Chapter VI: Appendix

NEW SLIDE RULES—FIFTH ROOTS, ETC.—THE SOLUTION OF ALGEBRAIC EQUATIONS—GAUGE POINTS AND SIGNS ON SLIDE RULES—TABLES AND DATA—SLIDE RULE DATA SLIPS.

THE PICKWORTH SLIDE RULE.—In this rule, made by Mr. A. W. Faber, the novel feature is the provision of a scale of cubes (F) in the stock or body of the rule. From Fig. 33 it will be seen that the scale is fixed on the bevelled side of a slotted recess in the back of the rule. The slide carries an index mark, which is seen through the slot and can be set to any graduation of the scale; in its normal position it agrees with 1 on the scale. The C scale on the face of the rule is divided into three equal parts by two special division lines, marked II. and III., which, together with the initial graduation 1 of the scale, serve for setting or reading off values on the D scale. Similar division lines are marked on the D scale.

In using the rule for cubes or cube roots the slide is drawn to the right, this movement never exceeding one-third of the length of the D scale. With this limited movement, and with a single setting of the slide, the values of ∛_̅a_, ∛(_a_ × 10), and ∛(_a_ × 100)) (_a_ being less than 10 and not less than 1) are given simultaneously and without any uncertainty as to the scales to use or the values to be read off.

_To Find the Cube of a Number._—The marks II. and III. on D divide that scale into three equal sections. If the number to be cubed is in the first section, I. on C is set to it; if in the second section, II. on C is set to it; if in the third section, III. on C is set to it. Then, under the index mark on the back of the slide will be found the significant figures of the cube on the scale F. If I. on C was used for the setting, the cube contains 1 digit; if II. was used, 2 digits; if III. was used, 3 digits. If the first figure of the number to be cubed is not in the units place, the decimal point is moved through _n_ places so as to bring the first significant figure into the units place, the cube found as above, and the decimal point moved in the _reverse direction_ through 3_n_ places.

_To Find the Cube Root of a Number._—The index mark is set to the significant figures of the number on scale F, and the cube root is read on D under I., II. or III. on C, according as the number has 1, 2 or 3 digits preceding the decimal point. Numbers which have 1, 2 or 3 figures preceding the decimal point are dealt with directly. Numbers of any other form are brought to one of the above forms by moving the decimal point 3 places (or such multiple of 3 places as may be required), the root found and its decimal point moved 1 place for each 3-place movement, but in the _reverse direction_.

THE “ELECTRO” SLIDE RULE.—In this special rule for electrical calculations, made by Mr. A. Nestler, the upper scales run from 0·1 to 1000, and are marked “Amp.” and “sq. mm.” respectively. The lower scale on the slide running from 1 to 10,000 is marked M (metres), while the lower scale on the rule (0·1 to 100) is marked “Volt.” The latter scale is so displaced that 10 on M agrees with 0·173 on the Volt scale. The four factors involved are the current strength (in Amp.); the area of a conductor (in sq. mm.); the length of the conductor (in metres); and the permissible loss of potential (in volts). Having given any three of these, the fourth can be found very readily. On the back of the slide are a scale of squares, a scale of cubes and a single scale corresponding to the D scale of an ordinary rule. Hence, by reversing the slide, it is possible to obtain the 2nd, 3rd and 4th powers and roots of numbers. In another form of the rule, the scale of metres is replaced by one of yards, while instead of the area of the conductor in sq. mm., the corresponding “gauge” sizes of wires are given.

THE “POLYPHASE” SLIDE RULE.—This instrument, made by the Keuffel & Esser Company, New York, has, in addition to the usual scales, a scale of cubes on the vertical edge of the stock of the rule, while in the centre of the slide there is a reversed C scale; _i.e._, a scale exactly similar to an ordinary C scale but with the graduations running from right to left. The rule is specially useful for the solution of problems containing combinations of three factors and problems involving squares, square roots, cubes, cube roots and many of the higher powers and roots. It is specially adapted for electrical and hydraulic work.

THE LOG-LOG DUPLEX SLIDE RULE.—The same makers have introduced a log-log duplex slide rule, in which the log-log scale is in three sections, placed one above the other, these occupying the position usually taken up by the A scale. These scales are used in the manner already described (page 86), but some advantage is obtained by the manner in which the complete log-log scale is divided, the limits being _e_^{¹⁄₁₀₀} to _e_^⅒ (on Scale L.L. 1); _e_^⅒ to _e_ (on Scale L.L. 2); and _e_ to _e_^{10} (on Scale L.L. 3), _e_ being the base of natural or hyperbolic logarithms (2·71828). In this way a total log-log range of from 1·01 to 22,000 is provided, meeting all practical requirements. These log-log scales are read in conjunction with a C scale placed at the upper edge of the slide. A similar C scale, but reversed in direction, is placed at the lower edge of the slide, this having red figures to distinguish it readily. The adjacent scale on the body of the rule is an ordinary D scale, and under this is an equally-divided scale giving the common logarithms of values on D. In the centre of the slide is a scale of tangents.

It will be understood that a “duplex” rule consists of two side strips securely clamped together at the two ends, forming the body of the rule, the slide moving between them; hence both front and back faces of the rule and slide are available, graduations on the one side being referred to those on the other by the cursor which extends around the whole. In this instrument, the scales on the back face are the ordinary scales of the standard rule with the addition of a scale of sines which is placed in the centre of the slide. It will be evident that this instrument is capable of dealing with a very wide range of problems involving exponential and trigonometrical formulæ.

SMALL SLIDE RULES WITH MAGNIFYING CURSORS.—Several makers now supply 5 in. rules having the full graduations of a 10 in. rule, and fitted with a magnifying cursor (Fig. 34). This forms a compact instrument for the pocket, but owing to the closeness of the graduations it is not usually possible to make a setting of the slide without using the cursor. This, of course, involves more movements than with the ordinary instrument. It is also very necessary to use the magnifying cursor in a _direct_ light, if accurate readings are to be obtained. If these slight inconveniences are to be tolerated, the principle could be extended, a 10 in. rule being marked as fully as a 20 in., and fitted with a magnifying cursor. The author has endeavoured, but without success, to induce makers to introduce such a rule.

The magnifying cursor, supplied by Messrs. A. G. Thornton, Limited, has a lens which fills the entire cursor. It has a powerful magnifying effect, and the change from the natural to the magnified reading is less abrupt than with the semicircular lens.

