A solenoid is a long coil of wire wound in a tight, regular pattern. When electric current flows through it, it behaves like a magnet.
Think of it as a magnetic battery that can create a strong, uniform field inside its core.
The magnetic field inside an ideal solenoid is given by the formula:
\$B = \mu_0 n I\$
🔌 The more turns or the higher the current, the stronger the field.
When you insert a ferromagnetic material (like iron) into the solenoid, the field increases because the material becomes magnetised and adds its own field.
The new field is:
\$B{\text{core}} = \mu0 \mu_r n I\$
🧲 Analogy: Imagine the core as a set of tiny magnets that line up with the solenoid’s field, boosting it like a team of friends pushing together.
Take a common iron nail and wrap a coil of wire around it. When you pass a current through the coil:
Result: The magnetic field inside the coil is much stronger than with air alone.
⚡️ Practical tip: This principle is used in transformers and electric motors.
Remember:
💡 Illustrate with a simple diagram or a short paragraph if the exam allows.
| Scenario | \$B\$ (T) | Explanation |
|---|---|---|
| Air core, \$n=1000\,\text{turns/m}\$, \$I=2\,\text{A}\$ | \$B = \mu_0 n I \approx 0.0025\,\text{T}\$ | Baseline field. |
| Iron core, \$\mu_r=200\$, same \$n\$ and \$I\$ | \$B{\text{core}} = \mu0 \mu_r n I \approx 0.5\,\text{T}\$ | Core amplifies field by factor \$\mu_r\$. |