General Physics II - Chapter 21: Magnetic Forces and Magnetic Fields
Magnetic Fields
Magnetism was first discovered in Magnesia, Asia Minor, where rocks could attract each other and were called “magnets.”
Magnets have two poles: North and South. The magnetic effect is strongest at the poles.
Similar poles repel each other, while opposite poles attract.
Magnetic Fields Visualization
Similar to electric fields, magnetic fields can be visualized surrounding a magnet.
The direction of the magnetic field is the direction a compass needle's north pole would point.
A compass needle is a bar magnet supported at its center that can rotate freely.
Magnetic field lines continue inside the magnet.
The magnetic field (\vec{B}) is a vector quantity measured in Tesla (T).
Magnetic Monopoles
Cutting a bar magnet in half results in two new magnets, not isolated poles.
Physicists have searched for single magnetic poles (monopoles), but none have been found.
Earth’s Magnetic Field
The north pole (N) of a compass needle points to the Earth’s north geographic pole, where the Earth’s south magnetic pole is located.
Earth's magnetic poles do not align with its geographic poles.
Magnetic declination is the angular difference between a compass needle's direction and true north (varies from 0° to about 20°).
Earth’s magnetic field is thought to be produced by electric currents in the Earth’s molten iron outer core.
Electric Currents and Magnetic Fields
Hans Oersted (1777–1851) discovered that a compass needle deflects when placed near a wire carrying an electric current (\vec{I}). The magnetic field lines produced by the current in a straight wire are circles centered on the wire.
Right-hand rule (1) determines the magnetic field direction:
Grasp the wire with your right hand, thumb pointing in the current direction.
Your fingers encircle the wire in the direction of the magnetic field.
Symbol ⨀ represents current pointing toward you (out of the page).
Symbol ⨂ represents current pointing away from you (into the page).
Magnetic Field of a Straight Wire
The magnetic field (\vec{B}) due to the current in a long straight wire is directly proportional to the current (\vec{I}) and inversely proportional to the distance (\vec{r}) from the wire:
B \propto \frac{I}{r}The proportionality constant is \frac{\mu0}{2\pi}, where \mu0 is the permeability of free space (\mu_0 = 4\pi \times 10^{-7} T⋅m/A).
The magnetic field magnitude is given by:
B = \frac{\mu_0 I}{2\pi r}
Magnetic Field of a Wire Loop
The magnetic field produced by a current in a wire loop at the loop center (\vec{P}) is given by:
B = \frac{\mu_0 I}{2R}
Where R is the loop radius and I is the current.
Magnetic Force on an Electric Current
Magnets exert a force on current-carrying wires.
For a straight wire placed in a magnetic field (\vec{B}), the force direction is perpendicular to both the current and the magnetic field.
Right-hand rule (2): Orient your right hand in the current direction (\vec{I}), bend fingers toward magnetic field lines (\vec{B}). Your thumb points toward the force on the wire.
Magnitude of the force is:
F_B = I\ell B \sin(\theta)
Where I is the current, B is the magnetic field, \ell is the wire length, and \theta is the angle between the current and magnetic field directions.If I and B are perpendicular, then FB = I\ell B, and if parallel, then FB = 0.
SI unit of magnetic field B is Tesla (T): 1 T = 1 N/(A⋅m).
The cgs unit for magnetic field is the gauss (G): 1 G = 10^{-4} T.
Force Between Two Parallel Wires
Two long parallel wires separated by distance d, carrying currents I1 and I2, exert a force on each other.
Each current produces a magnetic field
Equations, Physical Quantities, and Units
Equation | Physical Quantities & Units | Scalar/Vector |
|---|---|---|
B = \frac{\mu_0 I}{2\pi r} | B (Magnetic Field, Tesla (T)), I (Current, Ampere (A)), r (distance, meters (m)), \mu_0 (Permeability of Free Space, T⋅m/A) | B: Vector |
B = \frac{\mu_0 I}{2R} | B (Magnetic Field, Tesla (T)), I (Current, Ampere (A)), R (Loop Radius, meters (m)), \mu_0 (Permeability of Free Space, T⋅m/A) | B: Vector |
F_B = I\ell B \sin(\theta) | F_B (Magnetic Force, Newtons (N)), I (Current, Ampere (A)), \ell (Wire Length, meters (m)), B (Magnetic Field, Tesla (T)), \theta (Angle, radians) | F_B: Vector |