Repeat Prob. 2–28, except that the design situation is failure by excessive deflection, and it is
desired to minimize the weight.
Repeat Prob. 2–28, except that the design situation is failure by excessive deflection, and it is
desired to minimize the weight.
Eq. (2-26), p. 65, applies to a circular cross section. However, for any cross section shape it can be shown that I=C A^{2}, where C is a constant. For example, consider a rectangular section of height h and width b, where for a given scaled shape, h=c b, where c is a
constant. The moment of inertia is I=b h^{3} / 12, and the area is A=b h. Then I=h\left(b h^{2}\right) / 12 =c b\left(b h^{2}\right) / 12=(c / 12)(b h)^{2}=C A^{2}, where C=c / 12 (a constant)
Thus, Eq. (2-27) becomes
A=\left(\frac{k l^{3}}{3 C E}\right)^{1 / 2}and Eq. (2-29) becomes
m=A l \rho=\left(\frac{k}{3 C}\right)^{1 / 2} l^{5 / 2}\left(\frac{\rho}{E^{1 / 2}}\right)Thus, minimize f_{3}(M)=\frac{\rho}{E^{1 / 2}}, or maximize M=\frac{E^{1 / 2}}{\rho}. From Fig. (2-16)
From the list of materials given, aluminum alloys are clearly the best followed by steels and tungsten carbide. Polycarbonate polymer is not a good choice compared to the other candidate materials. .
Eq. (2-26)
I=\frac{\pi D^{4}}{64}=\frac{A^{2}}{4 \pi}Eq. (2-27)
A=\left(\frac{4 \pi k l^{3}}{3 E}\right)^{1 / 2}Eq. (2-29)
m=2 \sqrt{\frac{\pi}{3}}\left(k^{1 / 2}\right)\left(l^{5 / 2}\right)\left(\frac{\rho}{E^{1 / 2}}\right)