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 [http://www.iram.es/IRAMES/mainWiki/TelescopeSystemSummary Back to the IRAM 30m System Summary]
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 1. '''Gain-elevation curves.''' The most recent curves are given in the IRAM Annual Report 2007 attachment:IRAM_2007.pdf  1. '''Gain-elevation curves.''' The most recent curves are given in the IRAM Annual Report 2007
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New values measured in August 2007:

 || '''Freq''' || '''HPBW''' || '''Feff''' || '''Beff''' || '''Aeff''' || '''S/TA*''' || '''Comments''' ||
 || '''GHz''' || '''arcsec''' || '''%''' || '''%''' || '''%''' || '''Jy/K''' || ||
 || 86 || 28.5 || 98 || 78 || 64 || 5.9 || ||
 || 145 || 16.9 || 95 || 64 || 53 || 6.9 || ||
 || 210 || 11.3 || 94 || 62 || 51 || 7.2 || ||
 || 260 || 9.0 || 90 || 53 || 44 || 8.0 || ||
 || 345 || 7.0 || 87 || 39 || 32 || 10.6 || estimated ||

 1. '''Half power beam width HPBW.''' The HPBW can be well fitted by: HPBW/arcsec=2406/Freq/GHz or HPBW/rad=1.166 W/D, with the wavelength W and the telescope diameter D.

 1. '''Forward efficiency Feff.''' The values for Feff were updated after the 12th of December 2000 when a new reflecting ring was put around the secondary mirror. Forward efficiencies are derived from skydips. Values in the table are from measurements in August 2007.

 1. '''Aperture Efficiency Aeff.''' The aperture efficiency of the 30m telescope can be obtained via pointings on point-like celestial calibrators with a well known flux, like Uranus or Mars, when it is small. Aeff can be computed from 3.906 K TA* Feff / Ssou, where K is the correction factor that considers the coupling of the disk size of the planet to the HPBW, TA* is the peak antenna temperature, and Ssou is the intrinsic flux density of the planet. (see Eq.16 in attachment:spatial_response_framework_v1.8.pdf)

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[http://www.iram.es/IRAMES/mainWiki/TelescopeSystemSummary Back to the IRAM 30m System Summary]

Telescope efficiencies and beam widths

  • Below you find the forward and beam efficiencies upto 280 GHz measured in March 2005 ([http://www.iram.fr/IRAMFR/ARN/aug05/node6.html IRAM Newsletter 8/05]). Values above 300 GHz are predictions based on the observations compiled in the IRAM Annual Report 2007 attachment:IRAM_2007.pdf ).

    freq

    HPBW

    Beff

    Aeff

    S/TA*

    Feff

    Comments

    (GHz)

    (arcsec)

    (%)

    (%)

    (Jy/K)

    (%)

    (1)

    (2)

    (3)

    (4)

    (5)

    (6)

    72 (extrapolated)

    34

    79

    6.0

    95

    77 (extrapolated)

    32

    79

    6.0

    95

    86

    29

    78

    6.0

    95

    110

    22

    75

    6.3

    95

    145

    17

    69

    6.7

    93

    170

    14.5

    65

    7.1

    93

    210

    12

    57

    7.9

    91

    235

    10.5

    52

    8.7

    91

    260

    9.5

    46

    9.5

    88

    279

    9

    42

    10.4

    88

    310

    7.9

    37

    predicted

    345

    7.1

    32

    predicted

    360

    6.8

    30

    predicted

  • The half power beam width, HPBW, can be well fitted by: HPBW/arcsec = 2460/freq/GHz.

  • Main beam efficiency Beff. The data can be well fit by a Ruze function Beff = 1.2 Aeff' exp[-(4pi R sigma/ lambda)^2] with sigma being the rms value of the surface errors of the main dish, R the reduction factor for a steep main reflector, Aeff' is the aperture efficieny of the perfect telescope and lambda the wavelength in mm. The data can be fitted by R*sigma = 0.07 and epsilon = 0.69.

  • Aperture efficiency, Aeff. The aperture efficiency of the 30m telescope can be obtained via pointings on point-like celestial calibrators like Uranus or Mars. In the approximation that the beam is Gaussian and the edge taper is -14dB, it can also be derived from the beam efficiency using Aeff=Beff*0.80 (attachment:spatial_response_framework_v1.8.pdf)

  • Point source sensitivity S/TA*. S/TA* is 3.906*Feff/Aeff Jy/K for the 30m (see attachment:cali_rep.pdf).

  • Gain-elevation curves. The most recent curves are given in the IRAM Annual Report 2007

  • Forward efficiency Feff. The values for Feff are valid after the 12th of December 2000 when a new reflecting ring was put around the secondary mirror. Forward efficiencies are derived from skydips.

  • Error beams. A part of the power pattern is distributed in three error beams (see the analysis of attachment:greve_1998.pdf). The size of the described Gaussians is unchanged, however the main beam efficiencies have been improved in the meanwhile, lowering the strengths of the error beams. A new paper is in preparation. Astronomers should take the contribution of the error beam into account when converting antenna temperatures to brightness temperatures, especially when mapping extended sources.

  • Historic values: [http://www.iram.es/IRAMES/telescope/telescopeSummary/beam_effis.html Plot of efficiencies against frequency, measured in 2000], [http://www.iram.es/IRAMES/telescope/telescopeSummary/effi_history.html Compilation of efficiencies obtained in the past till 2001].


New values measured in August 2007:

  • Freq

    HPBW

    Feff

    Beff

    Aeff

    S/TA*

    Comments

    GHz

    arcsec

    %

    %

    %

    Jy/K

    86

    28.5

    98

    78

    64

    5.9

    145

    16.9

    95

    64

    53

    6.9

    210

    11.3

    94

    62

    51

    7.2

    260

    9.0

    90

    53

    44

    8.0

    345

    7.0

    87

    39

    32

    10.6

    estimated

  • Half power beam width HPBW. The HPBW can be well fitted by: HPBW/arcsec=2406/Freq/GHz or HPBW/rad=1.166 W/D, with the wavelength W and the telescope diameter D.

  • Forward efficiency Feff. The values for Feff were updated after the 12th of December 2000 when a new reflecting ring was put around the secondary mirror. Forward efficiencies are derived from skydips. Values in the table are from measurements in August 2007.

  • Aperture Efficiency Aeff. The aperture efficiency of the 30m telescope can be obtained via pointings on point-like celestial calibrators with a well known flux, like Uranus or Mars, when it is small. Aeff can be computed from 3.906 K TA* Feff / Ssou, where K is the correction factor that considers the coupling of the disk size of the planet to the HPBW, TA* is the peak antenna temperature, and Ssou is the intrinsic flux density of the planet. (see Eq.16 in attachment:spatial_response_framework_v1.8.pdf)


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Iram30mEfficiencies (last edited 2016-11-03 18:07:57 by CarstenKramer)