JCMT - Secondary Mirror Unit, SMU
JCMT - Secondary Mirror information
The image below shows the secondary mirror (or "subreflector")
of the James Clerk Maxwell
Telescope and its support structure. The mirror is 60cm in diameter
and is supported on a carbon fiber tetrapod structure for thermal
stability. The mirror is hyperboloid in shape and has a surface
accuracy of a few microns (1 micron = 1/10000 cm).
The secondary mirror allows the JCMT to focus submillimeter radiation
onto detectors built into receivers mounted at the primary focus in
the receiver cabin (located below the main mirror) and at the two
Nasmyth foci (located on the elevation axis).
Aside from providing focal adjustments for the JCMT, the secondary
mirror provides the means for eliminating the majority of sky
brightness variations originating from the Earth's atmosphere. This is
accomplished by vibrating ("chopping" or "nutating")
the mirror such that the difference signal
between two nearby points on the sky is obtained; since nearby points
contain the same contribution from the atmosphere, to a large degree
the difference represents the signal from a celestial target in one of
the two beam positions. Common chop distances are 60 or 120 arcsec, and
typical rates are 1.0 Hz for spectral line observations and 7.8125 Hz
for broadband continuum astronomy.
The carbon fiber tetrapod support contributes 6% to the telescope
spillover losses. The secondary has a shallow cone in the centre -
covering the area that corresponds to the shadow of the secondary on the
main dish - that prevents radiation being reflected back into the cabin
and causing standing waves. It doesn't eliminate all ground pickup, though.
SMU Task
Other documents concerning the SMU
Fault recovery suggestions (Feb 2002)
Reports on occasional issues (newest at top)
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