Self-inductance does not directly depend on the current flowing through a coil. Instead, it depends on physical properties such as:
- **Number of turns (N):** The more turns the coil has, the greater the inductance.
- **Core material permeability (μ):** Materials with higher magnetic permeability (like iron) increase inductance compared to air or vacuum.
- **Cross-sectional area (A) of the coil:** Larger areas result in higher inductance.
- **Length (l) of the coil:** Longer coils have lower inductance for the same number of turns.
However, the **induced EMF (electromotive force)**, which opposes changes in current due to self-inductance, depends on the rate of change of current (di/dt). This is captured by Faraday’s Law:
\[
\text{EMF} = -L \frac{di}{dt}
\]
Where \( L \) is the inductance, and \( \frac{di}{dt} \) is the rate of change of current.
So, while inductance \( L \) is a fixed property of the coil's design and materials, the effect of self-inductance (in terms of induced voltage) becomes more prominent when there are rapid changes in current.
In practical terms:
- For **small or constant currents**, self-inductance doesn’t produce significant effects.
- For **changing currents**, the opposition (induced voltage) increases with faster changes.