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Gear Geometry and Applied Theory Episode 2 Part 1 pot
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P1: FHA/JTH
CB672-10 CB672/Litvin CB672/Litvin-v2.cls February 27, 2004 0:19
10.5 Meshing of Involute Gear with Rack-Cutter 283
Choosing ζ >ζmin, we have to limit ζ due to the possibility of tooth pointing (see
Problem 10.6.2).
(ii) N > Nmin. Then ζ ≤ 0, and the rack-cutter can be displaced toward the gear center,
or the setting can be conventional (ζ = 0).
Change of Gear Tooth Thickness and Dedendum Height
The displacement of the rack-cutter affects the gear tooth thickness and the dedendum
dimension. Henceforth, we consider the change of tooth thickness (space width) that is
measured along the gear pitch circle. The space width of the gear that is measured along
the pitch circle is equal to the tooth thickness of the rack-cutter that is measured along
I–I, the rack-cutter centrode. In the case of the conventional setting of the rack-cutter,
the nominal value of the gear space width is
w = sc = pc
2 = π
2P (10.5.10)
where sc is the tooth thickness of the rack-cutter on the middle-line a–a. When a nonconventional setting of the rack-cutter is provided, the tooth thickness of the rack-cutter
on its centrode I–I is [Fig. 10.5.3(b)]
s ∗
c = sc − 2e tan αc = pc
2 − 2e tan αc . (10.5.11)
The gear space width is
w = s ∗
c = pc
2 − 2e tan αc . (10.5.12)
The radius of the dedendum circle is determined with the equation
rd = rp − b + e, (10.5.13)
and the dedendum height is (b − e). To keep the total height at the gear tooth at the
proper value it is necessary to change the radius of the addendum circle while preparing
the gear blank for cutting.
Problem 10.5.1
Consider a conventional setting of the rack-cutter (e = 0). The radius rG of the circle
where the initial point of the involute curve is located is represented by Eqs. (10.5.1)
and (10.5.2). Represent radius rG in terms of N, αc , and P; take a = 1/P.
Solution
rG = (N2 sin2 αc − 4N sin2 αc + 4) 1
2
2P sin αc
. (10.5.14)
Problem 10.5.2
Consider that radius rG is represented by Eq. (10.5.14). Derive an equation in
terms of N and αc when the initial point of the involute curve belongs to the base
circle.
P1: FHA/JTH
CB672-10 CB672/Litvin CB672/Litvin-v2.cls February 27, 2004 0:19
284 Spur Involute Gears
Figure 10.5.3: Illustration of (a) generation of standard and nonstandard gears and (b) tooth thickness
of the rack-cutter.
Solution
N = 2
sin2 αc
.
Problem 10.5.3
Transform expression (10.5.8) by using Eq. (10.5.4). Represent ζ in terms of N
and αc .
Solution
ζ ≥
2 − N sin2 αc
2 .
Problem 10.5.4
A gear with tooth number N > Nmin is generated by a rack-cutter with the profile angle
αc ; the diametral pitch is P; the addendum of the rack-cutter is b = 1.25/P; a nonconventional setting of the rack-cutter is used (e < 0). Represent in terms of N, αc , and
P1: FHA/JTH
CB672-10 CB672/Litvin CB672/Litvin-v2.cls February 27, 2004 0:19
10.6 Relations Between Tooth Thicknesses Measured on Various Circles 285
P the minimal radius of the gear dedendum circle with which undercutting might still
be avoided.
DIRECTIONS. Use Eq. (10.5.13) for rd . Expression (10.5.7) yields that undercutting may
still be avoided with
e = Nmin − N
P Nmin
= 2 − N sin2 αc
2P .
Solution
rd = N cos2 αc − 0.5
2P . (10.5.15)
Problem 10.5.5
Equation (10.5.15) determines the radius of the dedendum circle when the nonconventional setting of the rack-cutter is applied. The radius of the dedendum circle
when a conventional setting of the rack-cutter is applied is represented by the equation
r ∗
d = rp − 1.25
P .
Determine N in terms of αc when: (i) rd > r ∗
d , (ii) rd = r ∗
d , and (iii) rd < r ∗
d .
Solution
(i) N <
2
sin2 αc
; (ii) N = 2
sin2 αc
; (iii) N >
2
sin2 αc
.
10.6 RELATIONS BETWEEN TOOTH THICKNESSES MEASURED
ON VARIOUS CIRCLES
Consider that the tooth thickness tp =
AA on the pitch circle is given (Fig. 10.6.1). The
goal is to determine the tooth thickness tx =
BB on the circle of given radius rx; tx must
be represented in terms of P, pressure angle αc , tooth number N, and radius rx.
The tooth half-thickness and the corresponding angle β (or βx) are related by the
following equations:
β =
AA
2rp
= tp
2rp
(10.6.1)
βx = tx
2rx
(10.6.2)
Figure 10.6.1 yields
βx = β + inv αc − inv αx (10.6.3)
where inv αc = tan αc − αc , inv αx = tan αx − αx, and
cos αx = rb
rx
= N cos αc
2P rx
. (10.6.4)