Voyager 1 Narrow Angle Camera Description
Index
- Instrument Information
- Instrument Description
- Science Objectives
- Operational Considerations
- Calibration Description
- Field Of View
- Parameters
- Instrument Detector
- Instrument Electronics)
- Instrument Filters
- Instrument Optics
- Instrument Operational Modes
- Scan Platform
- References
Instrument Information
Instrument Id : ISSN
Instrument Host Id : VG1
Pi Pds User Id : BASMITH
Naif Data Set Id : UNK
Instrument Name : IMAGING SCIENCE SUBSYSTEM -
NARROW ANGLE
Instrument Type : VIDICON CAMERA
Build Date : 1976-12-17
Instrument Mass : 22.060000
Instrument Length : 0.980000
Instrument Width : 0.250000
Instrument Height : 0.250000
Instrument Serial Number : SN07
Instrument Manufacturer Name : JET PROPULSION LABORATORY
Instrument Description
The Voyager Imaging Science Subsystem (ISS) is a modified version of the slow scan vidicon camera designs that were used in the earlier Mariner flights. The system consists of two cameras, a high resolution Narrow Angle (NA) camera and a lower resolution, more sensitive Wide Angle (WA) camera. Unlike the other on board instruments, operation of the cameras is not autonomous, but is controlled by an imaging parameter table residing in one of the spacecraft computers, the Flight Data Subsystem (FDS) (Science and Mission Systems Handbook, 1987, JPL D-498, an internal JPL document available from the JPL vellum files).
The original mission was to Jupiter and Saturn. Voyager surpassed expectations and went on to encounter Uranus and Neptune. As the Voyager mission progressed the objects photographed were further from the sun so they appear more faint even though longer exposures were used. As the Voyager spacecrafts’ distance from the Earth increases, the telecommunications capability at each encounter decreases. The difference in capabilities from the Jupiter and Saturn encounters and that at Uranus and Neptune was considerable. The reduced telecommunications capability limits the number of data modes that imaging can use. Because of the diminished brightness of the objects being photographed, longer exposure times were used, many beyond the stated maximum of 15.360 seconds. Longer exposure times were all 48-second increments added to the maximum. In addition, the camera was slewed in order to avoid smeared imaging. The light flood state (on/off) was independent of the instrument mode.
Science Objectives
The overall objective of this experiment is exploratory reconnaissance of Jupiter, Saturn, Uranus, Neptune and their satellites and rings. Such reconnaissance, at resolutions and phase angles unobtainable from Earth, provides much new data relevant to the atmospheric and/or surface properties of these bodies. The experiment also has the following specific objectives: observe and characterize global circulation and meteorology; determine the horizontal and vertical structure of visible clouds; characterize the nature of any colored material which may be in clouds.
Operational Considerations
To make full scientific use of the imaging collection, it is necessary to understand the radiometric and geometric characteristics of the camera system and perform corrections to the data.
Each Voyager camera is unique in terms of its calibrated characteristics. Each has intrinsic shading (spatially non-uniform output DNs from flat field target) and exhibits barrel distortions typical of TV cameras flown on previous planetary missions. Because of these characteristics, the cameras were calibrated before launch. The response of the pixels to known targets, illumination, exposures, etc. was measured and Calibration Files were generated to remove radiometric an geometric distortions from the flight images. These Calibration Files and detailed information on their use are available through the Imaging Node.
Calibration Description
The calibration program for the Voyager television cameras consisted of three parts: (1) component calibrations (‘Voyager Imaging Science Subsystem Calibration Report’ July 31, 1978, M. Benesh and P. Jepsen, D618-802); (2) subsystem calibrations; and, (3) system calibrations. Component calibrations were carried out prior to camera assembly. Important measurements include spectral transmittance of the lens and filters, actual exposure times and shading characteristics of the shutter, and pertinent electro-optical properties of the vidicon. After the optics and sensor were assembled it was possible to run calibrations at the camera, or subsystem, level. Particular activities accomplished during this period included radiometric calibrations, focal length measurement, determination of the modulation transfer function, measurement of the geometric distortion, and calibrations required for color reconstruction. System calibrations were conducted after the cameras were installed on the spacecraft. Important tasks included measurement of the Field-Of-View (FOV) alignment and verification of the flat-field light transfer characteristics. Noise measurements were also made at the system level.