THE CHEMIST’S SLIDE RULE.—A slide rule, specially adapted for chemical calculations, has been introduced recently by Mr. A. Nestler. In this instrument the C and D scales are as usually arranged; but, in place of the A and B scales, there are a number of gauge points or marks denoting the atomic and molecular weights of the most important elements and combinations. The scales on the back of the slide are similarly arranged, so that by reversing the slide the operations can be extended very considerably. The rule finds its chief use in the calculation of analyses. Thus, to find the percentage of chlorine if _s_ grammes of a substance have been used and the precipitate of Ag.Cl. weighs _a_ grammes, we have the equation, _x_ = (Cl.)/(Ag.Cl.) × (_a_)/(_s_). Hence, the mark Ag.Cl. on the upper scale of the slide is set to the mark Cl. on the upper scale of the rule, when under _a_ on the C scale is found the quantity of chlorine on D. By setting the cursor to this value and bringing _s_ on C to the cursor, the percentage required can be read on C over 10 on D.

The rule is also adapted to the solution of various other chemical and electro-chemical calculations.

THE STELFOX SLIDE RULE.—This rule, shown in Fig. 35, has a stock 5 in. long, fitted with a 10 in. slide jointed in the middle of its length by means of long dowels. By separating the parts the compactness of a 5 in. rule is obtained. The upper scales on the rule and slide resemble the usual A and B scales. The D scale on the lower part of the stock is in two sections, the second portion being placed below the first, as shown in the illustration. The centre scale on the slide corresponds to the usual C scale, while on the lower edge of the slide is a similar scale, but with the index (1) in the middle of its length. The arrangement avoids the necessity of resetting the slide, as is sometimes necessary with the ordinary rule, and in general it combines the accuracy of a 10 in. rule with the compactness of a 5 in. rule; but a more frequent use of the cursor is necessary. This rule is made by Messrs. John Davis & Son, Limited, Derby.

ELECTRICAL SLIDE RULE.—Another rule by the same makers, specially useful for electrical engineers, has the usual scales on the working edges of the rule and slide, while in the middle of the slide is placed a scale of cubes. A log-log scale in two sections is provided; the power portion, running from 1·07 to 2, is found on the lower part of the stock, and the upper portion, running from 2 to 10^3, on the upper part of the stock. The uppermost scale on the stock is in two parts, of which that to the left, running from 20 to 100 and marked “Dynamo,” gives the efficiencies of dynamos; that on the right, running from 20 to 100 and marked “Motor,” gives the efficiencies of electric motors. The lowest scale on the stock, marked “Volt,” gives the loss of potential in copper conductors. The ordinary upper scale on the stock is marked L (length of lead) at the left, and KW (kilowatts) at the right; the ordinary upper scale on the slide is marked A (ampères) and mm^2 (sectional area) at the left, and HP (horse-power) at the right. Additional lines on the cursor enable the electrical calculations to be made either in British or metric units.

THE PICOLET CIRCULAR SLIDE RULE.—A simple form of circular calculator, made by Mr. L. E. Picolet of Philadelphia, is shown in Fig. 36. It consists of a base disc of stout celluloid on which turns a smaller disc of thin celluloid. A cursor formed of transparent celluloid is folded over the discs, and is attached so that the friction between the cursor and the inner disc enables the latter to be turned by moving the former. By holding both discs the cursor can be adjusted as required. The adjacent scales run in opposite directions, so that multiplication and division are performed as with the inverted slide in an ordinary rule. The outer scale, which is two-thirds the length of the main scale, enables cube roots to be found. Square roots are readily determined and continuous multiplication and division conveniently effected. Modified forms of this neatly made little instrument are also available.

OTHER RECENT SLIDE RULES.—Among other special types of slide rule, mention should be made of the _Jakin_ 10 in. rule for surveyors, made by Messrs. John Davis & Son, Limited, Derby. By the provision of a series of short subsidiary scales, the multiplication of a sine or tangent of an angle by a number can be obtained to an accuracy of 1 in 10,000. The _Davis-Lee-Bottomley_ slide rule, by the same makers, has special scales provided for circle spacing. The division of a circle into a number of equal parts, often required in spacing rivets, bolts, etc., and in setting out the teeth of gearwheels, is readily effected by the aid of this instrument. The _Cuntz_ slide rule is a very comprehensive instrument, having a stock about 2¼ in. wide, with the slide near the lower edge. Above the slide are eleven scales, referable to the main scales by the cursor. These scales enable squares and square roots, cubes and cube roots, and areas and circumferences of circles to be obtained by direct reading. A much more compact instrument could be obtained by removing one-half the scales to the back of the rule and using a double cursor.

In one form of 10 in. rule, supplied by Mr. W. H. Harling, London, the body of the rule is made of well-seasoned cane, with the usual celluloid facings. The rule has a metal back, enabling the fit of the slide to be regulated. This backing extends the full length of the rule, openings about 1 in. long being provided at each end, enabling the scales on the back of the slide to be set with greater facility than is possible with the notched recesses usually adopted. The author has long endeavoured, but without success, to induce makers to fit windows of glass or celluloid in place of the notched recesses. This would allow the graduation of the S and T scales to be set more accurately, and enable both to be used at each end of the rule—an advantage in certain trigonometrical calculations. It would have the further advantage of permitting each alternate graduation of the evenly-divided or logarithm scale to be placed at opposite sides of one central line, enabling the reading to be made more accurately and conveniently.

Many special slide rules have lately been devised for determining the time necessary to perform various machine-tool operations and for analogous purposes, while attention has again been given to rules for calculating the weights of iron and steel bars, plates, etc.

THE DAVIS-STOKES FIELD GUNNERY SLIDE RULE.—This rule, which is adapted for calculations involved in “encounter” and “entrenched” field gunnery, is designed for the 18 pr. quick-firing gun. The upper and lower portions of the boxwood stock are united by a flexible centre of celluloid, thus providing grooves front and rear to receive boxwood slides. Each of the nineteen scales is marked with its name, and corresponding scales are coloured red or black. The front edge is bevelled and carries a scale of 1 in 20,000. The rule solves displacement problems, map angles of sight, changes of corrector and range corrections for changes in temperature, wind and barometer, etc. A special feature for displacement calculations is the provision of a 50 yd. sub-base angle scale, by which the apex angle is read at one setting.

