Question 13.78: A hollow shaft with an outside diameter of 57 mm and an insi...

A hollow shaft with an outside diameter of 57 mm and an inside diameter of 47 mm is subjected to torque T. The shaft is made of aluminum [E = 70 GPa; ν = 0.33]. A strain gage is mounted on the shaft at the orientation shown in Figure P13.78.
(a) If T = 900 N-m, determine the strain reading that would be expected from the gage.
(b) If the gage indicates a strain value of ε = −1,400 με, determine the torque T applied to the shaft.

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(a) The cross-sectional area of the hollow shaft is

A=\frac{\pi}{4}\left(D^{2}-d^{2}\right)=\frac{\pi}{4}\left[(57  mm )^{2}-(47  mm )^{2}\right]=816.814  mm ^{2}

and the polar moment of inertia for the shaft is

J=\frac{\pi}{32}\left[D^{4}-d^{4}\right]=\frac{\pi}{32}\left[(57  mm )^{4}-(47  mm )^{4}\right]=557,271.413  mm ^{4}

The maximum shear stress in the hollow aluminum shaft (i.e., the shear stress on the outer surface) is found from the elastic torsion formula:

\tau_{\max }=\frac{T c}{J}=\frac{(900  N – m )(57  mm / 2)(1,000  mm / m )}{557,271.413  mm ^{4}}=46.028  MPa

The normal stresses in the x and y directions are zero; therefore, the stresses in the shaft at the location of the strain gage can be summarized as

\sigma_{x}=0  MPa , \quad \sigma_{y}=0  MPa , \quad \tau_{x y}=-46.028  MPa

Note: The negative sign on \tau_{x y} is determined by inspection. The stress element at the location of the strain gage looks like this:

From Eq. (13.18), determine the shear modulus G:

G=\frac{E}{2(1+v)}=\frac{70,000  MPa }{2(1+0.33)}=26,315.8  MPa

and compute the shear strain \gamma_{x y} from Eq. (13.22):

\gamma_{x y}=\frac{\tau_{x y}}{G}=\frac{-46.028  MPa }{26,315.8  MPa }=-1,749.058 \times 10^{-6}  rad

Write a normal strain transformation equation for the gage oriented at θ = 55°:

\begin{aligned}\varepsilon_{n} &=\varepsilon_{x} \cos ^{2} \theta+\varepsilon_{y} \sin ^{2} \theta+\gamma_{x y} \sin \theta \cos \theta \\&=(0  \mu \varepsilon) \cos ^{2}\left(55^{\circ}\right)+(0  \mu \varepsilon) \sin ^{2}\left(55^{\circ}\right)+(-1,749.058  \mu rad ) \sin \left(55^{\circ}\right) \cos \left(55^{\circ}\right) \\&=-821.788  \mu \varepsilon\end{aligned}

Therefore, the strain gage should be expected to read a normal strain of

\varepsilon_{n}=-822  \mu \varepsilon

 

(b) A normal strain transformation equation can be written for the gage:

\begin{gathered}\varepsilon_{n}=\varepsilon_{x} \cos ^{2} \theta+\varepsilon_{y} \sin ^{2} \theta+\gamma_{x y} \sin \theta \cos \theta \\\therefore    -1,400  \mu \varepsilon=\gamma_{x y} \sin \left(55^{\circ}\right) \cos \left(55^{\circ}\right)\end{gathered}

recognizing that the normal stresses in the x and y directions are zero.

From Eq. (13.22), substitute for \gamma_{x y}:

-1,400  \mu \varepsilon=\frac{\tau_{x y}}{G} \sin \left(55^{\circ}\right) \cos \left(55^{\circ}\right)

Solve for \tau_{x y}:

\tau_{x y}=\frac{\left(-1,400 \times 10^{-6}  rad \right)(26,315.8  MPa )}{\sin \left(55^{\circ}\right) \cos \left(55^{\circ}\right)}=-78.413  MPa

The torque T that causes this shear stress is

T=\frac{\tau_{x y} J}{c}=\frac{\left(78.413  N / mm ^{2}\right)\left(557,271.413  mm ^{4}\right)}{(57  mm / 2)}=1,533,241  N – mm =1.533  kN – m

 

 

 

 

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