Protons, neutrons, and electrons have **mass**.

m_{p} = 1.673*10^{-27} kg, m_{n} =1.675*10^{-27}
kg, m_{e} = 9.109*10^{-31} kg.

Massive particles produce gravitational fields and are acted on by gravitational fields. (Massive particles attract each other.)

A field is a way of explaining action at a distance. The magnitude of
the **gravitational field** produced by a massive
object at a point P is the force per
unit mass it exerts on another massive object located at that point. The
direction of the gravitational field is the direction of that force.

The magnitude of the gravitational force near the surface of Earth is F = mg, the gravitational field has magnitude F/m = g. Its direction is downward.

Protons and electrons have **charge**.

q_{p} = 1.602*10^{-19} C, q_{e} = -1.602*10^{-19} C.

Charged particle produce electric fields and are acted on by electric fields. (Charged particles attract or repel each other.)

The magnitude of the **electric field** **E** produced by a charged particle at a point P
is the **force per unit positive charge** it exerts on another charged particle located at
that point. The direction of the electric field is the direction of that
force on a positive charge. The actual force on a particle with charge
q is given by **F** = q**E**.

Electric field of a positive charge. A positive test charge is repelled. |
Electric field of a negative charge. A positive test charge is attracted. |

The magnitude of the electric field **E**
at a point P is inversely proportional to the square of the radial distance of the
point P away from the charge.

Moving charged particles also produce **magnetic fields** and are acted on by
magnetic fields. Currents are moving charges and produce magnetic fields.
Permanent magnets are the result of magnetization currents flowing inside
the material.
For a current flowing in a long straight wire,
the magnitude of the magnetic field **B** at a point P is inversely proportional to
the radial distance of the point P away from the wire. **B** encircles the
wire. The direction of **B** is given by the right-hand rule.

The picture below shows an iron-filing pattern, which reveals the nature of the magnetic field surrounding a current-carrying wire.

The magnetic field **B** produced by a current flowing in a coil is shown
below.

The direction of the field inside the coil is given by the right-hand rule. Curl the fingers of your right hand in the direction that the current flows in the solenoid. Your thumb points in the direction of

The magnetic field outside the coil resembles that of a permanent bar magnet shown below and the coil is called an electromagnet.

Magnetic fields are produced by currents. Permanent magnets are the result of "magnetization currents" flowing inside the material. Macroscopically, permanent magnets act like current loops. The internal currents of the electrons produce a net magnetization current flowing along the surface of the material. (In the interior of the material currents flowing in opposite directions produce zero net current.)

A small current loop also produces a magnetic field. The field-line pattern
is that of a small button magnet. We say that the loop has a magnetic moment
**μ **= IA**n**. Here I is the current
flowing in the loop, A is the area of the loop, and **n** is a unit vector
perpendicular to the area. The direction **n** of the magnetic moment is again defined by the right-hand rule.
Curl the fingers of your right hand in the direction that the current flows.
Your thumb points in the direction of **n**.
The magnetic field
lines of a loop with dipole moment **μ** are shown
below. The field-line pattern is that of a small magnet. We say that
**μ** points from the
**south pole** to the **north
pole** of the magnet. (Magnetic field lines therefore exit a
magnet at the north pole and enter at the south pole.)

The picture below shows the field pattern in a plane perpendicular to the loop, revealed with iron filings.

The magnetic field is a
**vector**. Magnetic fields produced by different currents sources can enhance each
other or cancel out.

Magnetic fields exert forces on other moving charge. The force a magnetic
field exerts on a charge q moving with velocity **v** is called the **
Lorentz force**. It is given by

**F **= q**v**×**B**.

The force **F** is perpendicular to the direction of the magnetic field **
B**. It also is perpendicular to the direction of the velocity **v**. **
F** is perpendicular to the plane that contains both **v** and **B**.
The magnitude of **F** is F = qvBsinθ, where
θ is the smallest angle between the directions of the
vectors **v** and **B**. If **v** and **B** are parallel or
anti-parallel to each other, then **v**×**B **=
0 and **F **= 0, since sinθ = 0. If **v** and
**B** are perpendicular to each other, then sinθ =
1 and **F** has its maximum possible magnitude F = qvB.

In an external magnetic field a magnetic moment (a current loop or a magnet) can experience a force and a torque.

The **torque**
**τ **= **μ **×** B**
tries to align the magnetic moment with the magnetic field.
Its magnitude is **
**τ = μBsinθ,
where θ is the smallest angle between the directions
of the vectors **μ** and **B**. The
torque is zero when **μ** and **B** are parallel or anti-parallel to each
other.

The **force** tries
to pull an aligned dipole into regions where the magnitude of the magnetic field
is larger and push an anti-aligned dipole into regions where magnitude the
magnetic field is smaller.

If the magnetic field is pointing into the z-direction, the force on a magnetic dipole in that field is given by

F_{z} = μ_{z}dB_{z}/dz.

Here μ_{z} =
μ cosθ
is the z-component of the magnetic moment.