THE DAVIS-MARTIN WIRELESS SLIDE RULE.—In wireless telegraphy it is frequently necessary to determine wave-length, capacity or self-induction when one or other of the factors of the equation, λ = 59·6√(LC) is unknown. The Davis-Martin wireless rule is designed to simplify such calculations. The upper scale in the stock (inductance) runs from 10,000 to 1,000,000; the adjacent scale on the slide (capacity) runs from 0·0001 to 0·01 but in the reverse direction. The lower scale on the stock (wave-length) runs from 100 to 1000, giving square roots of the upper scale; while on the lower edge of the scale are several arrows to suit the various denominations in which the wave-length and capacity may be expressed.

IMPROVED CURSORS.—In some slide-rule operations, notably in those involved in solving quadratic and cubic equations, it not infrequently happens that readings are obscured by the frame of the cursor. Frameless cursors have been introduced to obviate this defect. A piece of thick transparent celluloid is sometimes employed, but this is liable to become scratched in use. Fig. 37 shows a recent form of frameless glass cursor made by the Keuffel & Esser Company, Hoboken, N.J., which is satisfactory in every way.

Cursors having three hair lines are now fitted to some rules, the distance apart of the lines being equal to the interval 0·7854–1 on the A scale.

THE DAVIS-PLETTS SLIDE RULE.—In this rule a single log.-log. scale and its reciprocal scale are arranged opposite the ordinary upper log. scale. Thus, common logarithms can be read directly, while by taking advantage of the properties of characteristics and mantissas of common logarithms, the scale can be extended indefinitely. As 10 is the highest number on the log.-log. scale, it is carried down to within 0·025 of unity. The reading of log.-log. values above 10 is effected in a very simple manner. There is also a scale in the centre of the slide which, used in conjunction with the upper log. scale enables the natural logarithm of any number between 0·0001 and 10,000 to be read direct, while any number on the upper log. scale can be multiplied or divided by _e^x_ if the latter is between these limits. On the back of the slide are scales for all circular and hyperbolic functions, these being used in conjunction with the upper log. scales.

THE CROMPTON-GALLAGHER BOILER EFFICIENCY CALCULATOR has a stock in the thickness of which is a slot admitting a chart which can be moved at right angles to the two separate slides. On the bevelled edge of one slide, the graduations are continued so as to read against curves on the chart, through an opening in the stock.

THE DAVIS-GRINSTED COMPLEX CALCULATOR.—This slide rule is of considerable service in connection with calculations involving the conversion of complex quantities from the form _a_ + _j_ _b_ to the form R∠θ, and _vice versa_. The usual process of conversion necessitates repeated reference to trigonometrical tables, and is both tedious and time-taking. The Complex Calculator enables the conversions to be effected without reference to tables and with the minimum expenditure of time and labour.

The rule, which is about 16 in. long, has five scales. The upper one (A) is an ordinary logarithmic scale thrice-repeated. The adjacent scales on the slide comprise (1) a logarithmic scale of tangents (B) ranging from 0·1° to 45°, and (2) a logarithmic scale of secants (C) from 0° to 45°. The lower scales D and E are identical with the A scale, and are provided to enable multiplication, etc., to be performed without the need for a separate slide rule. Readings can be transferred from A to the lower scales by means of the cursor.

In using the rule to convert _a_ + _j_ _b_ to R∠θ, the index (45°) of the B scale is set to the larger component and the cursor to the smaller component, on scale A. Then θ (or its complement if _b_ is greater than _a_) is read on B under the cursor. The cursor is then set to θ on the C scale, and R is read on A under the cursor. The rule is made by Messrs. John Davis & Son, Limited, Derby.

THE SOLUTION OF ALGEBRAIC EQUATIONS.

The slide rule finds an interesting application in the solution of equations of the second and third degree; and although the process is essentially one of trial and error, it may often serve as an efficient substitute for the more laborious algebraic methods, particularly when the conditions of the problem or the operator’s knowledge of the theory of equations enables some idea to be obtained as to the character of the result sought. The principle may be thus briefly explained:—If 1 on C is set to _x_ on D (Fig. 38), we find _x_(_x_) = _x_^2 on D under _x_ on C. If, however, with the slide set as before, instead of reading under _x_, we read under _x_ + _m_ on C, the result on D will now be _x_(_x_ + _m_) = _x_^2 + _mx_ = _q_. Hence to solve the equation _x_^2 + _mx_ − _q_ = 0, we reverse the above process, and setting the cursor to _q_ on D, we move the slide until the number on C under the cursor, and that on D under 1 on C, _differ by m_. It is obvious from the setting that the _product_ of these numbers = _q_, and as their difference = _m_, they are seen to be the roots of the equation as required. For the equation _x_^2 − _mx_ + _q_ = 0, we require _m_ to equal the _sum_ of the roots. Hence, setting the cursor as before to _q_ on D, we move the slide until the number on C under the cursor, and that on D under 1 on C, are _together equal to_ _m_, these numbers being the roots sought. The alternative equations _x_^2 − _mx_ − _q_ = 0, and _x_^2 + _mx_ + _q_ = 0 are deducible from the others by changing the signs of the roots, and need not be further considered.

EX.—Find the roots of _x_^2 − 8_x_ + 9 = 0.

Set the cursor to 9 on D, and move the slide to the right until when
6·64 is found under the cursor, 1·355 on D is under 1 on C. These
numbers are the roots required.

The upper scales can of course be used; indeed, in general they are to be preferred.

EX.—Find the roots of _x_^2 + 12·8_x_ + 39·4 = 0.

Set the cursor to 39·4 on A, and move the slide to the right until we
read 7·65 on B under the cursor, and 5·15 on A over 1 on B. The roots
are therefore −7·65 and −5.15.

With a little consideration of the relative value of the upper and lower scales, the student interested will readily perceive how equations of the third degree may be similarly resolved. The subject is not of sufficient general importance to warrant a detailed examination being made of the several expressions which can be dealt with in the manner suggested; but the author gives the following example as affording some indication of the adaptability of the method to practical calculations.

EX.—A hollow copper ball, 7·5 in. in diameter and 2 lb. in weight,
floats in water. To what depth will it sink?

