QUESTION: How many different space phenomenon can the Hubble take pictures of? ANSWER from Dr. Louis Binder on May 20, 1996: The Hubble Telescope was designed to: * Investigate celestial bodies by studying their composition, physical characteristics, and dynamics. * Observe the formation of stars and galaxies, and study their formation and evolution. * Study the history and evolution of the universe. * Provide a long-term space-based research facility for opitcal astronomy. The scientific objectives will be acheived by research into: * Galaxies and Clusters - Extragalactic distances, star clusters, interacting galaxies, cosmological tests. * Interstellar Medium - Dust and extinction, supernovae remnants, planetary nebulae, star formation, circumstellar nebulosity. * Quasars and Active Galactic Nuclei - Quasi-stellar objects, Seyfert galaxies, BL Lac objects, radio galaxies, galacitc jets, gravitational lenses. * Stellar Astrophysics - Stellar Atmospheres and chemical composition, binary and variable stars, stellar photometry and polarimetry, parallaxes and proper motions of stars. * Stellar Populations - Color-magnitude and luminosity studies of star clusters,dynamics of clusters, structure of the galaxy and stellar surveys. * Solar System - Planetary features and atomspheres, satellites and rings, asteroids and comets, extra-solar planets, tests of general relativity. The Science Instruments include; The Hubble Space Telescope's current complement of science instruments include two cameras,two spectrographs, and fine guidance sensors (primarily used for astrometric observations). Because of HST's location above the Earth's atmosphere, these science instruments can produce high resolution images of astronomical objects. Ground-based telescopes can seldom provide resolution better than 1.0 arc-seconds, except momentarily under the very best observing conditions. HST's resolution is about 10 times better, or 0.1 arc-seconds. Wide Field/Planetary Camera 2 The original Wide Field/Planetary Camera (WF/PC1) was changed out and displaced by WF/PC2 on the STS-61 shuttle mission in December 1993. WF/PC2 was a spare instrument developed in 1985 by the Jet Propulsion Laboratory in Pasadena, California. WF/PC2 is actually four cameras. The relay mirrors in WF/PC2 are spherically aberrated to correct for the spherically aberrated primary mirror of the observatory. (HST's primary mirror is 2 microns too flat at the edge, so the corrective optics within WF/PC2 are too high by that same amount.) The "heart" of WF/PC2 consists of an L-shaped trio of wide-field sensors and a smaller, high resolution ("planetary") camera tucked in the square's remaining corner. Corrective Optics Space Telescope Axial Replacement COSTAR is not a science instrument; it is a corrective optics package that displaced the High Speed Photometer during the first servicing mission to HST. COSTAR is designed to optically correct the effects of the primary mirror's aberration on the three remaining scientific instruments: Faint Object Camera (FOC), Faint Object Spectrograph (FOS), and the Goddard High Resolution Spectrograph (GHRS). Faint Object Camera The Faint Object Camera is built by the European Space Agency. It is the only instrument to utilize the full spatial resolving power of HST. There are two complete detector systems of the FOC. Each uses an image intensifier tube to produce an image on a phosphor screen that is 100,000 times brighter than the light received. This phosphor image is then scanned by a sensitive electron-bombarded silicon (EBS) television camera. This system is so sensitive that objects brighter than 21st magnitude must be dimmed by the camera's filter systems to avoid saturating the detectors. Even with a broad-band filter, the brightest object which can be accurately measured is 20th magnitude. The FOC offers three different focal ratios: f/48, f/96, and f/288 on a standard television picture format. The f/48 image measures 22 X 22 arc-seconds and yields resolution (pixel size) of 0.043 arc-seconds. The f/96 mode provides an image of 11 X 11 arc-seconds on each side and a resolution of 0.022 arc-seconds. The f/288 field of view is 3.6 X 3.6 arc- seconds square, with resolution down to 0.0072 arc-seconds. Faint Object Spectrograph A spectrograph spreads out the light gathered by a telescope so that it can be analyzed to determine such properties of celestial objects as chemical composition and abundances, temperature, radial velocity, rotational velocity, and magnetic fields. The Faint Object Spectrograph (FOS) exmaines fainter objects than the HRS, and can study these objects across a much wider spectral range -- from the UV (1150 Angstroms) through the visible red and the near-IR (8000 Angstroms). The FOS uses two 512-element Digicon sensors (light intensifiers) to gather light. The "blue" tube is sensitive from 1150 to 5500 Angstroms (UV to yellow). The "red" tube is sensitive from 1800 to 8000 Angstroms (longer UV through red). Light can enter the FOS through any of 11 different apertures from 0.1 to about 1.0 arc-seconds in diameter. There are also two occulting devices to block out light from the center of an object while allowing the light from just outside the center to pass on through. This could allow analysis of the shells of gas around red giant stars of the faint galaxies around a quasar. The FOS has two modes of operation PP low resolution and high resolution. At low resolution, it can reach 26th magnitude in one hour with a resolving power of 250. At high resolution, the FOS can reach only 22nd magnitude in an hour (before S/N becomes a problem), but the resolving power is increased to 1300. Goddard High Resolution Spectrograph The High Resolution Spectrograph also separates incoming light into its spectral components so that the composition, temperature, motion, and other chemical and physical properties of the objects can be analyzed. The HRS contrasts with the FOS in that it concentrates entirely on UV spectroscopy and trades the extremely faint objects for the ability to analyze very fine spectral detail. Like the FOS, the HRS uses two 521-channel Digicon electronic light detectors, but the detectors of the HRS are deliberately blind to visible light. One tube is sensitive from 1050 to 1700 Angstroms; while the other is sensitive from 1150 to 3200 Angstroms. The HRS also has three resolution modes: low, medium, and high. "Low resolution" for the HRS is 2000 -- higher than the best resolution available on the FOS. Examining a feature at 1200 Angstroms, the HRS can resolve detail of 0.6 Angstroms and can examine objects down to 19th magnitude. At medium resolution of 20,000; that same spectral feature at 1200 Angstroms can be seen in detail down to 0.06 Angstroms, but the object must be brighter than 16th magnitude to be studied. High resolution for the HRS is 100,000; allowing a spectral line at 1200 Angstroms to be resolved down to 0.012 Angstroms. However, "high resolution" can be applied only to objects of 14th magnitude or brighter. The HRS can also discriminate between variation in light from objects as rapid as 100 milliseconds apart.