CHAPTER XII.

_PLOTTING MECHANICAL MOTIONS._

[Illustration: Fig. 257.]

Let it be required to find how much motion an eccentric will give to its

rod, the distance from the centre of its bore to the centre of the

circumference, which is called the throw, being the distance from A to B

in Figure 257. Now as the eccentric is moved around by the shaft, it is

evident that the axis of its motion will be the axis A of the shaft.

Then from A as a centre, and with radius from A to C, we draw the dotted

circle D, and from E to F will be the amount of motion of the rod in the

direction of the arrow.

This becomes obvious if we suppose a lead pencil to be placed against

the eccentric at E, and suppose the eccentric to make half a revolution,

whereupon the pencil will be pushed out to F. If now we measure the

distance from E to F, we shall find it is just twice that from A to B.

We may find the amount of motion, however, in another way, as by

striking the dotted half circle G, showing the path of motion of B, the

diameter of this path of motion being the amount of lateral motion given

to the rod.

[Illustration: Fig. 258.]

In Figure 258 is a two arm lever fast upon the same axis or shaft, and

it is required to find how much a given amount of motion of the long arm

will move the short one. Suppose the distance the long arm moves is to

A. Then draw the line B from A to the axis of the shaft, and the line C

the centre line of the long arm. From the axis of the shaft as a centre,

draw the circle D, passing through the eye or centre E of the short arm.

Take the radius from F to G, and from E as a centre mark it on D as at

H, and H is where E will be when the long arm moves to A. We have here

simply decreased the motion in the same proportion as one arm is shorter

than the other. The principle involved is to take the motion of both

arms at an equal distance from their axis of motion, which is the axis

of the shaft S.

[Illustration: Fig. 259.]

In Figure 259 we have a case in which the end of a lever acts directly

upon a shoe. Now let it be required to find how much a given motion of

the lever will cause the shoe to slide along the line _x_; the point H

is here found precisely as before, and from it as a centre, the dotted

circle equal in diameter to the small circle at E is drawn from the

perimeter of the dotted circle, a dotted line is carried up and another

is carried up from the face of the shoe. The distance K between these

dotted lines is the amount of motion of the shoe.

In Figure 260 we have the same conditions as in Figure 259, but the

short arm has a roller acting against a larger roller R. The point H is

found as before. The amount of motion of R is the distance of K from J;

hence we may transfer this distance from the centre of R, producing the

point P, from which the new position may be marked by a dotted circle as

shown.

[Illustration: Fig. 260.]

In Figure 261 a link is introduced in place of the roller, and it is

required to find the amount of motion of rod R. The point H is found as

before, and then the length from centre to centre of link L is found,

and with this radius and from H as a centre the arc P is drawn, and

where P intersects the centre line J of R is the new position for the

eye or centre Q of R.

[Illustration: Fig. 261.]

In Figure 262 we have a case of a similar lever actuating a plunger in a

vertical line, it being required to find how much a given amount of

motion of the long arm will actuate the plunger. Suppose the long arm to

move to A, then draw the lines B C and the circle D. Take the radius or

distance F, G, and from E mark on D the arc H. Mark the centre line J of

the rod. Now take the length from E to I of the link, and from H as a

centre mark arc K, and at the intersection of K with J is where the eye

I will be when the long arm has moved to A.

[Illustration: Fig. 262.]

In Figure 263 are two levers upon their axles or shafts S and S'; arm A

is connected by a link to arm B, and arm C is connected direct to a rod

R. It is required to find the position of centre G of the rod eye when D

is in position E, and when it is also in position F. Now the points E

and F are, of course, on an arc struck from the axis S, and it is

obvious that in whatever position the centre H may be it will be

somewhere on the arc I, I, which is struck from the centre S'. Now

suppose that D moves to E, and if we take the radius D, H, and from E

mark it upon the arc I as at V, then H will obviously be the new

position of H. To find the new position of G we first strike the arc J,

J, because in every position of G it will be somewhere on the arc J, J.

