M'kay, you probably have heard about the pencil-standing-on-end argument about symmetry. When the pencil is upright and balanced, the direction it will fall is unknown, but by symmetry it must be one of a possibly infinite number of directions. When it does fall the symmetry is broken.
Introduce a force to "restore" the symmetry (prosaically, lift the pencil back up onto its tip). Now you have to think about which symmetry is global, and which is local, and in respect of which fields.
Another common symmetry-breaking example is ferromagnetism. A bar of unmagnetized iron can point in any direction (let's place the bar inside an opaque sphere), but when it is magnetized the direction can be measured because of the magnetic field lines--the symmetry is broken. Spherical symmetry breaks when you identify a pair of antipodal points (because you have direction).
Introduce a force to "restore" the symmetry (prosaically, lift the pencil back up onto its tip). Now you have to think about which symmetry is global, and which is local, and in respect of which fields.
Another common symmetry-breaking example is ferromagnetism. A bar of unmagnetized iron can point in any direction (let's place the bar inside an opaque sphere), but when it is magnetized the direction can be measured because of the magnetic field lines--the symmetry is broken. Spherical symmetry breaks when you identify a pair of antipodal points (because you have direction).