A method for in-flight verification of the radiometric calibrations that were run on the ground is employed on the Narrow-Angle optics. It is very similar to the scheme used on the Wide-Angle optics except that eight lamps are required. They are located just within the Field-Of-View around the periphery of the telescope aperture. By either pulsing the lamps or leaving them on and varying the shutter exposure time a transfer curve may also be generated by using the calibration plaque. The method is identical to that described for the wide-angle optics. However, calibration data was collected but no new calibration files were generated during the Jupiter, Saturn, or Uranus encounters or their related cruise periods.
Although the INSTRUMENT_PARAMETER_NAME has been provided as Radiance, the Voyager Experiment Data Record (EDR) data set has not been radiometrically corrected, and thus images do not represent radiance units. In order to convert an image from Data Number (DN) to radiance units, the image must be calibrated. Radiometric calibration files, and selected radiometrically corrected images are available through the Imaging Node.
Field Of View (FOV)
Total Fovs : 1
Sample Bits : 8
FOV (Field Of View) Shape ‘SQUARE’
Section Id : ISSN
Fovs : 1
Horizontal Pixel Fov : 0.000530
Vertical Pixel Fov : 0.000530
Horizontal Fov : 0.424000
Vertical Fov : 0.424000
Parameters
Radiance is the amount of energy per time per projected area per steradian.
Instrument Parameter Name : RADIANCE
Sampling Parameter Name : PIXEL
Instrument Parameter Unit : DIMENSIONLESS
Noise Level : UNK
Instrument Detector
Detector Type : VIDICON
Detector Aspect Ratio : 1.000000
Minimum Wavelength : 0.280000
Maximum Wavelength : 0.640000
Nominal Operating Temperature : 282.000000
The sensor used in the Voyager Imaging Science Subsystem (ISS) camera system is a 25-mm diameter magnetic deflection vidicon (number B41-003, General Electro-dynamics Co.). The vidicon storage surface (target) is selenium sulphur and can store a high resolution (1500 TV lines) picture for over 100 s at room temperature. The active image area on the target is 11.14 x 11.14 mm. Each frame consists of 800 lines with 800 picture elements (pixels) per line, i.e., 1 pixel =14 microns. One frame requires 48 s for electronic readout. In addition to the normal frame readout of 48 s (1:1), four extended frame-time modes of 2:1, 3:1, 5:1, and 10:1 are available by command. Following readout, light flooding is used to remove any residual image that might remain from the previous frame. At the end of light flooding, 14 erase frames are used to stabilize and prepare the vidicon target for the next exposure sequence (VGR ISS Calibration Report, 1978, an internal JPL document available from JPL vellum files).
Sensitivity
Calibration experiments show the gain map indicating higher sensitivity toward the top of the frame in a radial manner. Dark-current ratio results indicate a mean within plus-or-minus 3% of the true linearity of the light transfer function. The required accuracy of the light transfer functions was plus-or- minus 5% of half-scale signal averaged over any randomly selected area of 10 contiguous pixels. This requirement was consistently met for all ISS flight cameras. The radiance of the used light cannons was supposed to be plus-or- minus 5% or better of the level to produce a half-scale signal. This criterion was also met. It is not clear whether the color spatial dependence is due to the vidicon, or whether the filters have varying transmissions. In the latter case, the ratios would be independent of light level; and this has been observed to be the case for all flight cameras. Moreover, vidicons have not shown scale variations of this magnitude in the past, so that it is easier to believe that they are due to the spectral filters rather than to the vidicons. The color sensitivity is sufficient to require a separate decalibration file for each spectral filter, which has been done, but not gross enough to cause concern about the quality of the image itself (VGR ISS Calibration Report, 1978, an internal JPL document available from JPL vellum files).
Instrument Electronics
The Imaging Science Subsystem (ISS) electronics consist of the vidicon support circuits and the signal chain. The vidicon support circuits are the vertical and horizontal sweep circuits, and the various power supplies for the vidicon filament, and the focus and alignment coils. The signal chain consists of the analog signal amplifiers, bandpass filters, and an eight bit analog-to-digital converter. The digital output is sent to the Flight Data Subsystem (FDS) for editing.
Filters
Spectral measurements at the manufacturer were taken on Beckman spectro- photometers, and verifications at Jet Propulsion Laboratory (JPL) were made with a Cary 14 spectro-photometer. Each test scan was run from 2000 to 7000 Angstroms to check for eventual leaks outside the passband (VGR ISS Calibration Report, 1978, an internal JPL document available from JPL vellum files). For spectral information on each filter, see Danielson, E. G., et al. Radiometric Performance of the Voyager Cameras, JGR, v. 86, Sept. 1981.