To find where that will be when H is at V, take the radius H, G, and

from V as a centre mark it on J, J, as at K, which is the position of G

when D is at E and H is at V. For the positions when D is at F we repeat

the process, taking the radius D, H, and from F marking P, and with the

radius H, G, and from P as a centre marking Q; then P is the new

position for H, and Q is that for G.

[Illustration: Fig. 263.]

In Figure 264 a lever arm A and cam C are in one piece on a shaft. S is

a shoe sliding on the line _x_, and held against the cam face by the rod

R; it is required to find the position of the face of the shoe against

the cam when the end of the arm is at D.

Draw line E from D to the axis of the shaft and line F. From the shaft

axis as a centre draw circle W; draw line J parallel to _x_. Take the

radius G H, and from K as a centre mark point P on W; draw line Q from

the shaft axis through P, and mark point T. From the shaft axis as a

centre draw from T an arc, cutting J at V, and V is the point where the

face of the shoe and the face of the cam will touch when the arm stands

at D.

[Illustration: Fig. 264.]

Let it be required to find the amount of motion imparted in a straight

line to a rod attached to an eccentric strap, and the following

construction may be used. In Figure 265 let A represent the centre of

the shaft, and, therefore, the axis about which the eccentric revolves.

Let B represent the centre of the eccentric, and let it be required to

find in what position on the line of motion _x_, the centre C of the rod

eye will be when the centre B of the eccentric has moved to E. Now since

A is the axis, the centre B of the eccentric must rotate about it as

denoted by the circle D, and all that is necessary to find the position

of C for any position of eccentric is to mark the position of B on

circle D, as at E, and from that position, as from E, as a centre, and

with the length of the rod as a radius, mark the new position of C on

the line _x_ of its motion. With the centre of the eccentric at B, the

line Q, representing the faces of the straps, will stand at a right

angle to the line of motion, and the length of the rod is from B to C;

when the eccentric centre moves to E, the centre line of the rod will be

moved to position P, the line Q will have assumed position R, and point

C will have moved from its position in the drawing to G on line _x_. If

the eccentric centre be supposed to move on to F, the point C will move

to H, the radii B C, E G, and F H all being equal in length. Now when

the eccentric centre is at E it will have moved one-quarter of a

revolution, and yet the point C will only have moved to G, which is not

central between C and H, as is denoted by the dotted half circle I.

[Illustration: Fig. 265.]

On the other hand, while the eccentric centre is moving from E to F,

which is but one-quarter of a revolution, the rod end will move from G

to H. This occurs because the rod not only moves _endwise_, but the end

connected to the eccentric strap moves towards and away from the line

_x_. This is shown in the figure, the rod centre line being marked in

full line from B to _x_. And when B has moved to E, the rod centre line

is marked by dotted line E, so that it has moved away from the line of

motion B _x_. In Figure 266 the eccentric centre is shown to stand at an

angle of 45 degrees from line _q_, which is at a right angle to the line

of motion _x x_, and the position of the rod end is shown at C, J and H

representing the extremes of motion, and G the centre of the motion.

[Illustration: Fig. 266.]

If now we suppose the eccentric centre to stand at T, which is also an

angle of 45 degrees to _q_, then the rod end will stand at K, which is

further away from G than C is; hence we find that on account of the

movement of the rod out of the straight end motion, the motion of the

rod end becomes irregular in proportion to that of the eccentric, whose

action in moving the eye C of the rod in a straight line is increased

(by the rod) while it is moving through the half rotation denoted by V

in figure, and diminished during the other half rotation.

In many cases, as, for example, on the river steamboats in the Western

and Southern States, cams are employed instead of eccentrics, and the

principles involved in drawing or marking out such cams are given in the

following remarks, which contain the substance of a paper read by Lewis

Johnson before the American Society of Mechanical Engineers. In Figure

267 is a side view of a pair of cams; one, C, being a full stroke cam

for operating the valve that admits steam to the engine cylinder; and

the other, D, being a cam to cut off the steam supply at the required

point in the engine stroke. The positions of these cams with relation to

the position of the crank-pin need not be commented upon here, more than

to remark that obviously the cam C must operate to open the steam inlet

valve in advance of cam D, which operates to close it and cause the

steam to act expansively in the cylinder, and that the angle of the

throw line of the cut-off valve D to the other cam or to the crank-pin

varies according as it is required to cut off the steam either earlier

or later in the stroke.

