Concept:
Delta-to-Wye (\(\Delta\)-to-\(Y\)) transformation allows us to convert three resistors connected in a closed loop delta configuration into an equivalent star/wye network connected to a central common node.
The general conversion formula for finding a resistor connected to a specific terminal node in the Wye network is given by:
\[
R_{\text{node}} = \frac{\text{Product of the two adjacent Delta resistors sharing that node}}{\text{Sum of all three Delta resistors}}
\]
For node \(a\), the two adjacent delta branches that share this vertex are \(R_{ab}\) and \(R_{ca}\). Therefore, the expression for \(R_a\) is:
\[
R_a = \frac{R_{ab} \times R_{ca}}{R_{ab} + R_{bc} + R_{ca}}
\]
Step 1: Extracting given values and computing the total denominator sum.
We are given the individual values of the delta network branches:
• \(R_{ab} = 10\ \Omega\)
• \(R_{bc} = 20\ \Omega\)
• \(R_{ca} = 30\ \Omega\)
Let us calculate the sum of all individual resistors in the delta loop:
\[
\text{Sum} = R_{ab} + R_{bc} + R_{ca} = 10 + 20 + 30 = 60\ \Omega
\]
Step 2: Applying the Delta-Wye transformation formula to calculate \(R_a\).
Substitute the relevant adjacent branch values and the total sum calculated above into the formula:
\[
R_a = \frac{10 \times 30}{60}
\]
Multiply the values in the numerator:
\[
10 \times 30 = 300
\]
Now substitute back and simplify the fraction:
\[
R_a = \frac{300}{60} = 5\ \Omega
\]
Hence, the value of the equivalent Wye resistor connected to node \(a\) is exactly \(5\ \Omega\). This directly corresponds to Option (C).