Magnetic field cycling in nuclear magnetic resonance (NMR) experiments has
been used since the early days of NMR. Originally such time-dependent magne
tic field experiments were motivated to study cross relaxation, spin system
thermodynamics and indirect detection of quadrupolar resonance. The first
apparatus used mechanical or pneumatic systems to shoot the sample between
two magnets, the typical "flying time" being a few hundreds of milliseconds
. As a natural evolution of the experimental technique and the need to exte
nd its application to samples with higher relaxation rates, faster magnetic
field switching devices were developed during the last years. Special elec
tric networks combined with sophisticated air core magnets allowed one to s
witch magnetic fields between zero and fields of the order of 0.5 T in a fe
w milliseconds. Today we refer to this new generation of instruments as "fa
st-field-cycling" devices. The technique has been successfully used during
the last years to obtain information on the molecular dynamics and order in
different materials, ranging from organic solids, metals, polymers, liquid
crystals, porous media to biological systems. At present it is also turnin
g to be an important tool for the design of contrast agents for magnetic re
sonance imaging. Fast field cycling was mainly oriented to T, relaxometry a
s a unique technique offering a dynamic window of several decades, ranging
from few kilohertz to several megahertz. However, there exist less conventi
onal applications of the technique that can also provide relevant informati
on concerning molecular dynamics, structure and molecular order. In this ar
ticle we will briefly deal with basic aspects of the technique, its evoluti
on, present-day relevant applications and the last improvements concerning
specialized instrumentation.