The aurorae are the result of collisions with the atmosphere of energe
tic particles that have their origin in the solar wind, and reach the
atmosphere after having undergone varying degrees of acceleration and
redistribution within the Earth's magnetosphere. The global scale phen
omenon represented by the aurorae therefore contains considerable info
rmation concerning the solar-terrestrial connection. For example, by c
orrectly measuring specific auroral emissions, and with the aid of com
prehensive models of the region, we can infer the total energy flux en
tering the atmosphere and the average energy of the particles causing
these emissions. Furthermore, from these auroral emissions we can dete
rmine the ionospheric conductances that are part of the closing of the
magnetospheric currents through the ionosphere, and from these we can
in turn obtain the electric potentials and convective patterns that a
re an essential element to our understanding of the global magnetosphe
re-ionosphere-thermosphere-mesosphere. Simultaneously acquired images
of the auroral oval and polar cap not only yield the temporal and spat
ial morphology from which we can infer activity indices, but in conjun
ction with simultaneous measurements made on spacecraft at other locat
ions within the magnetosphere, allow us to map the various parts of th
e oval back to their source regions in the magnetosphere. This paper d
escribes the Ultraviolet Imager for the Global Geospace Sciences porti
on of the International Solar-Terrestrial Physics program. The instrum
ent operates in the far ultraviolet (FUV) and is capable of imaging th
e auroral oval regardless of whether it is sunlit or in darkness. The
instrument has an 8 degrees circular field of view and is located on a
despun platform which permits simultaneous imaging of the entire oval
for at least 9 hours of every 18 hour orbit. The three mirror, unobsc
ured aperture, optical system (f/2.9) provides excellent imaging over
this full field of view, yielding a per pixel angular resolution of 0.
6 milliradians. Its FUV filters have been designed to allow accurate s
pectral separation of the features of interest, thus allowing quantita
tive interpretation of the images to provide the parameters mentioned
above. The system has been designed to provide ten orders of magnitude
blocking against longer wavelength (primarily visible) scattered sunl
ight, thus allowing the first imaging of key, spectrally resolved, FUV
diagnostic features in the fully sunlit midday aurorae. The intensifi
ed-CCD detector has a nominal frame rate of 37 s, and the fast optical
system has a noise equivalent signal within one frame of similar to 1
0 R. The instantaneous dynamic range is > 1000 and can be positioned w
ithin an overall gain range of 10(4), allowing measurement of both the
very weak polar cap emissions and the very bright aurora. The optical
surfaces have been designed to be sufficiently smooth to permit this
dynamic range to be utilized without the scattering of light from brig
ht features into the weaker features. Finally, the data product can on
ly be as good as the degree to which the instrument performance is cha
racterized and calibrated. In the VUV, calibration of an an imager int
ended for quantitative studies is a task requiring some pioneering met
hods, but it is now possible to calibrate such an instrument over its
focal plane to an accuracy of +/-10%. In summary, very recent advances
in optical, filter and detector technology have been exploited to pro
duce an auroral imager to meet the ISTP objectives.