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Excerpts from A Treatise of Fluxions
Maclaurin's Original Text & Analysis (1742) 

Both Volume I and Volume II of Colin Maclaurin's "A Treatise of Fluxions" can now be accessed online via Google Books. (Check out Wolfram's explanation of the term, fluxion.) In what follows, we provide an abbreviated table of contents for both volumes and present selected excerpts from these volumes.
Title Pages with GoogleBooks Links 


As is illustrated by the images displayed in the following two panels (click in one of the panels in order to view a higherresolution image), each published "Figure Plate" was digitized (by Google Books) in segments that must be digitally pieced together in order to reconstruct some of the individual figures. See, for example, the discussion that references Fig. 282, below.
Example Digitized Figure Plates 


Plate XXXII 
Plate XXXIII 
Volume I
Dedication (an 18^{th} Century Acknowledgment)  
Preface  
Introduction  1 
Book 1 (Of the Fluxions of Geometrical Magnitudes)  51 
Chapter I (Of the Grounds of this Method) — §§ 177  51 
Chapter II (Of the Fluxions of plane rectilineal Figures) — §§ 78104  109 
Chapter III (Of the Fluxions of plane curvilineal Figures) — §§ 105123  131 
Chapter IV (Of the Fluxions of Solids, and of third Fluxions) — §§ 124139  142 
Chapter V (Of the Fluxions of Quantities that are in a continued Geometrical Progression, the first term of which is invariable) — §§ 140150  152 
Chapter VI (Of Logarithms, and of the Fluxions of logarithmic Quantities) — §§ 151179  158 
Chapter VII (Of the Tangents of curve Lines) — §§ 180214  178 
Chapter VIII (Of the Fluxions of curve Surfaces) — §§ 215237  199 
Chapter IX ([Identifying Extrema and Inflection Points] of Curves that are defined by a common or by a fluxional Equation) — §§ 238285  214 
Chapter X (Of the Asymptotes of curve Lines, the Areas bounded by them and …) — §§ 286362  240 
Chapter XI (Of the Curvature of Lines … different kinds of Contact [with other Curves] … Caustics … centripetal Forces …) — §§ 363  304 
· Parabola — §371  311 
· Any Conic Section — §373  312 
· The Second Fluxion of a Curve — §384  324 
· Refraction of Light — §413  344 
· Centripetal and Centrifugal Forces — §416  346 
· Gravity — §419  348 
· Circular Motion — §432  356 
· When the Center of Forces is the Focus of a Conic Section — §446  370 
· When Gravity is Uniform or Varies as any Power of the Distance — §458  383 
· Orbit of the Moon, taking into account the Gravity of both the Earth and the Sun — §471  391 
· Prolate Spheroidal Fluid Figure — §491  409 
· The Earth's Equilibrium Shape — §492  410 
End of Book I, Chapter XI, § 494  413 
Volume II
Table of Principal Contents (5 pp.)  
Figure Plates (30 pp.)  
Book 1 (continued)  1 
Chapter XII (Of the Methods of Infinitesimals …) — §§ 495570  1 
· Centre of Gravity — §510  13 
· Of the Collision of Bodies — §511  14 
· Of the Descent of Bodies that Act upon One Another — §521  27 
· Of the Centre of Oscillation — §533  40 
· Of the Motion of Water Issuing from a Cylindric Vessel — §537  44 
· Of the Catenaria — §551  59 
· General Observations Concerning the Angles of Contact, etc. — §554  61 
· General Observations Concerning centripetal Forces, etc. — §563  67 
Chapter XIII (Determining the Lines of swiftest Descent in any Hypothesis of Gravity …) — §§ 571608  74 
· When Gravity is Directed Towards a Given Centre — §578  80 
· Isoperimetrical Problems — §588  88 
· The Solid of Least Resistance — §606  100 
Chapter XIV (Of the Ellipse Considered as the Section of a Cylinder … Of the Figure of the Earth …) — §§ 609  101 
· Properties of the Ellipse — §609  101 
· Of the Gravitation towards Spheres and Spheroids — §628  110 
· Of the Figures of Planets (including effects of rotation) — §636  116 
· Key Concluding Theorem! — §641  119 
· Using geometric relations, illustrate how to quantitatively determine gravitational acceleration …  
[see related comment by Todhunter (1873), below]  
▸ due to an arbitrarily shaped, uniformdensity configuration — §642  120 
▸ outside or on the surface of a uniformdensity sphere — §643  121 
▸ at the pole of an oblate spheroid — §644  122 
▸ at the equator of an oblate spheroid — §645  123 
▸ at both the pole and the equator of an oblong (i.e., prolate) spheroid — §647  125 
▸ due to a pair of concentric, confocal spheroids — §648  127 
· Apply Specifically to the Earth — §661  136 
· What if the Earth's Density isn't Uniform but, instead, Varies Linearly with Distance? — §670  143 
· Jupiter — §682  152 
· Tides — §686  154 
· Concluding Paragraph — §696  161 
End of Book I  162 
Maclaurin's Discussion of SelfGravitating, OblateSpheroidal Configurations
Paragraph (and related figure) extracted^{†} from Colin Maclaurin (1742)  
^{†}As displayed here (left panel), this paragraph has been pieced together from two text segments found on separate but sequential pages (pp. 110111) of Google's digitized volume. The diagram labeled Fig. 283 (topright panel) has been extracted from Maclaurin's Figure Plate XXXIII, which appears near the beginning of the same digitized file, and has been displayed here without modification. The diagrams in the bottomright panel have been reposted from Mathalino.com in an effort to illustrate what Maclaurin means by "frustum of a cone." 
Paragraph (and a pair of related diagrams) extracted^{†} from Colin Maclaurin (1742)
"A Treatise of Fluxions"
Volume II, Chapter XIV, §630  
^{†}The paragraph (left panel) has been extracted from p. 111 of Google's digitized volume and displayed here without modification. The pair of diagrams (right panel) has been extracted from Figure Plate XXXIII, which appears near the beginning of the same digitized file. Note that the diagram on the right has been (poorly) pieced together from segments that appear on two separate pages of Google's digitized volume, presumably because the figure plate, itself, is folded in the original print publication. 
Interpreting Maclaurin's Key Concluding Theorem
As noted above, in line with the table of contents for Volume II, the key theorem resulting from Maclaurin's analysis is …
Here we assess this geometrically formulated statement using today's more common differential operators and algebraic expressions. In particular, we draw from the discussion of Maclaurin spheroids that has been presented in an accompanying chapter of this H_Book.
CA: This is the semiminor (polar) axis of the spheroid, which we have called, .
CD: This is the semimajor (equatorial) radius of the spheroid, which we have called, .
With both and specified, the eccentricity of the oblate spheroid is also known via the expression,
Attraction of the Spheroid at the Pole: We interpret this phrase to mean the magnitude of the acceleration (force per unit mass) due to gravity at the pole, which is,





