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Magnetism

Manual: General · Subject: Magnetism

Investigate magnetic poles and field lines, Earth's magnetosphere, the right-hand rule for electromagnets, and the force on a current-carrying wire (F = BIL) with real-world applications.

Section

Magnetic Poles and Field Lines

Every magnet has two inseparable poles — a north (N) pole and a south (S) pole. Magnetic interactions follow a single fundamental rule:

  • Like poles repel (N–N or S–S push apart).
  • Unlike poles attract (N–S pull together).

No experiment has ever isolated a single magnetic pole (monopole); poles always exist in equal-and-opposite pairs — even when a magnet is broken in half, each fragment has its own north and south pole.

Magnetic field lines provide a visual map of a magnetic field's direction and strength:

  • By convention, lines emerge from the north pole and enter the south pole.
  • Closely packed lines indicate a strong field; widely spaced lines indicate a weak field.
  • Field lines never cross one another.
Earth's Magnetosphere

Earth generates a global magnetic field through convective motion of liquid iron in its outer core, behaving effectively like an enormous bar magnet. This field extends far into space, forming the magnetosphere — a teardrop-shaped cavity compressed on the sun-facing side and drawn out into a long magnetotail on the night side.

The magnetosphere acts as a planetary shield, deflecting the solar wind — a continuous stream of high-energy charged particles (mainly protons and electrons) ejected from the Sun at hundreds of kilometres per second. Without this shield, the solar wind would gradually erode Earth's atmosphere, as happened to Mars after its internal magnetic field collapsed billions of years ago. Charged particles that do enter along field lines near the poles produce the spectacular aurora borealis and aurora australis.

Electromagnets and the Right-Hand Rule

A wire carrying an electric current is surrounded by a magnetic field that forms concentric circular rings centred on the wire. The direction of this field is determined by the right-hand rule:

> Point the right thumb in the direction of conventional current flow (positive → negative); the curled fingers indicate the direction the magnetic field circles around the wire.

Winding the wire into a solenoid (a multi-turn helical coil) causes the individual field contributions of each loop to reinforce each other. Inside the solenoid the resulting field is strong and uniform, closely resembling that of a bar magnet with clearly defined north and south poles at its ends.

An electromagnet inserts a soft-iron core inside the solenoid:

  • Soft iron has very high magnetic permeability, strongly concentrating and amplifying the magnetic flux density inside the coil.
  • The magnetic field can be switched on and off by controlling the current.
  • Field strength is adjustable by varying the current magnitude or the number of coil turns.

Electromagnets are found in electric bells, relay switches, lifting cranes, loudspeakers, MRI scanners, and electric motors.

🔑

Right-hand rule for a solenoid: Curl the fingers of the right hand around the coil so they point in the direction of conventional current flow through the windings. The outstretched thumb points toward the north pole of the resulting electromagnet.

Force on a Current-Carrying Wire and Applications

A straight wire carrying current within an external magnetic field experiences a mechanical force. This force arises because the wire's own magnetic field interacts with the external one. Its magnitude is:

F=BILF = BIL

where:

  • FF — force on the wire (newtons, N)
  • BB — magnetic flux density of the external field (teslas, T)
  • II — current through the wire (amperes, A)
  • LL — length of wire inside the field (metres, m)

The force is maximum when the wire is perpendicular to the field and zero when it runs parallel to the field. The direction of the force is given by Fleming's left-hand rule: hold the left hand with the First finger (Field direction), seCond finger (Current direction), and thuMb (Motion/Force direction) all mutually perpendicular.

Worked example: A 0.30 m0.30\ \text{m} wire carries a current of 6.0 A6.0\ \text{A} perpendicular to a field of B=0.50 TB = 0.50\ \text{T}:

F=BIL=0.50×6.0×0.30=0.90 NF = BIL = 0.50 \times 6.0 \times 0.30 = 0.90\ \text{N}

Real-World Applications:

| Technology | How F=BILF = BIL is used |<br>|---|---|<br>| Electric motors | Current in a rotating coil experiences opposing forces on each side, producing continuous rotation |<br>| MRI scanners | Superconducting electromagnets create powerful, stable fields for high-resolution body imaging |<br>| Maglev trains | Electromagnetic repulsion and attraction levitate and propel the train without mechanical contact, eliminating friction |<br>| Loudspeakers | Varying current through a voice coil generates proportional forces that vibrate a paper cone, producing sound |

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