(Part B) Machinerys Handbook 31st Edition Pages 1484-2979

Machinery's Handbook, 31st Edition

CAMS AND CAM DESIGN

2379

Based upon polar coordinates, the radius of curvature is:

2 2 3

d m c m dr 2 φ − E

r

2

;

c

+

(10)

ρ

=

dr

r d d r 2

r

2 2 +

c

m

d

2

φ

φ

*Positive values (+) indicate convex curve; negative values ( − ), concave. In Equation (10), r = ( R min + y ), where R min is the smallest radius to the pitch curve (see Fig. 12 ) and y is the displacement of the follower from its lowest position given in terms of φ , the angle of cam rotation. The following formulas for r , dr / d φ , and d 2 r / d φ 2 may be substituted into Equation (10) to calculate the radius of curvature at any point of the cam pitch curve; however, to determine the possibility of undercutting of the convex portion of the cam, it is the minimum radius of curvature on the convex portion, ρ min , that is needed. The minimum radius of curvature occurs, generally, at the point of maximum negative acceleration. Parabolic motion: (11a) r R h h 2 1 min 2 β φ = + − − c m

h 720 1 °

dr

β φ

2 # # β

− c m

=

(11b)

d

φ β

φ πβ

h 4 180 2 °

d d r 2 φ

− ^ h

=

(11c) These equations are for the deceleration portion of the curve as explained in the footnote to Table 1. The minimum radius of curvature can occur at either φ = β /2 or at φ = β , depending on the magnitudes of h , R min , and β . Therefore, to determine which is the case, make two calcula­ tions using Formula (10), one for φ = β/ 2, and the other for φ = β . Simple harmonic motion: (12a) 2 2 2 π β cos r R h 2 1 min ; 180 ° β φ = + − c m E

180

2 180

dr

h

φ

°

°

sin

c

m

=

0 ≤ φ ≤ β

(12b)

d

φ

β

β

180

2 180

2 2 ° h

h

d d r 2

= ^

°

φ

cos

c

m

(12c) The minimum radius of curvature can occur at either φ = β /2 or at φ = β , depending on the magnitudes of h , R min , and β . Therefore, to determine which is the case, make two calcula­ tions using Formula (10), one for φ = β/ 2, and the other for φ = β . Cycloidal motion: (13a) 2 φ β β sin r R h 1 360 min ° π φ = + − c m ; E

β φ

2

β

360

h 180 1 °

dr

°

φ

cos

;

E

c

m

=

(13b)

0 ≤ φ ≤ β

d

φ πβ

β

360

h 2 180 2 2 ° πβ h

d d r 2 φ

= ^

°

φ

sin

c

m

(13c)

2

β

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