Concept:
• The visible brightness or visual glow of a standard resistive light bulb is strictly determined by the real power seamlessly dissipated across its internal filament, heavily dependent on the RMS current ($P = I_{rms}^2 R$).
• In a practical series AC circuit containing resistance and inductance, the driving operating current is meticulously governed by the total circuit impedance.
• The total impedance mathematically adjusts based on the inductive reactance, which is fiercely dependent on the physical inductance of the inserted coil.
Step 1: Understand the Initial State
The total electrical impedance $Z$ of the operating series circuit is robustly formulated as $Z = \sqrt{R_{bulb}^2 + X_L^2}$, where $X_L = \omega L$ physically represents the inductive reactance.
Initially, the inductor is an open air-core coil, meaning it has a relatively low baseline self-inductance $L_0$, dictated largely by the magnetic permeability of free space $\mu_0$.
The circuit draws a specific steady RMS current strictly based on this baseline impedance, causing the bulb to visibly glow with a certain stable brightness.
Step 2: Analyze the Effect of Inserting the Iron Bar
When a highly permeable soft iron bar is deliberately and deeply inserted inside the open coil, it forcibly completely replaces the air core with an iron core.
Soft iron intrinsically possesses a magnetic permeability ($\mu$) that is thousands of times significantly higher than that of empty air.
Because the physical self-inductance $L$ of a coil is mathematically strictly proportional to the permeability of its core material ($L \propto \mu$), introducing the iron bar drastically increases the fundamental self-inductance $L$ of the inductor coil.
As the self-inductance $L$ surges heavily upward, the inductive reactance $X_L$ proportionately and aggressively spikes up.
Step 3: Conclude the Effect on Bulb Brightness
Consequently, due to the massively inflated inductive reactance, the overall total impedance $Z$ of the entire series circuit substantially and noticeably increases.
Because the applied driving AC voltage source is held securely constant by definition of the problem, a much higher total impedance actively chokes the flow of electrons, strictly decreasing the operational RMS current $I_{rms}$ flowing continuously through the interconnected bulb.
With a noticeably reduced driving current, the actual thermal power actively dissipated by the glowing bulb ($P = I_{rms}^2 R_{bulb}$) heavily drops.
Since power strictly dictates brightness, the visual glow of the light bulb will dramatically and visibly decrease.