Concept:
The axial elongation or deflection (\(\delta\)) of a closely coiled helical spring subjected to an axial force load \(W\) is derived using Castigliano's theorem or strain energy methods in torsion. The canonical formula for deflection is:
\[
\delta = \frac{8 W D^3 n}{G d^4}
\]
Where the independent parameters are defined as:
• \(W\) = Applied axial force load on the spring.
• \(D\) = Mean diameter of the spring coil.
• \(n\) = Number of active coils or turns in the spring helix.
• \(G\) = Shear modulus of elasticity (modulus of rigidity) of the material.
• \(d\) = Diameter of the spring wire.
Step 1: Extracting proportional relationships from the given conditions.
The problem specifies that the two springs, designated as 'A' and 'B', share several identical properties:
• Same material \(\Rightarrow G_A = G_B = G\)
• Same coil diameter \(\Rightarrow D_A = D_B = D\)
• Same wire diameter \(\Rightarrow d_A = d_B = d\)
• Subjected to same load \(\Rightarrow W_A = W_B = W\)
By grouping all constant parameters into a single proportionality constant \(K\):
\[
K = \frac{8 W D^3}{G d^4}
\]
We can express the deflection of any spring in this problem as a direct linear function of its number of active turns:
\[
\delta = K \cdot n \quad \Rightarrow \quad \delta \propto n
\]
Step 2: Setting up the deflection ratio.
Using our proportionality relationship, the ratio of the deflection of spring 'A' (\(\delta_A\)) to that of spring 'B' (\(\delta_B\)) simplifies to the ratio of their respective numbers of turns:
\[
\frac{\delta_A}{\delta_B} = \frac{n_A}{n_B}
\]
Step 3: Calculating the numerical ratio using the given turn condition.
The problem states that the number of turns of spring 'A' is exactly half that of spring 'B':
\[
n_A = \frac{1}{2} n_B \quad \Rightarrow \quad \frac{n_A}{n_B} = \frac{1}{2}
\]
Substituting this value into our ratio equation:
\[
\frac{\delta_A}{\delta_B} = \frac{1}{2}
\]
Thus, the ratio of the deflection of spring 'A' to spring 'B' is \(\frac{1}{2}\), matching Option (1).