Concept:
A key is a mechanical component inserted between a rotating machine shaft and the hub of a pulley or gear to facilitate torque transmission. During operation, the transmitted torque \(T\) creates a tangential shearing force \(F\) at the outer surface boundary of the shaft.
The relationship connecting the torque \(T\), the tangential force \(F\), and the shaft radius (\(r = \frac{d}{2}\)) is written as:
\[
T = F \cdot \left(\frac{d}{2}\right) \quad \Rightarrow \quad F = \frac{2T}{d}
\]
This tangential force \(F\) acts directly on the critical shear plane of the embedded key. Let the key have width \(w\), thickness \(h\), and length \(l\). For a square key, the width matches the thickness:
\[
w = h = \frac{d}{4}
\]
Step 1: Determining the shearing area of the key.
Shear failure occurs when the key splits along its mid-plane parallel to the tangent of the shaft surface. The area resisting this shearing force is the product of the key's width (\(w\)) and its inserted length (\(l\)):
\[
A_{\text{shear}} = w \cdot l
\]
Substituting the given geometric dimension \(w = \frac{d}{4}\):
\[
A_{\text{shear}} = \left(\frac{d}{4}\right) \cdot l = \frac{l \cdot d}{4}
\]
Step 2: Calculating the average shear stress (\(\tau\)).
The average shear stress developed within the key is defined as the total tangential force divided by the resisting shear area:
\[
\tau = \frac{F}{A_{\text{shear}}}
\]
Substitute the expressions for \(F\) and \(A_{\text{shear}}\) into this formula:
\[
\tau = \frac{\left(\frac{2T}{d}\right)}{\left(\frac{l \cdot d}{4}\right)}
\]
Step 3: Simplifying the algebraic expression.
To simplify this fraction, we multiply the numerator by the reciprocal of the denominator:
\[
\tau = \frac{2T}{d} \times \frac{4}{l \cdot d} = \frac{2 \times 4 \times T}{l \cdot d \cdot d} = \frac{8T}{l \cdot d^2}
\]
The derived average shear stress matches Option (3).