Step 1: Understanding the Question:
We need to determine how the inductive reactance ($X_L$) of an ideal inductor responds when the fundamental frequency ($f$) of the connected alternating current source increases.
Step 2: Key Formula or Approach:
The inductive reactance ($X_L$) represents the opposition that an inductor offers to an alternating current. It is mathematically defined by the formula:
$$X_L = \omega L = 2\pi f L$$
where $\omega$ is the angular frequency, $f$ is the cyclic frequency, and $L$ is the self-inductance of the component.
Step 3: Detailed Explanation:
Let's analyze the mathematical relationship from the inductive reactance equation:
$$X_L = (2\pi L) \cdot f$$
Since the self-inductance $L$ of a given coil is a fixed structural constant, the entire term $(2\pi L)$ behaves as a constant multiplier. This means that inductive reactance is directly proportional to the supply frequency:
$$X_L \propto f$$
Because of this linear relationship, any increase in the supply frequency $f$ causes a proportional, linear increase in the inductive reactance $X_L$.
Step 4: Final Answer:
The inductive reactance increases because it is directly proportional to the frequency, matching option (B).