Instrument Filter ‘0 - CLEAR’
Filter Name : CLEAR
Filter Type : ABSORPTION
Minimum Wavelength : 0.280000
Maximum Wavelength : 0.640000
Center Filter Wavelength : 0.460000
Instrument Filter ‘1 - VIOLET’
Filter Name : VIOLET
Filter Type : INTERFERENCE
Minimum Wavelength : 0.350000
Maximum Wavelength : 0.450000
Center Filter Wavelength : 0.400000
Instrument Filter ‘2 - BLUE’
Filter Name : BLUE
Filter Type : INTERFERENCE
Minimum Wavelength : 0.430000
Maximum Wavelength : 0.530000
Center Filter Wavelength : 0.480000
Instrument Filter ‘3 - ORANGE’
Filter Name : ORANGE
Filter Type : INTERFERENCE
Minimum Wavelength : 0.590000
Maximum Wavelength : 0.640000
Center Filter Wavelength : 0.615000
Instrument Filter ‘4 - CLEAR’
Filter Name : CLEAR
Filter Type : ABSORPTION
Minimum Wavelength : 0.280000
Maximum Wavelength : 0.640000
Center Filter Wavelength : 0.460000
Instrument Filter ‘5 - GREEN’
Filter Name : GREEN
Filter Type : INTERFERENCE
Minimum Wavelength : 0.530000
Maximum Wavelength : 0.640000
Center Filter Wavelength : 0.585000
Instrument Filter ‘6 - GREEN’
Filter Name : GREEN
Filter Type : INTERFERENCE
Minimum Wavelength : 0.530000
Maximum Wavelength : 0.640000
Center Filter Wavelength : 0.585000
Instrument Filter ‘7 - ULTRAVIOLET’
Filter Name : ULTRAVIOLET
Filter Type : INTERFERENCE
Minimum Wavelength : 0.280000
Maximum Wavelength : 0.370000
Center Filter Wavelength : 0.325000
Instrument Optics ‘ISS-NA’
Telescope Diameter : 0.176500
Telescope F Number : 8.500000
Telescope Focal Length : 1.502380
Telescope Resolution : 0.000018
Telescope Serial Number : NAO-05
Telescope T Number : 12.110000
Telescope T Number Error : 0.110000
Telescope Transmittance : 0.600000
The Narrow-Angle camera optics is a 1500mm diameter focal length all- spherical, catadioptric cassegrain telescope (a modified MVM 1973 design) consisting of five elements plus an additional dust lens located between the shutter and the vidicon. The f stop number is 8.5. (VGR ISS Calibration Report, 1978, an internal JPL document available from JPL vellum files).
Instrument Operational Modes
Instrument Mode ‘IM2’
Data Path Type : RECORDED DATA PLAYBACK
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 1:1, full frame image, 800 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM3’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 1:1, full frame, 800 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM4’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 1:1, centered frame, 608 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM5’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 2:1, Top read out in frame #1, bottom read out in frame #2, 800 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM6’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 1:1, centered frame, 440 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM7’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 3:1, full frame, 800 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM8’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 1:1, centered frame, 272 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM9’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 3:1, centered, approx. 480 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM10’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 1:1, centered frame, approx. 160 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM11’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 5:1, centered frame, 800 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM12’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 5:1, centered frame, approx. 440 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM13’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 10:1, centered frame, 800 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM14’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 1:1, centered frame, approx. 80 pix/line (Jupiter and Saturn)
Instrument Mode ‘IM15’
Data Path Type : REALTIME
Gain Mode Id : LOW
Instrument Power Consumption : 14.000000
Scan rate (minor frame:line) is 2:1, centered frame, top read out in frame #1, bottom read out in frame #2, 800 pix/line (Jupiter and Saturn)
Scan Platform
Cone Offset Angle : 0.000000
Cross Cone Offset Angle : 0.000000
Twist Offset Angle : 0.000000
The measurements recorded below are the coordinates representing the center of the Wide Angle Field-Of-View (FOV) in relation to the center of the Narrow Angle FOV. As of 5/26/88 the Voyager 2 scan platform offset values were updated and the removal of all extraneous offset values for VG1 and VG2 accomplished. Only the most recently input values remain in the database for each spacecraft. These values are effective for all periods of data inclusive from launch to present. (June 7, 1989).
References
BARROS1988
BENESH1978
DANIELSONETAL1981
HARCH1987
HARCH1988A
HARCH1988B
HARCH1988C
JPL D-2468
JPL D-498
MARTINETAL1985
NAVE1980
SCIENCEV204N4392
SCIENCEV206N4421
SCIENCEV212N4491
SCIENCEV215N4532
SCIENCEV233N4759
SCIENCEV246N4936
SNYDERL1979
SSRV21N2
SSRV21N3