Attraction at the Circumference of the Equator: We interpret this phrase to mean the magnitude of the acceleration (force per unit mass) due to gravity in the equatorial plane, at the surface of the configuration, which is,





Centrifugal force in the equatorial plane arising from rotation: We interpret this phrase to mean the centrifugal acceleration (force per unit mass) given by the expression,



Maclaurin's theorem states that the rotating spheroidal configuration will be in equilibrium if,



or, equivalently,



We choose to rewrite this expression and label it as,
Maclaurin's Theorem
which, in our terminology, becomes






This is precisely the equilibrium frequency that we have derived elsewhere, from an evaluation of the gravitational potential of uniformdensity spheroids.
Prolate Spheroid
As one specific example, Maclaurin discusses the gravitational attraction at the pole of a uniformdensity, prolate spheroid in his §647 of Volume II (pp. 125127). While his discussion of this topic necessarily refers back to earlier sections — most importantly, §643 (spheres) and §644 (oblate spheroids) — it frequently refers to Figure 291, No. 2, which we have reproduced in the following figure.
Figure extracted^{†} from Colin Maclaurin (1742)  
^{†}The . 
In this animation sequence, the blue ellipse has an eccentricity, , and the red linesegment is drawn at an angle to the horizontal axis that varies over the range, . As is described in the accompanying text, the orange curve — Maclaurin's "AKG" curve — is mapped out as the angle, , is varied. 
While trying to decipher Maclaurin's geometrically based derivation, we have found it useful to redraw key elements of this figure, deriving relevant algebraic or trigonometric relations along the way. Because the "oblong" ellipse in Maclaurin's figure is oriented such that the axis of revolution — the symmetry axis — is horizontal, and because we prefer to associate the axis with the symmetry axis of the configuration, we will rather unconventionally refer to the horizontal axis as the (symmetry) axis. Adopting a cylindrical coordinate system furthermore means that, in our notation, the vertical axis will be the axis.
The blue ellipse centered on the origin of our plot represents Maclaurin's "ADBE" ellipse; in the expressions that follow, we will use and to refer, respectively, to the length of the semimajor axis (Maclaurin's linesegment "CA") and semiminor axis (Maclaurin's linesegment "CD") of the ellipse; and, following Maclaurin, we will refer to the leftmost point on the ellipse (Maclaurin's point "A") as the "pole" which is positioned at coordinate . (Note that in our plot, we have set , but otherwise we will leave its specification arbitrary.) In our plot, Maclaurin's "CNH" circle is represented by the green quarter circle centered on the pole. The blue ellipse is defined by the relation,






and, because it is offcenter, the green quarter circle is defined by the relation,