The water displaced = 27·7 × 2 = 55·4 cub. in. The cubic contents of
the immersed segment will be (π)/(3)(3_r_ _x_^2 − _x_^3), _r_ being
the radius and _x_ the depth of immersion. Hence (π)/(3)(3_r_ _x_^2 −
_x_^3) = 55·4, and 11·25_x_^2 − _x_^3 = 52·9.

To solve this equation we place the cursor to 52·9 on A, and move the
slide until the reading on D under 1 and that on B under the cursor
together amount to 11·25. In this way find 2·45 on D under 1, with 8·8
on B under the cursor _c_, _c_, as a pair of values of which the sum
is 11·25. Hence we conclude that _x_ = 2·45 in. is the result sought.

With the rule thus set (Fig. 39) the student will note that the slide
is displaced to the right by an amount which represents _x_ on D, and
therefore _x_^2 on A; while the length on B from 1 to the cursor line
represents 11·25 − _x_. Hence the upper scale setting gives
_x_^2(11·25 − _x_) = 11·25_x_^2 − _x_^3 = 52·9 as required.

When in doubt as to the method to be pursued in any given case, the student should work synthetically, building up a simple example of an analogous character to that under consideration, and so deducing the plan to be followed in the reverse process.

SCREW-CUTTING GEAR CALCULATIONS.

The slide rule has long found a useful application in connection with the gear calculations necessary in screw-cutting, helical gear-cutting, and spiral gear work.

SINGLE GEARS.—For simple cases of screw-cutting in the lathe it is only necessary to set the threads per inch to be cut to the threads per inch in the guide screw (or the pitch in inches in each case, if more convenient). Then any pair of coinciding values on the two scales will give possible pairs of wheels.

EX.—Find wheels to cut a screw of 1⅝ threads per inch with a guide
screw of 2 threads per inch.

Setting 1·625 on C to 2 on D, it is seen that 80 (driver) and 65
(driven) are possible wheels.

COMPOUND GEARS.—When wheels so found are of inconvenient size, a compound train is used, consisting (usually) of two drivers and two driven wheels, the product of the two former and the product of the two latter being in the same ratio as the simple wheels. Thus with 60 and 40 as drivers, and 65 and 30 as driven, we have, (60 × 40)/(65 × 30) = (2400)/(1950) = (2)/(1·625) as before.

With the slide set as above, values convenient for splitting up into suitable wheels are readily obtainable. Thus, (1600)/(1300); (2400)/(1950); (4000)/(3250); (4800)/(3900) are a few suggestive values which may be readily factorised.

SLIDE RULES FOR SCREW-CUTTING CALCULATIONS.—Special circular and straight slide rules for screw-cutting gear calculations have long been employed. For compound gears these usually entail the use of six scales, two on each of the two slides and two on the stock. The upper scale on the stock may be a scale of threads per inch to be cut, the adjacent scale (on the upper slide) a scale of threads per inch in the guide screw. Setting the guide screw-graduation to the threads to be cut, the lower slide is adjusted until a convenient pair of drivers is found in coincidence on the central pair of scales, while a pair of driven wheels are in coincidence on the two lower scales.

Some years ago, a slide rule was introduced by which compound gears could be obtained with a single slide. Assuming the set of wheels usually provided—20 to 120 teeth advancing by 5 teeth—the products of 20 × 25, 20 × 30, etc., up to 115 × 120 were calculated. These products were laid out along each of the two lower scales. The upper scales were a scale of threads per inch to be cut and a scale of the threads per inch of various guide screws. Setting the guide screw-graduation to the threads to be cut, any coinciding graduations on the lower scales gave the required pairs of drivers and driven wheels.

FRACTIONAL PITCH CALCULATIONS.—The author has long advocated the use of the slide rule for determining the wheels necessary for cutting fractional pitch threads, and it is gratifying to find its value in this connection is now being appreciated. For the best results a good 20 in. rule is desirable, but with care very close approximations can be found with an accurate 10 in. rule. In any case a magnifying cursor or a hand reading-glass is of great assistance.

EX.—Find wheels to cut a thread of 0·70909 in. pitch; guide screw, 2
threads per inch.

To 0·70909 on D, set 0·5 (guide screw pitch in inches) on C. To make
this setting as accurately as possible, the method described on page
112 may be used. Set 10 on C to about 91 on D, and note that the
interval 77–78 on C represents 0·91 of the interval 70–71 on D. Set
the cursor to 78 on C and bring 5 to the cursor. The slide is then set
so that 5 on C agrees with 7·091 on D.

Inspection of the two scales shows various coinciding factors in the ratio required. The most accurate is seen to be (55 on C)/(78 on D). These values may be split up into (55 × 50)/(65 × 60) to form a suitable compound train of gears.

GAUGE POINTS AND SIGNS ON SLIDE RULES.

Many slide rules have the sign (Prod.)/(−1) at the right-hand end of the D scale, while on the left is (Quot.)/(+1.) It is somewhat unfortunate that these signs refer to rules for determining the number of digits in products and quotients, which are used to a considerable extent on the Continent, and conflict with those used in this country. By the Continental method the number of digits in a product is equal to the sum of the digits in the two factors, if the result is obtained on the LEFT _of the first factor_; but if the result is found on the RIGHT of the first factor, it is equal to this sum − 1. The sign (Prod.)/(−1) the _right_-hand end of the D scale provides a visible reminder of this rule.

Similarly for division:—The number of digits in a quotient is equal to the number of the digits in the dividend, minus those in the divisor, if the quotient appears on the RIGHT _of the dividend_, and to this difference + 1, if the quotient appears on the LEFT of the dividend. The sign (Quot.)/(+1) at the _left_-hand end of the D scale provides a visible reminder of this rule.

The sign

+ⵏ–
⟵ⵏ⟶
–ⵏ+

found at both ends of the A scale is of general application but of questionable utility. It is assumed to represent a fraction, the vertical line indicating the position of the decimal point. If the number 455 is to be dealt with in a multiplication on the lower scales, we may suppose the decimal point moved two places to the left, giving 4·55, a value which can be actually found on the scale. If we use this value, then to the number of digits in this result, as many must be added as the number of places (two in this case) by which the decimal point was moved. If the point is moved to the right, the number of places must be subtracted. Similarly, in division, if the decimal point in the divisor is moved _n_ places to the left, then _n_ places must be subtracted at the end of the operation; while if the point is moved through _n_ places to the right, then _n_ places must be added. The sign referred to, which, of course, applies to all scales, completely indicates these processes and is submitted as a reminder of the procedure to be followed by those using the method described.