[Illustration: Fig. 267.]

The cam yoke is composed of two halves, Y and Y', bolted together by

bolts B, which have a collar at one end and two nuts at the other end,

the inner nuts N N enabling the letting together of the two halves

of the yoke to take up the wear. It is obvious that as the shaft

revolves and carries the cam with it, it will, by reason of its shape,

move the yoke back and forth; thus, in the position of the parts shown

in Figure 267, the direction of rotation being denoted by the arrow, cam

C will, as it rotates, move the yoke to the left, and this motion will

occur from the time corner _a_ of the cam meets the face of Y' until

corner _b_ has passed the centre line _d_. Now since that part of the

circumference lying between points _a_ and _b_ of the cam is an arc of a

circle, of which the axis of the shaft is the centre, the yoke will

remain at rest until such time as _b_ has passed line _d_ and corner _a_

meets the jaw Y of the yoke; hence the period of rest is determined by

the amount of circumference that is made concentric to the shaft; or, in

other words, is determined by the distance between _a_ and _b_.

The object of using a cam instead of an eccentric is to enable the

opening of the valves abruptly at the beginning of the piston stroke,

maintaining a uniform steam-port opening during nearly the entire length

of stroke, and as abruptly closing the valves at the termination of the

stroke.

Figure 268 is a top view of the mechanism in Figure 267; and Figure 269

shows an end view of the yoke. At B, in Figure 268, is shown a guide

through which the yoke-stem passes so as to be guided to move in a

straight line, there being a guide of this kind on each side of the

yoke.

[Illustration: Fig. 268.]

The two cams are bolted to a collar that is secured to the crank-shaft,

and are made in halves, as shown in the figures and also in Figures 270

and 271, which represent cams removed from the other mechanism. To

enable a certain amount of adjustment of the cams upon the collar, the

bolts which hold them to the collar fit closely in the holes in the

collar, but the cams are provided with oblong bolt holes as shown, so

that the position of either cam, either with relation to the other cam

or with relation to the crank-pin, can be adjusted to the extent

permitted by the length of the oblong holes.

[Illustration: Fig. 269.]

The crank is assumed in the figures to be on its dead centre nearest to

the engine cylinder, and to revolve in the direction of the arrows. The

cams are so arranged that their plain unflanged surfaces bolt against

the collar.

The method of drawing or marking out a full stroke cam, such as C in

Figure 267, is illustrated in Figure 272, in which the dimensions are

assumed to be as follows:

Diameter of crank shaft, 7-1/2 inches; travel of cam, 3 inches; width of

yoke, 18 inches.

[Illustration: Fig. 270.]

The circumference of the cam is composed of four curved lines, P, P', K

1, and K 2. The position of the centre of the crank shaft in this

irregularly curved body is at X. The arcs K 1 and K 2 differ in radius,

but are drawn from the same point, X, and hence are concentric with the

crank shaft.

The arcs P, P', are of like radius, but are drawn from the opposite

points S, S', shown at the intersection of the arcs P, P', with the

arc K 1. Thus arcs P, P', are eccentric to the crank shaft.

[Illustration: Fig. 271.]

[Illustration: Fig. 272.]

[Illustration: Fig. 273.]

To draw the cam place one point of the dividers at X, which is the

centre of the crank shaft, and draw the circle E equal to width of yoke,

18 inches. Through this centre X, draw the two right lines A and B. On

the line B, at the intersection of the curved line E, draw the two

vertical lines A 1, A 1. With a radius of 10-1/2 inches, and with one

point of the dividers at X, draw the arc K 1. With a radius of 7-1/2

inches, and one point of the dividers at X, draw the arc K 2. With a

radius of 18 inches, and one point of the dividers at the intersection

of the arc E, with the vertical line A 1 at S, draw the arc P opposite

to S, and let it merge or lose itself in the curved line K 2. Draw the

other curved line P' from the other point S, and we have a full stroke

cam of the dimensions required, and which is represented in Figure 273,

removed from the lines used in constructing it.

