Concept:
• Self-inductance firmly and mathematically measures a conductive coil's inherent natural ability to dynamically oppose any rapid, sudden changes in its internal flowing electrical current.
• Dimensional formulas elegantly and systematically break down complex, derived electromagnetic quantities strictly into their fundamental baseline mechanical and electrical base units.
• The induced electromotive force strictly links a coil's self-inductance mathematically with the precise time-rate of temporal current change occurring within it.
Step 1: Derive the Dimensional Formula for Self-Inductance
We start strongly and strategically from the well-known, foundational energy formula involving an energized inductor:
\[ U = \frac{1}{2} L I^2 \]
Here, $U$ physically represents the stored magnetic potential energy, $L$ critically represents the self-inductance, and $I$ rigidly represents the operating current.
We strategically and algebraically rearrange this specific formula to clearly isolate the self-inductance variable on one side:
\[ L = \frac{2U}{I^2} \]
Since the numerical mathematical constant $2$ is completely dimensionless, the final physical dimension of $L$ entirely depends strictly on the fundamental physical dimensions of energy and current.
The universally accepted, standard dimensional formula for standard energy (equivalent to Work) is $[ML^2T^{-2}]$.
The firmly established standard dimensional formula for foundational electrical current is inherently $[A]$.
Substituting these specific reliable base dimensions smoothly and carefully into the algebraically rearranged equation yields:
\[ [L] = \frac{[ML^2T^{-2}]}{[A^2]} \]
Moving the current dimension cleanly into the upper numerator gives the final expression:
\[ [L] = [ML^2T^{-2}A^{-2}] \]
Step 2: Identify Parameters for Numerical Calculation
The initial electrical current strongly flowing in the coil is strictly recorded as $I_1 = 8.0 \text{ A}$.
The drastically and rapidly reduced final current is firmly recorded as $I_2 = 2.0 \text{ A}$.
The exact time interval over which this rapid, dynamic change thoroughly occurs is given as $\Delta t = 0.6 \text{ s}$.
The absolute average magnitude of the opposing induced electromotive force securely registered during this event is $|e| = 50 \text{ V}$.
Step 3: Calculate the Exact Self-Inductance
The primary governing mathematical formula firmly connecting all these dynamic variables is famously given by Faraday's and Lenz's laws combined together:
\[ |e| = L \left| \frac{\Delta I}{\Delta t} \right| \]
We mathematically and carefully determine the absolute magnitude of the rapid change in the operating current:
\[ |\Delta I| = |I_2 - I_1| = |2.0 - 8.0| = |-6.0| = 6.0 \text{ A} \]
Now, we meticulously substitute all the carefully collected and verified numerical values squarely back into the primary algebraic formula:
\[ 50 = L \times \left( \frac{6.0}{0.6} \right) \]
Calculating the simple internal mathematical fraction cleanly provides a very neat factor of exactly ten:
\[ 50 = L \times 10 \]
Isolating the self-inductance variable firmly by performing basic division elegantly yields the final answer:
\[ L = \frac{50}{10} = 5 \text{ H} \]
The total self-inductance of the rigorously tested induction coil is precisely evaluated to be strictly 5 Henrys.