Question 3.116: The table gives data concerning the shrink fit of two cylind...

The table gives data concerning the shrink fit of two cylinders of differing materials and 3–119 dimensional specification in inches. Elastic constants for different materials may be found in Table A–5. Identify the radial interference δ, then find the interference pressure p, and the tangential normal stress on both sides of the fit surface. If dimensional tolerances are given at fit surfaces, repeat the problem for the highest and lowest stress levels.

Problem
Number
Inner Cylinder  Outer Cylinder
Material d _{ i } d _{ 0} Material D _{ i } D _{ 0}
3–116 Steel 0 2.002 Steel 2.000 3.00
3–117 Steel 0 2.002 Cast iron 2.000 3.00
3–118 Steel 0 1.002/1.003 Steel 1.001/1.002 2.00
3–119 Aluminum 0 2.003/2.006 Steel 2.000/2.002 3.00
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From Table A-5E_{i}=E_{o}=30  Mpsi , v_{i}=v_{o}=0.292 . \quad r_{i}=0, R=1 \text { in, } r_{o}=1.5 \text { in }

The radial interference is \delta=\frac{1}{2}(2.002-2.000)=0.001  in

Eq. (3-57),

\begin{aligned}p &=\frac{E \delta}{2 R^{3}}\left[\frac{\left(r_{o}^{2}-R^{2}\right)\left(R^{2}-r_{i}^{2}\right)}{r_{o}^{2}-r_{i}^{2}}\right]=\frac{30\left(10^{6}\right) 0.001}{2\left(1^{3}\right)}\left[\frac{\left(1.5^{2}-1^{2}\right)\left(1^{2}-0\right)}{\left(1.5^{2}-0\right)}\right] \\&=8333  psi \doteq 83.3 \text { kpsi } \end{aligned}

The tangential stresses at the interface for the inner and outer members are given by Eqs. (3-58) and (3-59), respectively.

\left.\left(\sigma_{t}\right)_{i}\right|_{r=R}=-p \frac{R^{2}+r_{i}^{2}}{R^{2}-r_{i}^{2}}=-(8333) \frac{1^{2}+0^{2}}{1^{2}-0^{2}}=-8333  psi \doteq-8.33  kpsi

 

\left.\left(\sigma_{t}\right)_{o}\right|_{r=R}=p \frac{r_{o}^{2}+R^{2}}{r_{o}^{2}-R^{2}}=(8333) \frac{1.5^{2}+1^{2}}{1.5^{2}-1^{2}}=21670  psi \doteq 21.7  kpsi

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Eq. (3-57) : p=\frac{E \delta}{2 R^{3}}\left[\frac{\left(r_{o}^{2}-R^{2}\right)\left(R^{2}-r_{i}^{2}\right)}{r_{o}^{2}-r_{i}^{2}}\right]

Eq. (3-58) : \left.\left(\sigma_{t}\right)_{i}\right|_{r=R}=-p \frac{R^{2}+r_{i}^{2}}{R^{2}-r_{i}^{2}}

Eq. (3-59) : \left.\left(\sigma_{t}\right)_{o}\right|_{r=R}=p \frac{r_{o}^{2}+R^{2}}{r_{o}^{2}-R^{2}}

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