The signs π, _c_, _c′_, and M are explained in the Section on “Gauge Points,” p. 53.

On some rules additional signs are found on the D scale. One, locating the value (180 × 60)/(π) = 3437·74 and hence giving the number of minutes in a radian, is marked ρ′. Another, representing the value (180 × 60 × 60)/(π) = 206265, and hence giving the number of seconds in a radian is marked ρ″. A third point, marked ρ_{˶}, placed at the value (200 × 100 × 100)/(π) = 636620, is used when the newer graduation of the circle is employed.

These gauge points are useful when converting angles into circular measure, or _vice versa_, and also for determining the functions of small angles.

A gauge point is sometimes marked at 1146 on the A and B scales. This is known as the “Gunner’s Mark,” and is used in artillery calculations involving angles of less than 20°, when, for the purpose in view, the tangent and circular measure of the angle may be regarded as equal. For this constant, the angle is taken in minutes, the auxiliary base in feet, and the base in yards. The auxiliary base in feet on B is set to the angle in minutes on A when over 1146 on B is the base in yards on A. The value (1)/(1146) = (π × 3)/(180 × 60).

TABLES AND DATA.

MENSURATION FORMULAE.

Area of a parallelogram = base × height.

Area of rhombus = ½ product of the diagonals.

Area of a triangle = ½ base × perpendicular height.

Area of equilateral triangle = square of side × 0·433.

Area of trapezium = ½ sum of two parallel sides × height.

Area of any right-lined figure of four or more unequal sides is found
by dividing it into triangles, finding area of each and adding
together.

Area of regular polygon = (1) length of one side × number of sides ×
radius of inscribed circle; or (2) the sum of the triangular areas
into which the figures may be divided.

Circumference of a circle = diameter × 3·1416.

Circumference of circle circumscribing a square = side × 4·443.

Circumference of circle = side of equal square × 3·545.

Length of arc of circle = radius × degrees in arc × 0·01745.

Area of a circle = square of diameter × 0·7854.

Area of sector of a circle = length of arc × ½ radius.

Area of segment of a circle = area of sector − area of triangle.

Side of square of area equal to a circle = diameter × 0·8862.

Diameter of circle equal in area to square = side of square × 1·1284.

Side of square inscribed in circle = diameter of circle × 0·707.

Diameter of circle circumscribing a square = side of square × 1·414.

Area of square = area of inscribed circle × 1·2732.

Area of circle circumscribing square = square of side × 1·5708.

Area of square = area of circumscribing circle × 0·6366.

Area of a parabola = base x ⅔ height.

Area of an ellipse = major axis × minor axis × 0·7854.

Surface of prism or cylinder = (area of two ends) + (length ×
perimeter).

Volume of prism or cylinder = area of base × height.

Surface of pyramid or cone = ½(slant height × perimeter of base) +
area of base.

Volume of pyramid or cone = (⅓)(area of base × perpendicular height).

Surface of sphere = square of diameter × 3·1416.

Volume of sphere = cube of diameter × 0·5236.

Volume of hexagonal prism = square of side × 2·598 × height.

Volume of paraboloid = ½ volume of circumscribing cylinder.

Volume of ring (circular section) = mean diameter of ring × 2·47 ×
square of diameter of section.

SPECIFIC GRAVITY AND WEIGHT OF MATERIALS.

METALS. ─────────────────────┬───────────────┬───────────────┬─────────────── METAL. │ Specific │ Weight of 1 │ Weight of 1 │ Gravity. │Cub. Ft. (Lb.).│Cub. In. (Lb.). ─────────────────────┼───────────────┼───────────────┼─────────────── Aluminium, Cast │ 2·56│ 160│ 0·0927 Aluminium, Bronze │ 7·68│ 475│ 0·275 Antimony │ 6·71│ 418│ 0·242 Bismuth │ 9·90│ 617│ 0·357 Brass, Cast │ 8·10│ 505│ 0·293 „ Wire │ 8·548│ 533│ 0·309 Copper, Sheet │ 8·805│ 549│ 0·318 „ Wire │ 8·880│ 554│ 0·321 Gold │ 19·245│ 1200│ 0·695 Gun metal │ 8·56│ 534│ 0·310 Iron, Wrought (mean) │ 7·698│ 480│ 0·278 „ Cast (mean) │ 7·217│ 450│ 0·261 Lead, Milled Sheet │ 11·418│ 712│ 0·412 Manganese │ 8·012│ 499│ 0·289 Mercury │ 13·596│ 849│ 0·491 Nickel, Cast │ 8·28│ 516│ 0·300 Phosphor Bronze, Cast│ 8·60│ 536·8│ 0·310 Platinum │ 21·522│ 1342│ 0·778 Silver │ 10·505│ 655│ 0·380 Steel (mean) │ 7·852│ 489·6│ 0·283 Tin │ 7·409│ 462│ 0·268 Zinc, Sheet │ 7·20│ 449│ 0·260 „ Cast │ 6·86│ 428│ 0·248 ─────────────────────┴───────────────┴───────────────┴───────────────

MISCELLANEOUS SUBSTANCES.
────────────┬──────────┬──────────
SUBSTANCE. │ Specific │Weight of
│ Gravity. │1 Cub. In.
│ │ (Lb.).
────────────┼──────────┼──────────
Asbestos │ 2·1–2·80 │·076-·101
Brick │ 1·90 │ ·069
Cement │2·72–3·05 │·0984-·109
Clay │ 2·0 │ ·072
Coal │ 1·37 │ ·0495
Coke │ 0·5 │ ·0181
Concrete │ 2·0 │ ·072
Fire-brick │ 2·30 │ ·083
Granite │ 2·5–2·75 │·051-·100
Graphite │ 1·8–2·35 │·065-·085
Sand-stone │ 2·3 │ ·083
Slate │ 2·8 │ ·102
Wood— │ │
Beech │ 0·75 │ ·0271
Cork │ 0·24 │ ·0087
Elm │ 0·58 │ ·021
Fir │ 0·56 │ ·0203
Oak │ ·62-·85 │·025-·031
Pine │ 0·47 │ ·017
Teak │ 0·80 │ ·029
────────────┴──────────┴──────────

