Classifications

• • G—PHYSICS
  • G02—OPTICS
  • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
  • G02B23/00—Telescopes, e.g. binoculars; Periscopes; Instruments for viewing the inside of hollow bodies; Viewfinders; Optical aiming or sighting devices
  • G02B23/16—Housings; Caps; Mountings; Supports, e.g. with counterweight

Definitions

• the invention relates to a reflector carrier device according to the preamble of claim 1.
• Such a reflector support device is known from the publication SPIE, Vol. 1236 Advanced Technology Optical Telescopes IV (1990) page 90 ff.
• two rotationally symmetrical primary mirrors are arranged as astronomical instruments at a predetermined distance on a common carrier. With the help of deflecting mirrors, the reflected rays are brought to a common focus.
• deflecting mirrors There are also multiple deflecting mirrors and a protective housing on the carrier.
• the entire mass of the carrier, the mirrors and the superstructures rests on two swivel bearings of a turntable that can be moved in the horizontal plane. Since the swivel bearings are loaded with the entire weight due to the system, there is a risk that negative effects on image formation will occur, not least because of the natural vibration and frequency of the optical and mechanical devices, which can only be limited by costly, technically difficult countermeasures. Since increasing primary mirror diameters and the associated additional auxiliary devices lead to a large increase in mass, it is difficult to provide swivel bearings which can accommodate these masses while observing the required parameters.
• the known carrier device is therefore not particularly suitable for large telescopes, but also for reflector systems with diameters of more than 8 meters, which are used in other ways.
• a generic carrier device is described in the literature reference H. Hügenell "The Big Eye to Space: The Central Axis Mirror - ZAS", 1989, pages 22 to 25.
• the support for a reflector telescope is in this case mounted hydrostatically with a large contact surface in a stationary trough adapted to the spherical shape of the support in such a way that it can be pivoted about the elevation axis.
• the carrier has a circular cylinder at two diametrically opposite ends coaxial to the elevation axis, each of which is rotatably arranged in a bearing shell and has a rotary drive.
• the bearing shells are located in a ring which is arranged concentrically to the tub and which can be rotated about the elongation axis and which also has a drive.
• the invention has for its object to provide a carrier device of the type mentioned, in which reflector.
• a basic idea of the invention is therefore to distribute the mounting of the actual carrier over two separate components, the main mass being derived via one component tel are arranged on a common, self-supporting carrier, which is hydrostatically large in a tub around its elevation axis and the common optical axis
• the invention is described below with reference to an embodiment shown in the drawing.
• the double reflector is used as a mirror telescope.
• Fig. 1 shows schematically a vertical cross section through a mirror support system of a mirror telescope with two off-axis hyperbol reflectors
• FIG. 2 schematically shows a top view of the mirror support system according to FIG. 1;
• FIGS. 1 and 2 each schematically show a cross section through the mirrors of the mirror support system according to FIGS. 1 and 2 with different mirror arrangements;
• spindle-shaped housing is integrated, which is provided with two adjacent openings for the radiation incident into the interior of the two reflectors or for receiving or emitting high-energy radiation.
• the entire reflector support device including support, trough and ring, are covered by a dome structure designed as a flat spherical cap, that the dome structure is hydrostatically rotatably mounted in a stationary concrete ring, and that the concrete ring is separated from the rest of the stationary foundation by strong, hard rubber-elastic buffers.
• a particularly expedient management of the dome structure is achieved in that it is rotatably arranged on a bearing bed in the end face of the concrete wall, and in that the fixed bearing can be hydraulically or pneumatically converted into a sliding bearing.
• Fig. 1 shows schematically a vertical cross section through
• FIG. 2 schematically shows a top view of the reflector support system according to FIG. 1;
• Fig. 4 each schematically show a cross section through the
• FIG. 6 each schematically show details of the reflector arrangement according to FIG. 4;
• FIG. 7 shows a perspective, partially sectioned illustration of the reflector support system according to FIGS. 1 and 2;
• each primary mirror 5,7 has a diameter of more than 8 m.
• An optimal adaptation to the known diffraction effect of the atmosphere spanning the earth is achieved with aperture diameters of approx. 15 m.
• the reflector support system 12 is rotatably mounted on the one hand about the elevation axis 120 and on the other hand within a horizontal plane that runs normal to the drawing plane. In order to keep the presentation clear, the stationary ones are shown in FIG.
• the reflector support system 12 has a closed, essentially self-supporting, spindle-shaped housing which has two openings 16, 17 lying next to one another for the incidence of radiation. failure in the interior on the two primary mirrors 5,7 is provided.
• the reflector support system 12 has a circular cylinder 10, 13 concentric to the elevation axis 120, the outer jacket of which serves in each case for low-friction mounting for the rotational movement about the elevation axis 120 and access to the housing is possible via the interior thereof.
• An annular casing 11 arranged coaxially to the elevation axis 120 serves for guiding and as a supporting frame.
• a mirror telescope used as an optical instrument comprises, in addition to the two primary mirrors 5, 7, two separate secondary deflection mirrors 2, 3 and two separate tertiary deflection mirrors 6, which are arranged in such a way that the radiation from both primary mirrors 5, 7 is directed onto a common Nasmith Focus 4 is bundled in the elevation axis 120.
• the two reflectors 5, 6 and the respectively associated secondary deflecting mirrors 2, 3 are so-called off-axis mirrors, ie. H. their surfaces represent surface sections of a hypothetical large, aspherical mirror body 126 (FIG. 3); SM (FIG. 7).
• the area of the incident radiation is designated by 123 and 124, respectively, and the virtual focal points and the primary focus are provided with the reference symbols 8, 9 and 1, respectively.
• the two tertiary deflecting mirrors 6 are of flat design.
• FIG. 3 only serves to explain the final situation of primary mirrors 5, 6 in reflector support system 12 shown in FIG. 4.
• FIG. 3 only shows an intermediate consideration that is useful for the final concept.
• the two reflectors 5 ', 7' with the mutually facing edges are each at a predetermined distance a from the common optical axis (OA)
• FIG. 3 also shows with 126 that hypothetical, aspheric and rotationally symmetrical reflector from which the two reflectors 5 ', 7' are "cut out" offset from the optical axis 125 by the distance a.
• the hypothetical focal point of the hypothetical, aspherical and rotationally symmetrical reflector 126 is denoted by F 'and its outer marginal rays, which illustrate a large aperture ratio, are denoted by 41 and 44 respectively (here in the case of a hyperbolic mirror). They coincide on the outer edges of the reflectors 5 ', 7' facing away from one another with their outer marginal rays.
• the inner edge rays incident on the mutually facing edges of the reflectors 5 ', 7' are designated 42 and 43, respectively.
