the law of the Variation discovered by Tycho;—
were pointed out in the first edition of the Principia, as the
consequences of the theory. Moreover, the quantities of these
inequalities were calculated and compared with observation with the
utmost confidence, and the agreement in most instances was
striking. The Variation agreed with Halley’s recent observations
within a minute of a degree.34
The Mean Motion of the Nodes in a
year agreed within less than one-hundredth of the whole.35
The
Equation of the Motion of the Nodes also agreed well.36
The
Inclination of the Plane of the Orbit to the ecliptic, and its changes,
according to the different situations of the nodes, likewise agreed.37
The Evection has been already noticed as encumbered with peculiar
difficulties: here the accordance was less close. The Difference of
the daily progress of the Apogee in syzygy, and its daily Regress in
35. Quadratures, is, Newton says, “4¼ minutes by the Tables, 6⅔ by our
calculation.” He boldly adds, “I suspect this difference to be due to
the fault of the Tables.” In the second edition (1711) he added the
calculation of several other inequalities, as the Annual Equation, also
discovered by Tycho; and he compared them with more recent
observations made by Flamsteed at Greenwich; but even in what
has already been stated, it must be allowed that there is a wonderful
accordance of theory with phenomena, both being very complex in
the rules which they educe.
34 B. iii. Prop. 29.
35 Prop. 32.
36 Prop. 33.
37 Prop. 35.
The same theory which gave these Inequalities in the motion of
the Moon produced by the disturbing force of the sun, gave also 410
corresponding Inequalities in the motions of the Satellites of other
planets, arising from the same cause; and likewise pointed out the
necessary existence of irregularities in the motions of the Planets
arising from their mutual attraction. Newton gave propositions by
which the Irregularities of the motion of Jupiter’s moons might be
deduced from those of our own;38
and it was shown that the motions
of their nodes would be slow by theory, as Flamsteed had found it to
be by observation.39
But Newton did not attempt to calculate the
effect of the mutual action of the planets, though he observes, that in
the case of Jupiter and Saturn this effect is too considerable to be
neglected;40
and he notices in the second edition,41
that it follows
from the theory of gravity, that the aphelia of Mercury, Venus, the
Earth, and Mars, slightly progress.
36. 38 B. i. Prop. 66.
39 B. iii. Prop. 23.
40 B. iii. Prop. 13.
41 Scholium to Prop. 14. B. iii.
In one celebrated instance, indeed, the deviation of the theory of
the Principia from observation was wider, and more difficult to
explain; and as this deviation for a time resisted the analysis of Euler
and Clairaut, as it had resisted the synthesis of Newton, it at one
period staggered the faith of mathematicians in the exactness of the
law of the inverse square of the distance. I speak of the Motion of the
Moon’s Apogee, a problem which has already been referred to; and
in which Newton’s method, and all the methods which could be
devised for some time afterwards, gave only half the observed
motion; a circumstance which arose, as was discovered by Clairaut
in 1750, from the insufficiency of the method of approximation.
Newton does not attempt to conceal this discrepancy. After
calculating what the motion of apse would be, upon the assumption
of a disturbing force of the same amount as that which the sun
exerts on the moon, he simply says,42
“the apse of the moon moves
about twice as fast.”
42 B. i. Prop. 44, second edit. There is reason to believe,
however, that Newton had, in his unpublished calculations,
rectified this discrepancy.
The difficulty of doing what Newton did in this branch of the
subject, and the powers it must have required, may be judged of
from what has already been stated;—that no one, with his methods,
has yet been able to add any thing to his labors: few have
undertaken to illustrate what he has written, and no great number
37. have understood it throughout. The extreme complication of the
forces, and of the conditions under which they act, makes the
subject by far the most thorny walk of mathematics. It is necessary to
resolve the action 411 into many elements, such as can be
separated; to invent artifices for dealing with each of these; and then
to recompound the laws thus obtained into one common conception.
The moon’s motion cannot be conceived without comprehending a
scheme more complex than the Ptolemaic epicycles and eccentrics
in their worst form; and the component parts of the system are not, in
this instance, mere geometrical ideas, requiring only a distinct
apprehension of relations of space in order to hold them securely;
they are the foundations of mechanical notions, and require to be
grasped so that we can apply to them sound mechanical reasonings.
Newton’s successors, in the next generation, abandoned the hope of
imitating him in this intense mental effort; they gave the subject over
to the operation of algebraical reasoning, in which symbols think for
us, without our dwelling constantly upon their meaning, and obtain
for us the consequences which result from the relations of space and
the laws of force, however complicated be the conditions under
which they are combined. Even Newton’s countrymen, though they
were long before they applied themselves to the method thus
opposed to his, did not produce any thing which showed that they
had mastered, or could retrace, the Newtonian investigations.
Thus the Problem of Three Bodies,43
treated geometrically,
belongs exclusively to Newton; and the proofs of the mutual action of
the sun, planets, and satellites, which depend upon such reasoning,
could not be discovered by any one but him.
43 See the history of the Problem of Three Bodies, ante, in Book
vi. Chap. vi. Sect. 7.