The slide rule : $b a practical manualPickworth, Charles N. (Charles Newton)
Science
The slide rule : $b a practical manual
Pickworth, Charles N. (Charles Newton)
Slide-rule
Special graduations, marking the position of constant factors which
frequently enter into engineering calculations, are found on most slide
rules. Usually the values of π = 3·1416 and (π)/(4) = 0·7854—the “gauge
points” for calculating the circumference and area of a circle—are
marked on the upper scales. The first should be given on the lower
scales also. Marks _c_ and _c_^1 are sometimes found on the lower scales
at 1·128 = √((4)/(π)) and at 3·568 = √((40)/(π)). These are useful in
calculating the contents of cylinders and are thus derived:—Cubic
contents of cylinder of diameter _d_ and length _l_ = (π)/(4)_d_^2_l_;
substituting for (π)/(4) its reciprocal (4)/(π), the formula becomes
(_d_^2)/(1·273 × _l_), and by taking the square root of the fractional
part we have (_d_)/(1·128)^2 × _l_. This is now in a very convenient
form, since by setting the gauge point _c_ on C to _d_ on D, we can read
over _l_ on B the cubic contents on A. This example indicates the
principle to be followed in arranging gauge points. Successive
multiplication is avoided by substituting the reciprocal of the
constant, thus bringing the expression into the form (_a_ × _b_)/(_c_),
which, as we know, can be resolved by one setting of the slide. The
advantage of dividing _d_ before squaring is also evident. The mark
_c_^1 = _c_ × √(10) is used if it is necessary to draw the slide more
than one-half its length to the right.
A gauge point, M, at 31·83 = (100)/(π) is found on the upper scales of
some rules. Setting this point on B to the diameter of a cylinder on A,
the circumference is read over 1 or 100 on B or the area of the curved
surface over the length on B.
As another example of establishing a gauge point, we will take the
formula for the theoretical delivery of pumps. If _d_ is the diameter of
the plunger in inches, _l_ the length of stroke in feet, and Q the
delivery in gallons, we have
Q = _d_^2 × (π)/(4) × _l_ × (12)/(277). (N.B.—277 cubic inches = 1
gallon.)
Multiplying out the constant quantities and taking its reciprocal, we
readily transform the statement into Q = (_d_^2_l_)/(29·4) or
((_d_)/(5·42))^2 × _l_. Hence set gauge point 5·42 on C to _d_ on
D and over length of stroke in feet on B, read delivery in gallons per
stroke on A; or over piston speed in feet per minute on B, read
theoretical delivery in gallons per minute on A.
Several examples of gauge points will be found in the section on
calculating the weights of metal (see pages 59 and 60). In most cases
their derivation will be evident from what has been said above. In the
case of the weight of spheres, we have Vol. = 0·5236_d_^3, and this
multiplied by the weight of 1 cubic inch of the material will give the
weight W in lb. Hence for cast-iron, W = 0·5236 × _d_^3 × 0·26, which is
conveniently transformed into W = (_d_ × _d_^2)/(7·35) as in the example
on page 60.
Public-domain text, read in full here on John Shaqi.
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