ULTIMATE STRENGTH OE MATERIALS. ──────────────────┬────────────┬────────────┬────────────┬──────────── MATERIAL. │ Tension in │Compression │Shearing in │ Modulus of │lb. per sq. │ in lb. per │lb. per sq. │ Elasticity │ in. │ sq. in. │ in. │ in lb. per │ │ │ │ sq. in. ──────────────────┼────────────┼────────────┼────────────┼──────────── Cast Iron │ 11,000 to│ 50,000 to│ │ 14,000,000 │ 30,000│ 130,000│ │ to │ │ │ │ 23,000,000 „ aver.│ 16,000│ 95,000│ 11,000│ Wrought Iron │ 40,000 to│ │ │ 26,000,000 │ 70,000│ │ │ to │ │ │ │ 31,000,000 „ aver.│ 50,000│ 50,000│ 40,000│ Soft Steel │ 60,000 to│ │ │ 30,000,000 │ 100,000│ │ │ to │ │ │ │ 36,000,000 Soft Steel aver.│ 80,000│ 70,000│ 55,000│ Cast Steel aver.│ 120,000│ │ │ 15,000,000 │ │ │ │ to │ │ │ │ 17,000,000 Copper, Cast │ 19,000│ 58,000│ │ „ Wrought │ 34,000│ │ │ 16,000,000 Brass, Cast │ 18,000│ 10,500│ │ 9,170,000 Gun Metal │ 34,000│ │ │ 11,500,000 Phosphor Bronze │ 58,000│ │ 43,000│ 13,500,000 Wood, Ash │ 17,000│ 9,300│ 1,400│ „ Beech │ 16,000│ 8,500│ │ „ Pine │ 11,000│ 6,000│ 650│ 1,400,000 „ Oak │ 15,000│ 10,000│ 2,300│ 1,500,000 Leather │ 4,200│ │ │ 25,000 ──────────────────┴────────────┴────────────┴────────────┴────────────

POWERS, ROOTS, ETC., OF USEFUL FACTORS.
_n_ │(1)/(_n_)│ _n_^2 │ _n_^3 │ √_̅n_ │ (1)/(√_̅n_) │ ∛_̅n_ │ (1)/(∛_̅n_)
────────────────┼─────────┼───────┼──────────┼──────┬┴───────────┬─┴────┬──┴─────────
π = 3·142 │ 0·318│ 9·870│ 31·006│ 1·772│ 0·564│ 1·465│ 0·683
2π= 6·283 │ 0·159│ 39·478│ 248·050│ 2·507│ 0·399│ 1·845│ 0·542
(π)/(2) = 1·571 │ 0·637│ 2·467│ 3·878│ 1·253│ 0·798│ 1·162│ 0·860
(π)/(3) = 1·047 │ 0·955│ 1·097│ 1·148│ 1·023│ 0·977│ 1·016│ 0·985
(4)/(3)π = 4·189│ 0·239│ 17·546│ 73·496│ 2·047│ 0·489│ 1·612│ 0·622
(π)/(4) = 0·785 │ 1·274│ 0·617│ 0·484│ 0·886│ 1·128│ 0·923│ 1·084
(π)/(6) = 0·524 │ 1·910│ 0·274│ 0·144│ 0·724│ 1·382│ 0·806│ 1·241
π^2 = 9·870 │ 0·101│ 97·409│ 961·390│ 3·142│ 0·318│ 2·145│ 0·466
π^3 = 31·006 │ 0·032│961·390│29,809·910│ 5·568│ 1·796│ 3·142│ 0·318
(π)/(32) = 0·098│ 10·186│ 0·0095│ 0·001│ 0·313│ 3·192│ 0·461│ 2·168
_g_ = 32·2 │ 0·031│1036·84│ 33,386·24│ 5·674│ 0·176│ 3·181│ 0·314
2_g_ = 64·4 │ 0·015│4147·36│ 267,090│ 8·025│ 0·125│ 4·007│ 0·249
────────────────┴─────────┴───────┴──────────┴──────┴────────────┴──────┴────────────

HYDRAULIC EQUIVALENTS.

1 foot head = 0·434 lb. per square inch.
1 lb. per square inch = 2·31 ft. head.
1 imperial gallon = 277·274 cubic inches.
1 imperial gallon = 0·16045 cubic foot.
1 imperial gallon = 10 lb.
1 cubic foot of water = 62·32 lb. = 6·232 imperial gallons.
1 cubic foot of sea water = 64·00 lb.
1 cubic inch of water = 0·03616 lb.
1 cubic inch of sea water = 0·037037 lb.
1 cylindrical foot of water = 48·96 lb.
1 cylindrical inch of water = 0·0284 lb.
A column of water 12 in. long 1 in. square = 0·434 lb.
A column of water 12 in. long 1 in. diameter = 0·340 lb.
Capacity of a 12 in. cube = 6·232 gallons.
Capacity of a 1 in. square 1 ft. long = 0·0434 gallon.
Capacity of a 1 ft. diameter 1 ft. long = 4·896 gallons.
Capacity of a cylinder 1 in. diameter 1 ft. long = 0·034 gallon.
Capacity of a cylindrical inch = 0·002832 gallon.
Capacity of a cubic inch = 0·003606 gallon.
Capacity of a sphere 12 in. diameter = 3·263 gallons.
Capacity of a sphere 1 in. diameter = 0·00188 gallon.
1 imperial gallon = 1·2 United States gallon.
1 imperial gallon = 4·543 litres of water.
1 United States gallon = 231·0 cubic inches.
1 United States gallon = 0·83 imperial gallon.
1 United States gallon = 3·8 litres of water.
1 cubic foot of water = 7·476 United States gallons.
1 cubic foot of water = 28·375 litres of water.
1 litre of water = 0·22 imperial gallon.
1 litre of water = 0·264 United States gallon.
1 litre of water = 61·0 cubic inches.
1 litre of water = 0·0353 cubic foot.