[Illustration: Fig. 274.]

The engravings from and including Figure 274 illustrate the lines

embracing cut-off cams of varying limits of cut-off, but all of like

travel and dimensions, which are the same as those given for the full

stroke cam in Figure 272.

In drawing cut-off cams, the stroke of the engine plays a part in

determining their conformation, and in the examples shown this is

assumed to be 4 feet. Figure 274 illustrates the manner of finding

essential points in drawing or marking out cut-off cams. With X as a

centre, and a radius of 2 feet, draw the circle E 1, showing the path of

the crank-pin in making a revolution. This circle has a diameter of 4

feet, equal to the stroke of the engine. Draw the horizontal line B,

passing through the centre of circle E 1. Within the limits of circle E

1, subdivide line B into eight equal parts, as at 1, 2, 3, 4, etc. Draw

the vertical lines, 1, 2, 3, 4, etc., until they each intersect the

circle E 1.

[Illustration: Fig. 275.]

With X as a centre, draw the circle E, having a diameter of 18 inches,

equal to the space in the yoke embracing the cam.

From the centre X draw the series of radial lines through the points of

intersection of the vertical lines 1, 2, 3, 4, etc., from the circle E

1, and terminating at X. We will now proceed to utilize the scale

afforded by Figure 274, in laying off the cut-off cam shown in Figure

276, of half stroke limit.

[Illustration: Fig. 276.]

With X as a centre, draw the circle E, Figure 275, having a diameter of

18 inches. Bisect this circle with the straight lines A and B, which

bear the same relation to their enclosing circle that the lines A, B,

do to the circle E in Figure 274.

[Illustration: Fig. 277.]

It will be observed, in Figure 274, that the vertical line A is (at the

top half) also No. 4, representing 4/8, or half of the stroke. With a

radius of 18 inches, and one point of the dividers placed at V, which is

at the intersection of the circle E with the horizontal line B in Figure

275, draw the arc P. With the same radius and with one compass point

rested at V', draw the arc P'; then two arcs, P and P', intersecting at

the point S.

With the same radius and one point of the compasses at S, draw the arc H

H. The arcs K 1 and K 2 are drawn from the centre X, with a radius of

10-1/2 for K 1 and 7-1/2 inches for K 2, and only serve in a half

stroke cam to intersect the curved lines already drawn, as shown in

Figure 275. In practice, the sharp corner at S would be objectionable,

owing to rapid wear at this point; and hence a modification of the

dimensions for this half stroke cam would be required to obtain a larger

wearing surface at the point S, but the cam of this limit (1/2 stroke)

is correctly drawn by the process described with reference to Figure

275, the outline of the cam so constructed being shown in Figure 276.

[Illustration: Fig. 278.]

In Figure 278 is shown a cam designed to cut off the steam at

five-eighths of the piston stroke, the construction lines being given

in Figure 277, for which draw circle E and straight lines A and B, as in

the preceding example. By reference to Figure 274 it will be observed

that the diagonal line drawn through circle E at 5 is drawn from the

straight line marked 5, which intersects circle E 1, and as this

straight line 5 represents five-eighths of the stroke laid off on line

B, it determines the limit of cut-off on the five-eighths cam in Figure

277.

[Illustration: Fig. 279.]

Turning then to Figure 274, take on circle E the radius from radial line

4 to radial line 5, and mark it in Figure 277 from the vertical line

producing V'.

