Concept:
Self-inductance (\(L\)) is a measure of a coil's resistance to changes in electric current. It acts as electrical inertia.
• Induced Emf Formula: The average magnitude of the electromotive force induced in an inductive system depends on the self-inductance and the average rate of change of current:
\[
\varepsilon = -L \frac{\Delta I}{\Delta t} \quad \Rightarrow \quad |\varepsilon| = L \left| \frac{\Delta I}{\Delta t} \right|
\]
Where \(\Delta I = I_{\text{final}} - I_{\text{initial}}\) is the net difference in current amplitude, and \(\Delta t\) is the specific duration of the time interval.
• Dimensional Analysis: We can determine the dimensions of \(L\) by isolating it from the energy stored in an inductor:
\[
U = \frac{1}{2} L I^2 \quad \Rightarrow \quad L = \frac{2U}{I^2}
\]
Since energy (\(U\)) has dimensions of work done, and current (\(I\)) has basic fundamental dimensions of Amperes (\(A\)), we can evaluate the dimensional structure.
Step 1: Deriving the Dimensional Formula of Self-Inductance (\(L\)).
Let us use the fundamental definition relating magnetic energy stored in an inductor:
\[
\text{Energy } (U) = \frac{1}{2} L I^2
\]
Isolating the self-inductance term:
\[
L = \frac{2U}{I^2}
\]
Now, substituting the standard dimensional formulas for each constituent parameter:
• Dimensional formula of Potential/Kinetic Energy or Work Done:
\[
[U] = [Work] = [Force \times Displacement] = [M^1 L^1 T^{-2} \times L^1] = [M^1 L^2 T^{-2}]
\]
• Dimensional formula of Electric Current:
\[
[I] = [A^1] \quad \Rightarrow \quad [I^2] = [A^2]
\]
Combining these base units together in the expression for \(L\):
\[
[L] = \frac{[M^1 L^2 T^{-2}]}{[A^2]} = [M^1 L^2 T^{-2} A^{-2}]
\]
Answer Part 1: The dimensional formula for self-inductance is \([M^1 L^2 T^{-2} A^{-2}]\).
Step 2: Extracting numerical data from the text for the mathematical problem.
From the problem statement, we have the following values:
• Initial value of current, \(I_1 = 8.0 \, \text{A}\)
• Final value of current, \(I_2 = 2.0 \, \text{A}\)
• Continuous time interval, \(\Delta t = 0.6 \, \text{s}\)
• Average induced electromotive force amplitude, \(\varepsilon = 50 \, \text{V}\)
Step 3: Calculate the change in current (\(\Delta I\)) and the self-inductance \(L\).
The net change in current traversing the coil is:
\[
\Delta I = I_2 - I_1 = 2.0 \, \text{A} - 8.0 \, \text{A} = -6.0 \, \text{A}
\]
Now, utilizing Faraday's self-induction formula to relate the given values:
\[
\varepsilon = -L \frac{\Delta I}{\Delta t}
\]
Substitute the values into the equation:
\[
50 = -L \left( \frac{-6.0}{0.6} \right)
\]
Simplifying the terms within the parentheses:
\[
\frac{-6.0}{0.6} = -10
\]
Substitute this back into the relation:
\[
50 = -L \times (-10)
\]
\[
50 = 10L
\]
Isolating the variable \(L\) by dividing both sides by 10:
\[
L = \frac{50}{10} = 5 \, \text{H}
\]
The SI unit for self-inductance is the Henry (H).
Answer Part 2: The self-inductance of the given coil is \(5 \, \text{H}\) (Henries).