───────────────────────────────────────────────────────────────────────── EQUIVALENTS OF POUNDS AVOIRDUPOIS. ─┬───────┬────────────┬────────────────┬────────────────┬──────────────── │ 10 │ 100 │ 1000 │ 10,000 │ 100,000 ─┼───────┼────────────┼────────────────┼────────────────┼──────────────── │qr. lb.│cwt. qr. lb.│ton cwt. qr. lb.│ton cwt. qr. lb.│ton cwt. qr. lb. 1│ 0 10│ 0 3 16│ 0 8 3 20│ 4 9 1 4│ 44 12 3 12 2│ 0 20│ 1 3 4│ 0 17 3 12│ 8 18 2 8│ 89 5 2 24 3│ 1 2│ 2 2 20│ 1 6 3 4│ 13 7 3 12│133 18 2 8 4│ 1 12│ 3 2 8│ 1 15 2 24│ 17 17 0 16│178 11 1 20 5│ 1 22│ 4 1 24│ 2 4 2 16│ 22 6 1 20│223 4 1 4 6│ 2 4│ 5 1 12│ 2 13 2 8│ 26 15 2 24│267 17 0 16 7│ 2 14│ 6 1 0│ 3 2 2 0│ 31 5 0 0│312 10 0 0 8│ 2 24│ 7 0 16│ 3 11 1 20│ 35 14 1 4│357 2 3 12 9│ 3 6│ 8 0 4│ 4 0 1 12│ 40 3 2 8│401 15 2 24 ─┴───────┴────────────┴────────────────┴────────────────┴────────────────

TRIGONOMETRICAL FUNCTIONS.

RIGHT-ANGLED TRIANGLES.

]

Sin. A = (_a_)/(_b_) Sec. A = (_b_)/(_c_) Tan. A = (_a_)/(_c_)

Cos. A = (_c_)/(_b_) Cosec. A = (_b_)/(_a_) Cotan. A = (_c_)/(_a_)

Versin. A = (_b_ − _c_)/(_b_). Coversin. A = (_b_ − _a_)/(_b_).

───────┬─────────┬─────────────────────────────────────────────────────
Given. │Required.│ Formulæ.
───────┼─────────┼─────────────────────────────────────────────────────
_a_,_b_│ A,C,_c_ │Sin. A = (_a_)/(_b_) Cos. C = (_a_)/(_b_) _c_ =
│ │ √((_b + a_)(_b − a_))
│ │
_a_,_c_│ A,C,_b_ │Tan. A = (_a_)/(_c_) Cotan. B = (_a_)/(_c_) _b_ =
│ │ √(_a_^2 + _c_^2)
│ │
A,_a_ │C,_c_,_b_│ C = 90° − A _c_ = _a_ × Cotan. A _b_ =
│ │ (_a_)/(Sin. A)
│ │
A,_b_ │C,_a_,_c_│C = 90° − A _a_ = _b_ × Sin. A _c_ = _b_ × Cos.
│ │ A
│ │
A,_c_ │C,_a_,_b_│ C = 90° − A _a_ = _c_ × Tan. A _b_ =
│ │ (_c_)/(Cos. A)
│ │
───────┴─────────┴─────────────────────────────────────────────────────

OBLIQUE-ANGLED TRIANGLES.

_s_ = ½(_a + b + c_)

]

───────────┬─────────┬─────────────────────────────────────────────────
Given. │ │ Formulæ.
───────────┼─────────┼─────────────────────────────────────────────────
A,B,C,_a_ │ Area= │(_a_^2 × Sin. B × Sin. C) ÷ 2 Sin. A
A,_b_,_c_ │ „ │½(_c_ × _b_ × Sin. A)
_a_,_b_,_c_│ „ │√(_s_(_s_ − _a_)(_s_ − _b_)(_s_ − _c_))
───────────┼─────────┼─────────────────────────────────────────────────
Given. │Required.│ Formulæ.
───────────┼─────────┼─────────────────────────────────────────────────
A,C,_a_ │ _c_ │ _c_ = _a_(Sin. C)/(Sin. A)
───────────┼─────────┼─────────────────────────────────────────────────
A,_a_,_c_ │ C │ Sin. C = (_c_ Sin. A)/(_a_)
───────────┼─────────┼─────────────────────────────────────────────────
_a_,_c_,B │ A │ Tan. A = (_a_ Sin. B)/(_c_ − _a_ Cos. B)
───────────┼─────────┼─────────────────────────────────────────────────
_a_,_b_,_c_│ A │Sin. ½A = √(((_s_ − _b_)(_s_ − _c_))/(_b_ × _c_))
„ │ „ │ Cos. ½A = √((_s_(_s_ − _a_))/(_b_ × _c_));
„ │ „ │ Tan. ½A = √(((_s_ − _b_)(_s_ − _c_))/(_s_(_s_ −
│ │ _a_)))
───────────┴─────────┴─────────────────────────────────────────────────

COMPOUND ANGLES.

Sin. (A + B) = Sin. A Cos. B + Cos. A Sin. B.
Sin. (A − B) = Sin. A Cos. B − Cos. A Sin. B.
Cos. (A + B) = Cos. A Cos. B − Sin. A Sin. B.
Cos. (A − B) = Cos. A Cos. B + Sin. A Sin. B.

Tan. (A + B) = (Tan. A + Tan. B)/(1 − Tan. A Tan. B).

Tan. (A − B) = (Tan. A − Tan. B)/(1 + Tan. A Tan. B).

SLIDE RULE DATA SLIPS, COMPILED BY C. N. PICKWORTH, WH.SC.

(_It is suggested that this page be removed by cutting through the above line, and selected portions of the Sectional Data Slips attached to the back of the Slide Rule._)

¹⁄₃₂ │0·03125
¹⁄₁₆ │0·0625
³⁄₃₂ │0·09375
⅛ │0·125
⁵⁄₃₂ │0·15625
³⁄₁₆ │0·1875
⁷⁄₃₂ │0·21875
¼ │0·25
⁹⁄₃₂ │0·28125
⁵⁄₁₆ │0·3125
¹¹⁄₃₂ │0·34375
⅜ │0·375
¹³⁄₃₂ │0·40625
⁷⁄₁₆ │0·4375
¹⁵⁄₃₂ │0·46875
¹⁷⁄₃₂ │0·53125
⁹⁄₁₆ │0·5625
¹⁹⁄₃₂ │0·59375
⅝ │0·625
²¹⁄₃₂ │0·65625
¹¹⁄₁₆ │0·6875
²³⁄₃₂ │0·71875
¾ │0·75
²⁵⁄₃₂ │0·78125
¹³⁄₁₆ │0·8125
²⁷⁄₃₂ │0·84375
⅞ │0·875
²⁹⁄₃₂ │0·90625
¹⁵⁄₁₆ │0·9375
³¹⁄₃₂ │0·96875

Circ. of circle = 3·1416 _d_.