If B is constant, then dB_{z}/dz
= 0 and there is no force. In an inhomogeneous field where dB_{z}/dz is
not zero, the magnetic dipole experiences a force in the z-direction, unless θ = 90^{o}
and μ_{z}=
0. Since
for a classical current loop **μ** can point into any direction the force F_{z} can
have any value from -μdB_{z}/dz to +μdB_{z}/dz.

If we passed a beam of magnetic dipoles, which were randomly oriented and could not change their orientation during the passage, through an inhomogeneous magnetic field, different dipoles would be deflected by different amounts.

**Permanent magnets**

Magnetic fields are produced by currents. Permanent magnets are the result
of magnetization currents flowing inside the material. We may expect that electrons
in atoms can
have a magnetic moment similar to the magnetic moment of tiny current loops,
since they have angular momentum, and angular momentum is usually associated
with orbits. It has been experimentally verified that if electrons in atoms have angular momentum **L**, then they have a magnetic
moment **μ **that is proportional to **L**,
**μ **=
γ**L**, with
γ
= -|q_{e}|/(2m_{e}) a
constant of proportionality. Since the orbital angular
momentum is quantized, so is the magnetic moment due to orbital angular momentum. The
orbital angular momentum of
many electrons with orbital angular momentum **L**_{1}, **L**_{2}, **L**_{3}, ... adds up to
yield the total angular momentum **
L** = **L**_{1} + **L**_{2} + **L**_{3} + ...
, and the total magnetic moment **μ** due to the
total orbital angular momentum is proportional to
**L**.

In 1915 Einstein and the Dutch
physicist de Haas carried out an experiment to show the** link between the angular
momentum of atoms and their magnetic moments**. Einstein and de Haas suspended an
iron cylinder from a thin fiber inside a coil, where one measures an
approximately uniform magnetic field when a current is flowing. Initially
no current is flowing, and the magnetic moments of the individual atoms
of the cylinder are randomly oriented, and the cylinder has no net magnetic
moment. However, when a current is switched on, the
magnetic field **B** will exert a torque on the magnetic moments **μ** of
the individual atoms, and they will line up parallel to the magnetic field. If the
angular momentum **L** of each atom is proportional to **μ**, then this alignment of the
atomic magnetic moments must cause an alignment of the atomic angular momenta,
anti-parallel to the magnetic field **B** because the proportional constant
γ is negative.

But angular momentum about an axis is conserved if no external torque about that
axis is present. The total angular momentum **L**_{tot} about
the direction of the magnetic field remains zero because no external torque
about that direction acts on the cylinder. When **B** is
turned on, the atomic angular momenta line up anti-parallel to **B**. So for
the total angular momentum to the remain zero, the
cylinder starts to rotate around its central axis with the angular momentum of the cylinder parallel to **B**.

Einstein was a great theoretician, but this was the only experiment he ever published.

The possible values that we can measure for the
square of the magnitude of the orbital angular momentum are L^{2} =
l(l+1)ħ^{2}.
The possible projections we can measure along any axis, for example the z-axis,
are L_{z} = mħ.
Here
l is an integer,
l = 0, 1, 2, ... , and for a given l, m can take on
values from -l to
l in integer steps. Since L_{z} is quantized, μ_{z} is
quantized, μ_{z}
= -|q_{e}|mħ/(2m_{e})
= -μ_{B}m.
Here μ_{B}
= |q_{e}|ħ/(2m_{e})
is called the **Bohr magneton**. If we passed a beam of randomly
oriented atoms with orbital angular momentum **L** through an inhomogeneous magnetic field,
we would expect different atoms to be deflected by different amounts depending
on the value of μ_{z}.

F_{z} = μ_{z}dB_{z}/dz.

Since L_{z} can take on 2l + 1 different values,
μ_{z}
can take on 2l
+ 1 different values, and we expect 2l
+ 1 different deflection
angles. Note that 2l + 1 is always an odd integer.

**The Stern-Gerlach experiment**

In 1921, Otto Stern and Walter Gerlach performed such an experiment. The actual experiment was carried out with a beam of neutral silver atoms from a hot oven because silver atoms could be readily detected using a photographic emulsion.

A beam of silver atoms emerges from a furnace held at 1000 K. It is
collimated using 0.1 mm slits, passed between the poles of a magnet, and directed
onto a screen, where the atoms are detected.
The speed of the silver
atoms is approximately 500 m/s (from (3/2)kT = (1/2)mv^{2}, k = 1.38*10^{-23 }J/K). In the experiment the silver atoms hit the screen in two distinct spots. The
measurement yields only two possible values for μ_{z}.

What is going on?

If the magnetic moment of a silver atom was due to the orbital angular
momentum of the electrons, an odd number of spots would have to be measured.
However, as we will see in the next module, electrons in silver atoms in their
ground state have no net orbital angular momentum. The magnetic moment of
a silver atoms is not due to the orbital angular momentum of its electrons, but
due to the **spin** of one electron.