Question 11.3: Contact Ratio of Meshing Gear and Pinion A gearset has N1 to...

Contact Ratio of Meshing Gear and Pinion

A gearset has N_{1} tooth pinion, N_{2} tooth gear, pressure angle \phi , and diametral pitch P (Figure 11.7).

Find:

a. The contact ratio

b. The pressure angle and contactratio, if the center distance is increased by 0.2 in.

Given: N_{1} = 15, N_{2} = 45, \phi = 20°, P = 2.5 in.^{−1}

a=\frac{1}{P}=\frac{1}{2.5}=0.4  \text { in. (by Table } 11.1 \text { ) }

Assumption: Standard gear sizes are considered.

 

Table 11.1
Commonly Used Standard Tooth Systems for Spur Gears
Item 20° Full Depth 20° Stub 25° Full Depth
Addendum a 1/P 0.8/P 1/P
Dedendum b_{d} 1.25/P l/P 1.25/P
Clearance f 0.25/P 0.2/P 0.25/P
Working depth h_{k} 2/P 1.6/P 2/P
Whole depth h 2.25/P 1.8/P 2.25/P
Tooth thickness t 1.571/P 1.571/P 1.571/P
F11.7
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Applying Equation 11.2, the pitch diameter for the pinion and gear are found to be

P = \frac{N}{d}     (11.2)

d_1=\frac{15}{2.5}=6  in .=152.4  mm \quad \text { and } \quad d_2=\frac{45}{2.5}=18  in .=457.2  mm

Hence, the gear pitch radii are

r_1=3 in .=76.2  mm  \text { and } r_2=9  in .=228.6  mm

a. The center distance c is the sum of the pitch radii. So

c = 3 + 9 =  12 in. = 304.8 mm

The radii of the base circles, using Equation 11.9, are

r_b=r \cos \phi     (11.9)

\begin{array}{l} r_{b 1}=3 \cos 20^{\circ}=2.819  in .=71.6  mm \\ r _{b 2}=9 \cos 20^{\circ}=8.457  in .=214.8  mm \end{array}

Substitution of the numerical values into Equation 11.14 gives the contactratio as

C_r=\frac{1}{p \cos \phi}\left[\sqrt{\left(r_p+a_p\right)^2-\left(r_p \cos \phi\right)^2}+\sqrt{\left(r_g+a_g\right)^2-\left(r_g \cos \phi\right)^2}\right]-\frac{c \tan \phi}{p}      (11.14)

\begin{aligned} c_r &=\frac{2.5}{\pi \cos 20^{\circ}}\left[\sqrt{(3+0.4)^2-(2.819)^2}+\sqrt{(9+0.4)^2-(8.457)^2}\right]-\frac{12 \tan 20^{\circ}}{\pi / 2.5} \\ &=1.61 \end{aligned}

Comment: The result, about 1.6, represents a suitable value.

b. For the case in which the center distance is increased by 0.2 in., we have c = 12.2 in. It follows that

c=\frac{1}{2}\left(d_1+d_2\right), \quad d_1+d_2=2(12.2)=24.4  in .      (b)

By Equation 11.2,

\frac{N_1}{d_1}=\frac{N_2}{d_2}, \frac{15}{d_1}=\frac{45}{d_2}        (c)

Solving Equations (b) and (c), we have d_{1} = 6.1 in. and d_{2} = 18.3 in. or r_{1} = 3.05 in. and r_{2} = 9.15 in.

The diametral pitch becomes P = N_{1}/d_{1} = 15/6.1 = 2.459 in·^{−1}. The addendum is therefore a = a_{1} = a_{2} = 1/2.459 = 0.407 in. Base radii of the gears will remain the same. The new pressure angle can now be obtained from Equation 11.9:

\phi_{\text {new }}=\cos ^{-1}\left(\frac{r_{b 1}}{r_1}\right)=\cos ^{-1}\left(\frac{2.819}{3.05}\right)=22.44^{\circ}

Through the use of Equation 11.14, the new contact ratio is then

\begin{aligned} c_{r, \text { new }} &=\frac{2.459}{\pi \cos 22.44^{\circ}}\left[\sqrt{(3.05+0.407)^2-(2.819)^2}+\sqrt{(9.15+0.407)^2-(8.457)^2}\right]-\frac{12.2 \tan 22.44^{\circ}}{\pi / 2.459} \\ &=1.52 \end{aligned}

Comment: Results show that increasing the center distance leads to an increase in pressure angle but decrease in the contact ratio.

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