The red linesegment in our plot is what Maclaurin refers to as "AM" which, in his words, is any right line from the pole A. We will use the variable, , to identify the angle between this linesegment and the horizontal axis; in determining the gravitational attraction at pole A, Maclaurin ultimately sweeps this angle through the range, . Points lying along this line are defined by the relation,






Intersection With Circle
Hence, the red linesegment intersects the green quartercircle when,












Correspondingly,
Intersection With Ellipse
Similarly, the red linesegment intersects the blue ellipse when,









The roots of this quadratic equation are,












The "inferior" root gives,
while the "superior" root gives,



Correspondingly,
and,
The "inferior" root clearly identifies the intersection of the red linesegment with the pole of the prolate spheroid. The "superior" root identifies the point at which the red linesegment intersects and crosses the blue ellipse, away from the pole.
Generate Curve AKG
In §644 (p. 122 of Volume II) of his Treatise, Maclaurin states that "the gravity at the pole A towards the spheroid ADBE will be measured by [the ratio],"
where the numerator, "AKGC," is the area under the curve, "AKG," and the denominator is the length of the semimajor axis, . So a key element of Maclaurin's derivation is the proper construction of the curve, "AKG." The key sentence from his §644 appears to be the following:
We interpret this phrase to mean that, as the angle, , varies from to , the curve "AKG" is generated by plotting, as the ordinate, the length of the linesegment "AQ" and, as the abscissa, the coordinate location of the vertical line, "RN" — we'll label this, . In our terminology, as derived above, is the coordinate of the intersection of the red linesegment with the green quartercircle, that is,



And the magnitude of "AQ" is obtained from the coordinate location of the vertical line, "MQ" — that is, the coordinate of the intersection of the red linesegment with the blue ellipse — as derived above. Specifically, we interpret Maclaurin's phrase to mean that,



Using the first of these two expressions, we can rewrite the tangent function directly in terms of the ordinate, ; specifically,
Hence,


















In our above figure, this function, normalized to , is delineated by the orange triangles over the coordinate range, . If our interpretation of Maclaurin's discussion is correct, this is precisely the curve in Maclauin's Figure 291, No. 2 that is labeled, "AKG."
Area Under the Curve
The area, "AKGC" — which, according to Maclaurin, gives the gravitational acceleration at the pole A — can be determined by carrying out the integral,



This integral can be more cleanly evaluated if we make the variable substitution,
with a corresponding shift in the limits of integration from , for , to , for . Specifically, we find,












This is precisely the expression for the coefficient, , that is traditionally used in the expression for the gravitational potential inside homogeneous, prolate spheroids.
Material that appears after this point in our presentation is under development and therefore
may contain incorrect mathematical equations and/or physical misinterpretations.
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Comparison With More Traditional Derivation
In our separate derivation of the gravitational acceleration at the pole of a prolate spheroid that uses a more traditional approach, we obtained this key coefficient by integrating over a different function, namely,






By comparing Maclaurin's approach to the more traditional one, we conclude that,



We should be able to demonstrate explicitly that these two integrands are the same. We begin by recognizing that the relationship between the dimensionless coordinate, , that we have used to decipher Maclaurin's presentation and the dimensionless coordinate, , that was used in our separate analysis, is,
Returning to the first expression in the above subsection that details the intersection of the red linesegment with the blue ellipse, we can therefore write,






Recalling that,
we see that,












Furthermore, we see that the transformation from to is,


















Putting these two expressions together, we conclude that the integrand is,









This does not appear to match the other integrand. I must be misinterpreting something!
To be done: I suspect that Maclaurin's approach will look more familiar if I redo the "traditional" derivation from the point of view of a spherical coordinate system (positioning pole A at the origin), in which an axisymmetric volume element takes the form,
where, from above,
See Also
 Our review of the Properties of Homogeneous Ellipsoids
 Our derivation of the properties of Maclaurin Spheriods
 Wikipedia's documentation of Colin Maclaurin
 Chandrasekhar's (1967) historical account
 Notes on the Life and Works of colin Maclaurin by Charles Tweedie (1919)
 I. Todhunter (1873), A History of the Mathematical Theories of Attraction and the Figure of the Earth, from the time of Newton to that of Laplace. Note that Todhunter's discussion of Maclaurin's contributions can be found in Chapter IX, pp. 133175.
Extracted from §252 of I. Todhunter (1873)
252. "Maclaurin then in his Articles 644 … 647 investigates accurate expressions for the attraction of any ellipsoid of revolution on a particle at the pole or at the equator. The investigations are conducted in the manner of the time by representing the attractions by the areas of certain curves, and finding the areas by the method of fluents. The results agree with those obtained by analysis, and presented in modern works on Statics. Maclaurin's processes are remarkable specimens of ingenuity, considering the date of their publication; but they will not be very interesting to a modern reader." 
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