Step 1: Understanding the Concept:
Resistors can be combined in different networks to achieve specific total values.
- In a series combination, the equivalent resistance is the sum of all parts: $R_s = R_1 + R_2 + \dots$ (the total is always larger than the largest single resistor).
- In a parallel combination, the inverse values add up: $\frac{1}{R_p} = \frac{1}{R_1} + \frac{1}{R_2} + \dots$ (the total is always smaller than the smallest single resistor).
- Mixed circuit combinations combine these two behaviors.
Step 2: Key Formula or Approach:
The target equivalent resistance is $R_{\text{eq}} = \frac{11}{5} \ \Omega = 2.2 \ \Omega$.
Let's analyze the limits to eliminate incorrect choices quickly:
- All series: $1 + 2 + 3 = 6 \ \Omega$ (Too large).
- All parallel: smaller than $1 \ \Omega$ (Too small).
This means we must test the mixed network options (C) and (D).
Step 3: Detailed Explanation:
Let's evaluate Option (D): 2 Ω and 3 Ω are connected in parallel, and this parallel pair is placed in series with the remaining 1 Ω resistor.
1. Calculate the parallel pair ($R_p$) for the 2 Ω and 3 Ω resistors:
\[ R_p = \frac{R_2 \times R_3}{R_2 + R_3} = \frac{2 \times 3}{2 + 3} = \frac{6}{5} \ \Omega = 1.2 \ \Omega \]
2. Add the 1 Ω series resistor to this parallel group:
\[ R_{\text{total}} = R_1 + R_p = 1 \ \Omega + \frac{6}{5} \ \Omega \]
\[ R_{\text{total}} = \frac{5 + 6}{5} = \frac{11}{5} \ \Omega = 2.2 \ \Omega \]
This configuration yields exactly the targeted value. Let's verify why Option (C) fails:
- Parallel pair of 1 Ω and 2 Ω: $R_p = \frac{1 \times 2}{1 + 2} = \frac{2}{3} \ \Omega$.
- Adding 3 Ω in series: $3 + \frac{2}{3} = \frac{11}{3} \ \Omega \neq \frac{11}{5} \ \Omega$.
Step 4: Final Answer:
The correct combination is achieved when 2 Ω and 3 Ω are combined in parallel and 1 Ω is placed in series with both.