Question 6.70: The plan view of a link is the same as in Prob. 6–30; howeve...

The plan view of a link is the same as in Prob. 6–30; however, the forces F are completely reversed, the reliability goal is 0.998, and the material properties are S _{u t} = 64LN(1, 0.045) kpsi and S _{y} = 54LN(1, 0.077) kpsi. Treat Fa as deterministic, and specify the thickness h.

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This is a very important task for the student to attempt before starting Part 3. It illustrates the drawback of the deterministic factor of safety method. It also identifies the a priori decisions and their consequences.
The range of force fluctuation in Prob. 6-30 is – 16 to + 5 kip, or 21 kip. Let the repeatedly-applied F_{a} be 10.5 kip. The stochastic properties of this heat of AISI 1018 CD are given in the problem statement.

Function Consequences
Axial F_{a}=10.5 kip
Fatigue load \begin{aligned}&C_{F a}=0 \\&C_{k c}=0.125\end{aligned}
Overall reliability R ≥ 0.998; z=-3.09
with twin fillets R \geq \sqrt{0.998}=0.999 C_{K f}=0.11
Cold rolled or machined surfaces C_{k a}=0.058
Ambient temperature C_{k d}=0
Use correlation method C_{\phi}=0.138
Stress amplitude \begin{aligned}&C_{K f}=0.11 \\&C_{\sigma a}=0.11\end{aligned}
 Significant strength S_{e} C_{S e}=\left(0.058^{2}+0.125^{2}+0.138^{2}\right)^{1 / 2}=0.195

 

Choose the mean design factor which will meet the reliability goal. From Eq. (6-88)

\begin{aligned}C_{n} &=\sqrt{\frac{0.195^{2}+0.11^{2}}{1+0.11^{2}}}=0.223 \\\bar{n} &=\exp \left[-(-3.09) \sqrt{\ln \left(1+0.223^{2}\right)}+\ln \sqrt{1+0.223^{2}}\right] \\\bar{n} &=2.02\end{aligned}

In Prob. 6-30, it was found that the hole was the significant location that controlled the analysis. Thus,

\begin{aligned}& \sigma _{a}=\frac{ S _{e}}{ n } \\&\bar{\sigma}_{a}=\frac{\bar{S}_{e}}{\bar{n}} \quad \Rightarrow \quad \bar{K}_{f} \frac{F_{a}}{h\left(w_{1}-d\right)}=\frac{\bar{S}_{e}}{\bar{n}}\end{aligned}

We need to determine \bar{S}_{e}

\begin{aligned}\bar{k}_{a} &=2.67 \bar{S}_{u t}^{-0.265}=2.67(64)^{-0.265}=0.887 \\k_{b} &=1 \\\bar{k}_{c} &=1.23 \bar{S}_{u t}^{-0.0778}=1.23(64)^{-0.0778}=0.890 \\\bar{k}_{d} &=\bar{k}_{e}=1 \\\bar{S}_{e} &=0.887(1)(0.890)(1)(1)(0.506)(64)=25.6 kpsi\end{aligned}

From the solution to Prob. 6-30, the stress concentration factor at the hole is K_{t}=2.68.
From Eq. (6-78) and Table 6-15

\begin{aligned}&\bar{K}_{f}=\frac{2.68}{1+\frac{2(2.68-1)}{2.68} \frac{5 / 64}{\sqrt{0.2}}}=2.20 \\&h=\frac{\bar{K}_{f} \bar{n} F_{a}}{\left(w_{1}-d\right) \bar{S}_{e}}=\frac{2.20(2.02)(10.5)}{(3.5-0.4)(25.6)}=0.588\end{aligned}

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Eq. (6-78) : \bar{K}_{f}=\frac{K_{t}}{1+\frac{2\left(K_{t}-1\right)}{K_{t}} \frac{\sqrt{a}}{\sqrt{r}}}

Eq. (6-88) : \bar{n}=\exp \left[-z \sqrt{\ln \left(1+C_{n}^{2}\right)}+\ln \sqrt{1+C_{n}^{2}}\right] \doteq \exp \left[C_{n}\left(-z+C_{n} / 2\right)\right]

 

 

Table 6–15
Heywood’s Parameter
√a and coefficients of
variation C_{K f} for steels
Notch Type \sqrt{ a }(\sqrt{\text { in }}) ,S_{\text {ut }} \text{in kpsi} \sqrt{ a }(\sqrt{ m m }) , S_{\text {ut }} \text{in MPa} Coefficient of Variation C_{K f}
Transverse hole 5 / S_{u t} 174 / S_{u t} 0.1
Shoulder 4 / S_{u t} 139 / S_{u t} 0.11
Groove 3 / S_{u t} 104 / S_{u t} 0.15

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