Now, with a radius of 18 inches, and one point of the dividers fixed at

point V, forming the intersection of the circle E with the horizontal

line B, draw the arc P. With the same radius, and one point of the

dividers fixed at point V', draw the opposite arc P'. With a radius of

10-1/2 inches from the centre X, draw the arc K 1, intersecting lines P

P', at S S. With a radius of 7-1/2 inches, draw the curved line K 2,

opposite to curved line K 1. Now, with a radius of 18 inches, and one

point of the dividers fixed alternately at S S, draw the arcs H, H, from

their intersection with the circle E, until they merge into the curved

line K 2. These curved lines embrace a cut-off cam of five-eighths

limit, shown complete in Figure 278.

[Illustration: Fig. 280.]

From the instructions already given it should be easy to understand that

the three-fourths and seven-eighths cams, shown in Figures 279, 280, 281

and 282, are drawn by taking the points of their cut-off from the same

scale shown in Figure 274, at the diagonal points 6 and 7, intersecting

circle E in that figure; and cut-off cams of intermediate limit of

cut-off can be drawn by further subdividing the stroke line B, in Figure

274, into the required limits.

[Illustration: Fig. 281.]

Cut-off cams of any limit are necessarily imperfect in their operations

as to uniformity of cut-off from opposite ends of the slides, not from

any defect in the rule for laying them off, but from the well-known fact

of the crank pin travelling a greater distance, while driven by the

piston from the centre of the cylinder, through its curved path from the

cylinder, over its centre, and back to the centre of the cylinder, than

in accomplishing the remaining distance of its path in making a complete

revolution; and, although the subdivisions of eighths of the stroke

line B, in Figure 274, does not truly represent a like division of the

piston stroke, owing to deviation, caused by inclination of the

connecting rod in traversing from the centres to half stroke, still it

will be found that laying off a cut-off cam by this rule is more nearly

correct than if the divisions on stroke line B were made to correspond

exactly with a subdivision of piston stroke into eighths.

[Illustration: Fig. 282.]

The cut-off in cams laid off by the rules herein described is greater in

travelling from one side of the slides than in travelling from the

opposite end, one cut-off being more than the actual cut-off of piston

stroke, and the other less; and in practical use, owing to play or lost

motion in the connections from cam to valve, the actual cut-off is less

than the theoretical; hence cut-off cams are usually laid off to

compensate for lost motion; that is, laid off with more limit; for

instance, a five-eighths cam would be laid off to cut-off at

eleven-sixteenths instead of five-eighths.

[Illustration: Fig. 283.]

Figure 283 represents the motion a crank, C, imparts to a connecting

rod, represented by the thick line R, whose end, B, is supposed to be

guided to move in a straight line. The circle H represents the path of

the crank-pin, and dots 1, 2, 3, etc., are 24 different crank-pin

positions equidistant on the circle of crank-pin revolution. Suppose the

crank-pin to have moved to position 1, and with the compasses set to the

length of the rod R, we set one point on the centre of position 1, and

mark on the line of motion _m_ the line _a_, which will be the position

rod end B will have moved to. Suppose next that the crank-pin has moved

into position 2, and with the compass point on the centre of 2 we mark

line 2, showing that while the crank-pin moved from 1 to 2, the rod end

moved from _a_ to _b_; by continuing this process we are enabled to

discern the motion for the whole of the stroke. The backward stroke will

be the same, for corresponding crank-pin positions, for both strokes;

thus, when the rod end is at 7 the crank-pin may be at 7 or at 17. This

fact enables us to find the positions for the positions later than 6, on

the other side of the circle, as at 17, 16, 15, etc., which keeps the

engraving clear.

[Illustration: Fig. 284.]