• the image plane (focus) F of the hypothetical large mirror is also the common image plane of the two reflectors 5 ', 7'.
• F is the focal length of the hypothetical large mirror or the mirror combination of the two reflectors 5 ', 7'.
• the image plane F has a grid dimension s. If another surface shape of the large mirror 126 is used, the beam paths also change analogously.
• the basic juries of the two reflectors 5 ', 7' are completely identical because they have the same diameter and the same distance a from the optical axis of the hypothetical large mirror
• the reflectors 5 ', 7' are used to generate large areas
• Reflectors composed of individual segments (see FIG. 7), which are each individually adjustable.
• the segments can be made of quartz for earthbound systems. Its supporting structure has cavities which can be flooded by a cooling gas in order to maintain a constant temperature, whereby a coolant exchange can take place via bores.
• a cooling gas in order to achieve the end position shown in FIG. 4 when using a hyperbolic shaped large mirror 126, the
• reflectors 5, 7 are arranged at a distance b from the optical axis 125 which is greater than the optical distance a.
• the two reflectors 5, 7 are symmetrical to the optical axis 125 and each inclined at an angle a to the optical axis 125 in such a way that those edge rays 420 and 430 which are closest to the optical axis 125 are at a distance from it cut that is larger than the focal length f of the hypothetical large reflector 126. In this way, the dead area A 'of the observation is eliminated.
• the inclination of the reflectors 5,7 by the angle a to the optical axis 125 is omitted when using differently shaped large mirror surfaces.
• the superimposition of the beams reflected by the two primary mirrors 5, 7 results in an object imaging in the focal plane which is carried out from different angles and which allows an interference image of this object within an optimal image grid dimension.
• the total light intensity of an equivalent, one-piece primary mirror with a diameter of 21.21 m results.
• the two secondary deflecting mirrors 2, 3 go back to a separate hypothetical mirror SM (FIG. 7) that would be required to reflect the reflected light of the hypothetical large mirror 126 to reflect the so-called Cassegrain or Nasmith focus (or other, further common focal points).
• the two secondary deflecting mirrors 2, 3 therefore consist of partial surfaces of a convexly curved hypothetical mirror surface which are spaced from its optical axis and which are dimensioned such that they reflect the reflection rays of the reflectors 5, 7 over the plane tertiary mirror 6 to the desired focal point 4 (Fig. L) or immediately one
• FIG. 5 further illustrates, using the example of a primary reflector 5, that not only the two primary mirrors are composed of separately controllable and adjustable, honeycomb-shaped segments 19, but also the secondary deflecting mirrors 2 and 3, respectively, by adapting the size ratios hold, only a single segment 19 or 18 in the primary mirror 5 or secondary mirror 2 is shown in FIG. 5.
• FIG. 6 shows the manner in which an uninterrupted arrangement of honeycomb elements 18 is arranged in a row
• Reflector surface is obtained.
• the exact alignment to the respective focal point takes place by means of computer-controlled actuators.
• FIG. 7 shows a perspective representation of the manner in which a reflector arrangement according to FIG. 5 is expanded into a paired arrangement and is arranged within the mirror carrier system 12.
• the hypothetical reflector from which the two secondary deflecting mirrors 2, 3 are derived is shown in the figure to complement the above statements and is designated by SM.
• the spindle-shaped housing of the reflector support system 12 is in a tight, circular trough 22 on one
• the effective liquid storage area is designated by 21.
• the tub 22 itself is again rotatably supported hydrostatically in a concrete bed in the horizontal plane and surrounded by a stationary, ring-shaped concrete jacket 23. Together with an outer concrete ring 25, this forms a foundation and a concentric guide for a rotatably mounted ring 24, which has two bearing shells 20 for the
• Circular cylinder 10.13 of the reflector support system 12 is provided. Both the ring 24 and the tub 22 are each separately hydrostatically mounted, so that the effect of their own mass is negligible. In addition, the ring 24 and the trough 22 are each acted upon by a drive via which they can be set into a rationing movement in the horizontal plane. Both drives are electronically coupled in such a way that the ring 24 serves as a master or as a reference for the shell 22 for controlling the angular velocity during a common rotation about the elongation axis of the reflector carrier system 12.
• the Betonummante ⁇ ung 23 ensures that the rotary drive forces for the ring 24 and the tub 22 do not interfere with each other, but can be precisely controlled without undesirable mutual interference.
• the trough 22 takes up the main load of the reflector support system 12.
• the bearings 20 of the circular cylinder 10.13 are relieved in comparison. This enables precise control of the so-called altazimuthal tracking in the sky.
• the annular casing 11 of the reflector support system 12 is provided with a further drive 30 (FIG. 9).
• the casing 11 also serves to stabilize the rotation of the mirror support system 12.
• the rotary drive unit 30 is arranged where the reflector support system 12 merges into its hydrostatic bearing in the tub 22.
• the rotary drive unit 30 comprises two coaxial drive wheels 127, for example gear wheels, which interact with corresponding counterparts or predetermined tracks 31 on the annular casing 11.
• FIG. 8 further illustrates that the entire reflector support system 12, the trough 22 and the ring 24 together with the concrete casing 23 and the foundation 25 are covered by a dome structure (protective dome) 28 serving as weather protection.
• the Cupola 28 is designed as a flat spherical cap and placed concentrically over the entire system.
• slit-shaped openings (not shown), which are required for the incidence of light, from the zenith position of the telescope to the deepest angular positioning of the optical openings to the horizon, it can optionally be closed without gaps with a single locking mechanism.
• the openings are slit-shaped, so that a lateral surface belonging to the spherical cap extends between these openings.
• the locking mechanism is stabilized in this way because the spanning closure width offers a firm support exactly in the middle and along the closure path.
• the dome structure 28 is mounted in a stationary concrete ring 27 in a hydrostatically rotatable manner in the horizontal plane. The mass of the dome structure 28 is removed into the ground via the annular concrete wall 27.
• the concrete ring 27 is separated from the foundation 25 by strong, hard rubber-elastic buffers 26, which are arranged in a ring.
• the soil outside the entire system is designated with 29.
• the dome structure 28 comprises a supporting structure 34 and an outer cladding 35.
• the guidance in the annular concrete wall 27 takes place via a bearing bed 33 in the end face of the concrete wall 27, in which a hollow body 32 arranged on the dome structure 28 engages.
• the hollow body 32 and the bearing bed 33 act in this way
• the bearing is acted upon hydraulically or pneumatically, so that a low-friction rotational movement can take place.
• a constantly horizontally aligned and low-vibration inner platform is arranged inside the circular cylinder 10, 13, which extends so far into the interior of the reflector support system 12 that the instruments and devices required for the Nasmith focus can be accommodated in a user-friendly manner.