Area „ „ = 0·7854 _d_^2.

Sq. eq. area to cir., _s_ = 0·886 _d_.

Circle eq. to sq., _d_ = 1·128 _s_.

Sq. inscbd. in circ., _s_ = 0·707 _d_.

Circsb. circ. of sq., _d_ = 1·414 _s_.

Area of ellipse = 0.7854 _a_ × _b_.

Surface of sphere = 3·1416 _d_^2.

Volume „ „ = 0·5236 _d_^3.

„ „ cone = 0·2618 _d_^2 _h_.

Radian = (180°)/(π) = 57·29 deg.

Base of nat. or hyp. log. = e = 2·7183.

Nat. or hyp. log. = com. log. × 2·3026.

g (at London) 32·18 ft. per sec., per sec.

Abs. temp. = deg. F. + 461° = deg. C. + 274°.

C.° = (5)/(9)(F.° − 32°); F.° = (9)/(5)C.° + 32°.

Cal. pr.—Ther. units per lb.: Coal, 14,300;

petrol’m, 20,000; coal gas per cu. ft., 700.

Sp. heat:—Wt. iron, 0·1138; C.I., 0·1298;

copper, brass, 0·095; lead, 0·0314.

Inch = 25·4 mil’metres; mil’metre = 0·03937 in.

Foot = 0·3048 metres; metre = 3·2809 feet.

Yard = 0·91438 metre; metre = 1·0936 yards.

Mile = 1·6093 kilomtrs.; kilomtr. = 0·6213 mile.

Sq. in. = 6·4513 sq. cm.; sq. cm. = 0·155 sq. in.

Sq. ft. = 9·29 sq. decmtr.; sq. decmtr. = 0·1076 sq. ft.

Sq. yd. = 0·836 sq. metre; sq. metre = 1·196 sq. yds.

Sq. ml. = 258·9 hectares; hectare = 0·00386 sq. ml.

Cu. in. = 16·386 c. cm.; c. cm. = 0·06102 cu. in.

Cu. ft. = 0·0283 c. metre; c. metre = 35·316 cu. ft.

Grain = 0·0648 gramme; gram. = 15·43 grs.

Ounce = 28·35 grams.; „ = 0·03527 oz.

Pound = 0·4536 kilogm.; kilogm. = 2·204 lb.

Ton = 1·016 tonnes; tonne = 0·9842 ton.

Mile per hr. = 1·466 ft., or 44·7 cm., per sec.

Lb. per cu. in. = 0·0276 kilogram per cu. cm.

Kilogram per cu. cm. = 36·125 lb. per cu. in.

Lb. per cu. ft. = 16·019 kilogm. per cu. mtre.

Grain per gall. = 0·01426 gramme per litre.

Gramme per litre = 70·116 grains per gall.

Ultimate Strength│Lb. per Sq. in.
„ │Tens’n.│Comp’n.
─────────────────┼───────┼───────
Wt. iron │ 50,000│ 50,000
Cast „ │ 16,000│ 95,000
Steel │ 80,000│ 70,000
Copper │ 21,000│ 50,000
Brass │ 18,000│ 10,500
Lead │ 2,500│ 7,000
Pine │ 11,000│ 6,000
Oak │ 15,000│ 10,000

Weight of Metals.│ Cub. In. │ Cub. Ft. │12 Cu. In.
─────────────────┼──────────┼──────────┼──────────
Wt. iron │ 0·277│ 480│ 3·33
Cast „ │ 0·260│ 450│ 3·12
Steel │ 0·283│ 490│ 3·40
Copper │ 0·318│ 550│ 3·82
Brass │ 0·300│ 520│ 3·61
Zinc │ 0·248│ 430│ 2·98
Alumin’m │ 0.096│ 168│ 1·16
Lead │ 0.411│ 710│ 4·93

Lb. per sq. in. = 2·31 ft. water = 2·04 in. mercury = 0·0703 kilo. per sq. cm. Atmosphere = 14·7 lb. per sq. in. = 33·94 ft. water = 1·0335 „ „ Ft. hd. water = 0·433 lb. per sq. in. = 62·35 lb. per sq. ft. = 0·0304 „ „ Cub. ft. of water = 62·35 lb. = 0·0278 ton = 28·315 litres = 7·48 U.S. galls. Gall. (Imp.) = 277·27 cu. in. = 0·1604 cu. ft. = 10 lb. water = 4·544 litres. Litre = 1·76 pints = 0·22 gall. = 61 cu. in. = 0·0353 cu. ft. = 0·264 U.S. gall. Horse-power = 33,000 ft.-lb. per min. = 0·746 kilowatt = 42·4 heat units per min. Heat unit = 778 ft.-lb. = 1055 watt-sec. = 107·5 kilogrammetres = 0·252 calorie. Foot-pound = 0·00129 heat unit = 1·36 joules = 0·1383 kilogrammetres. Kilowatt = 1·34 H.P. = 44,240 ft.-lb. per min. = 3412 heat units per hour.

-----

Footnote 1:

It will be recognised that n is the characteristic of the logarithm of
the original number.

Footnote 2:

The special case in which the numerator is 1, 10, or any power of 10
must be treated by the rule for reciprocals (page 27).

Footnote 3:

The possible need for traversing the slide, to change the indices,
when using the C and D scales, is not considered as a setting.

Footnote 4:

The reader may be reminded that cross-multiplication of the factors in
any such slide rule setting will give a constant product, _e.g._, 20 ×
94·5 = 27 × 70.

Footnote 5:

In this case cross _dividing_ gives a constant quotient, _e.g._, 8 ÷ 3
= 4 ÷ 1·5. Since the upper scale is now a scale of reciprocals, the
ratio is really

O ⅛ ¼
───────────
D 1·5 3

Footnote 6:

These lines should not be brought to the working edge of the scale but
should terminate in the horizontal line which forms the border of the
finer graduations, their value being read into the calculation by
means of the cursor (see page 55).

Footnote 7:

The same principle may be applied to the cursor.

Footnote 8:

Philosophical Transactions of the Royal Society, 1815.

------------------------------------------------------------------------

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