In Figure 284 a pinion, P, drives a gear-wheel, D, on which there is a

pin driving the sliding die A in the link L, which is pivoted at C, and

connected at its upper end to a rod, R, which is connected to a bolt, B,

fast to a slide, S. It is required to find the motion of S, it moving in

a straight line, dotted circle H' representing the path of the pin in

the sliding die A, arc H representing the line of motion of the upper

end of link L, and lines N, O, its centre line at the extreme ends of

its vibrating motion. In Figure 285 the letters of reference refer to

the same parts as those in Figure 284. We divide the circle H' of pin

motion into 24 equidistant parts marked by dots, and through these we

draw lines radiating from centre, C, and cutting arc H, obtaining on the

arc H the various positions for end Z of rod R, these positions being

marked respectively 1, 2, 3, 4, etc., up to 24. With a pair of

compasses set to the length of rod R from 1 on H, as a centre, we mark

on the line of motion of the slide, line _a_, which shows where the

other end of rod R will be (or in other words, it shows the position of

bolt B in Figure 284), when the centre of A, Figure 284, is in position

1, Figure 285.

[Illustration: Fig. 285.]

From 2 on arc H, we mark with the compasses line _b_ on line M, showing

that while the pin moved from 1 to 2, the rod R would move slide S,

Figure 284, from _a_ to _b_, in Figure 285. From 3 we mark _c_, and so

on, all these marks being above the horizontal line M, representing the

line of motion, and being for the forward stroke. For the backward

stroke we draw the dotted line from position 17 up to arc H, and with

the compasses at 17 mark a line beneath the line M of motion, pursuing

the same course for all the other pin motions, as 18, 19, etc., until

the pin arrives again at position 24, and the link at O, and has made a

full revolution, and we shall have the motion of the forward stroke

above and that of the backward one below the line of motion of the

slide, and may compare the two.

[Illustration: Fig. 286.]

[Illustration: Fig. 287.]

[Illustration: Fig. 288.]

[Illustration: Fig. 289.]

Figures 286 and 287 represent the Whitworth quick return motion that is

employed in many machines. F represents a frame supporting a fixed

journal, B, on which revolves a gear-wheel, G, operated by a pinion, P.

At A is an arm having journal bearing in B at C. This arm is driven by a

pin, D, fast in the gear, G; hence as the gear revolves, pin D moves A

around on C as a centre of motion. A is provided with a slot carrying a

pin, X, on which is pivoted the rod, R. The motion of end N of the rod R

being in a straight line, M, it is required to find the positions of N

during twenty-four periods in one revolution of G. In Figure 288 let H'

represent the path of motion of the driving pin D, about the centre of

B, and H the path of motion of X about the centre C; these two centres

corresponding to the centres of B and C respectively, in Figure 287. Let

the line M correspond to the line of motion M in Figure 286. Now since

it is the pin D, Figure 287, that drives, and since its speed of

revolution is uniform, we divide its circle of motion H' into

twenty-four equal divisions, and by drawing lines radiating from centre

C, and passing through the lines of division on H' we get on circle H

twenty-four positions for the pin X in Figure 286. Then setting the

compasses to the length of the rod (R, Figure 286), we mark from

position 1 on circle H as a centre line, _a_; from position 2 on H we

mark line _b_, and so on for the whole twenty-four positions on circle

H, obtaining from _a_ to _n_ for the forward, and from _n_ to _y_ for

the motion during the backward stroke. Suppose now that the mechanism

remaining precisely the same as before, the line M of motion be in a

line with the centres C, B, instead of at a right angle to it, as it is

in Figure 286, and the motion under this new condition will be as in

Figure 289; the process for finding the amount of motion along M from

the motion around H being precisely as before.

[Illustration: Fig. 290.]

In Figure 290 is shown a cutter-head for a wood moulding machine, and it

is required to find what shape the cutting edge of the cutter must be

to form a moulding such as is shown in the end view of the moulding in

the figure. Now the line A A being at a right angle to the line of

motion of the moulding as it is passed beneath the revolving cutter, or,

what is the same thing, at a right angle to the face of the table on

which the moulding is moved, it is obvious that the highest point C of

the moulding will be cut to shape by the point C of the cutter; and that

since the line of motion of the end of the cutter is the arc D, the

lowest part of the cutter action upon the moulding will be at point E.

It will also be obvious that as the cutter edge passes, at each point,

its length across the line A A, it forms the moulding to shape, while

all the cutting action that occurs on either side of that line is

serving simply to remove material. All that we have to consider,

therefore, is the action on line A A.

