Describe the effect on the magnetic field around straight wires and solenoids of changing the magnitude and direction of the current

4.5.3 Magnetic Effect of a Current

Straight Wires

Think of an electric current as a stream of tiny charged “water” particles flowing through a wire. Just like a river creates swirling eddies around rocks, a current creates a magnetic field that circles the wire. The direction of the field depends on the direction of the current (right‑hand rule). The strength of the field is given by Ampère’s law:

\$B = \frac{\mu_0 I}{2\pi r}\$

Where \$I\$ is the current, \$r\$ is the distance from the wire, and \$\mu_0\$ is the magnetic constant.

  • ⚡️ Increasing the current (e.g., turning up a dimmer) makes the magnetic field stronger everywhere around the wire.
  • 🔁 Reversing the current flips the direction of the magnetic field lines (like turning a fan clockwise to counter‑clockwise).
  • 🌀 Changing the distance r from the wire reduces the field strength proportionally to \$1/r\$.

Exam Tip: When asked to sketch the field around a straight wire, remember the right‑hand rule: point your thumb along the current direction, and your fingers curl in the direction of the magnetic field.

Solenoids

A solenoid is a coil of wire that behaves like a long bar magnet when current flows through it. Inside the coil, the magnetic field lines are almost straight and parallel, giving a strong, uniform field. Outside, the field is weak and spreads out like a gentle breeze.

The magnetic field inside a long solenoid is:

\$B = \mu_0 n I\$

Where \$n\$ is the number of turns per unit length and \$I\$ is the current.

  • 🔄 Increasing the current I increases the field linearly.
  • 🔁 Reversing the current flips the north and south poles of the solenoid.
  • 📈 Adding more turns (higher n) also strengthens the field.

ParameterEffect on B
Current \$I\$Directly proportional (↑I → ↑B)
Turn density \$n\$Directly proportional (↑n → ↑B)
Direction of IReverses field direction (north ↔ south)

Exam Tip: For a solenoid, remember that the field inside is uniform and given by \$B = \mu_0 n I\$. If the question asks about the field outside, note that it is much weaker and can be approximated as zero for a long solenoid.

Practical Example: The Electromagnet

Wrap a coil of wire around a nail (the core). When you connect a battery, the current creates a magnetic field that turns the nail into a magnet. Increase the battery voltage or add more turns, and the nail becomes a stronger magnet. Flip the battery leads, and the magnet’s north and south poles swap places. This is a classic demonstration of how changing the magnitude and direction of current controls magnetic fields.

Quick Check: If you double the current in a straight wire, by what factor does the magnetic field at a fixed distance change? (Answer: It doubles.)