magnetic dipole

In this case a substantial internal magnetic dipole moment is expected.

Which matches the expression of the force between two magnetic dipoles.

A magnetic dipole is a closed circulation of electric current.

The magnetic dipoles of the atoms point in random directions.

The effect is caused by the non-concentricity of the Earth and its magnetic dipole.

The second order arises due to the mutual interaction of the magnetic dipoles.

So the nuclear magnetic dipole momentum is much smaller than that of the whole atom.

It is defined as the net magnetic dipole moment per unit volume of that region.

This small difference was later called anomalous magnetic dipole moment of the electron.

It is the magnetic dipole rotational transitions that are observed.

Such material has magnetic dipoles that, when adjacent, prefer to point in opposite directions.

The reason for the low upper limit on the internal magnetic dipole moment is not properly understood.

The magnetic field of a magnetic dipole is depicted in the figure.

This pole model is also called the Gilbert model of a magnetic dipole.

An example of a magnetic dipole moment occurring is in a wire loop with flowing current.

Antihydrogen has, like many atoms and especially hydrogen, a small magnetic dipole moment.

From experience working the ore buckets, she knew the feel of locked-in magnetic dipoles.

There is an energy associated with a magnetic dipole moment in the presence of a magnetic field.

Magnetic dipoles - for example, a bar magnet - align in a particular direction relative to the earth.

In addition to current loops, the electron, among other fundamental particles, has a magnetic dipole moment.

R is an important input in the calculation of the anomalous magnetic dipole moment.

A magnetic dipole was placed on metamaterial (slab) ground plane.

The first case is a magnetic dipole of constant magnitude that has a fast (fixed) orientation.

The rotational structures of the bands are determined by magnetic dipole selection rules.

The same formulas are valid for 3Σ±–3Σ± magnetic dipole transitions.