It may be observed also that the highest point C of the cutter edge must

not be less than 1/4 inch from the corner of the cutter head, which

gives room for the nut N (that holds the cutter to the head) to pass

over the top of the moulding in a 2-1/2 inch head. In proportion as the

heads are made larger, however, less clearance is necessary for the nut,

as is shown in Figure 291, the cutter edge extending to C, and therefore

nearly up to the corner of the head. Its path of motion at C is shown by

dotted arc B, which it will be observed amply clears the nut N. In

practice, however, point C is not in any size of cutter-head placed

nearer than 1/4 inch from corner X of the cutter-head.

To find the length of the cutter edge necessary to produce a given depth

of moulding, we may draw a circle _i_, Figure 292, equal in diameter to

the size of the cutter head to be used, and line A A. The highest point

of cutting edge being at _e_, and the lowest at g, then circles _d_ and

_f_ represent the line of motion of these two points; and if we mark the

cutter in, the necessary length of cutting edge on the cutter is

obviously from _a_ to _b_.

[Illustration: Fig. 291.]

[Illustration: Fig. 292.]

Now the necessary depth of cutter edge being found for any given

moulding, or part of a moulding, the curves for the edge may be found as

follows: Suppose the moulding is to be half round, as in the end view in

Figure 290. The width of the cutter must of course equal the width of

the moulding, and the length or depth of cutting edge required may be

found from the construction shown in Figure 292; hence all that remains

is to find the curve for the cutting edge. In Figure 293, let A A

represent the centre of the cutter width, its sides being F F', and its

end B B. From centre C draw circle D, the upper half of which will serve

to represent the moulding. Mark on A the length or depth the cutting

edge requires to be, ascertaining the same from the construction shown

in Figure 292, and mark it as from C to K'. Then draw line E E, passing

through point K. Draw line G, standing at the same angle to A A as the

face _h b_, Figure 292, of the cutter does to the line A A, and draw

line H H, parallel to G. From any point on G, as at I, with radius J,

draw a quarter of a circle, as K. Mark off this quarter circle into

equal points of division, as by 1, 2, 3, etc., and from these points of

division draw lines, as _a_, _b_, _c_, etc.; and from these lines draw

horizontal lines _d_, _e_, _f_, etc. Now divide the lower half of circle

D into twice as many equal divisions as quarter circle K is divided

into, and from these points of division draw perpendiculars _g_, _h_,

_i_, etc. And where these perpendiculars cross the horizontal lines, as

_d_, will be points through which the curve may be drawn, three of such

points being marked by dots at _p_, _q_, _r_. If the student will, after

having drawn the curve by this construction, draw it by the construction

that was explained in connection with Figure 79, he will find the two

methods give so nearly identical curves, that the latter and more simple

method may be used without sensible error.

[Illustration: Fig. 293.]

[Illustration: Fig. 294.]

When the curves of the moulding are not arcs of circles they may be

marked as follows:

Take the drawing of the moulding and divide each member or step of it by

equidistant lines, as _a_, _b_, _c_, _d_, _e_, _f_, _g_, in Figure 294;

above the moulding draw lines representing the cutter, and having found

the depth of cutting edge for each member by the construction shown in

Figure 292, finding a separate line, _a b_, for each member of the

moulding, transfer the depths so found to the face of the cutter; divide

the depth of each member of the cutter into as many equal divisions as

the corresponding member of the moulding is divided into, as by lines

_h_, _i_, _j_, _k_, _l_, _m_, _n_. Then draw vertical lines, as _o_,

_p_, _q_, _r_, etc.; and where these lines meet the respective lines

_h_, _i_, _j_, etc., are points in the curve, such points being marked

on the cutter by dots.

Mechanical Drawing Self-Taught Comprising instructions in the selection and preparation of drawing instruments, elementary instruction in practical mechanical drawing; together with examples in simple geometry and elementary mechanism, including screw threads, gear wheels, mechanical motions, engines and boilers · 第 12 / 15 章