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• Physics & Mathematics (AREA)
• Astronomy & Astrophysics (AREA)
• General Physics & Mathematics (AREA)
• Optics & Photonics (AREA)
• Telescopes (AREA)
• Organic Low-Molecular-Weight Compounds And Preparation Thereof (AREA)

Applications Claiming Priority (2)

Publications (1)

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• 1990
  • 1990-12-13 DE DE4039880A patent/DE4039880C1/de not_active Expired - Fee Related
• 1991
  • 1991-05-08 CH CH1397/91A patent/CH682956A5/de not_active IP Right Cessation
  • 1991-12-10 EP EP92900286A patent/EP0515609A1/de not_active Withdrawn
  • 1991-12-10 US US07/916,980 patent/US5367407A/en not_active Expired - Fee Related
  • 1991-12-10 CA CA002075836A patent/CA2075836A1/en not_active Abandoned
  • 1991-12-10 AU AU90361/91A patent/AU657932B2/en not_active Ceased
  • 1991-12-10 JP JP4500245A patent/JPH05504850A/ja active Pending
  • 1991-12-10 WO PCT/CH1991/000259 patent/WO1992010775A1/de not_active Application Discontinuation
• 1992
  • 1992-12-10 KR KR1019920701902A patent/KR920704175A/ko not_active Application Discontinuation
• 1993
  • 1993-04-20 LV LVP-93-253A patent/LV10816B/lv unknown

Non-Patent Citations (1)

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