8.3 Orbit Use Determination Examples
The easiest way to learn to compute total orbit time requests is to work through a few examples. Below we provide four different examples:
- Example in Section 8.3.1 is a simple WFC image in one filter, using dithers.
- Example in Section 8.3.2 is a two-orbit multi-filter WFC observation using dithering.
- Example in Section 8.3.3 is a one-orbit WFC grism spectroscopic observation.
- Example in Section 8.3.4 is a two-orbit SBC observation.
These examples represent fairly typical uses of ACS.
8.3.1 Sample Orbit Calculation 1
Consider a target to be imaged with WFC in a given filter in one orbit. Using the ETC, we find that we need 2400 seconds of exposure time to reach the desired level of signal-to-noise ratio. Given that the observation is split into a series of two dithers, we map the overheads and the science exposure times onto the orbit as follows:
Table 8.3: Orbit Calculation for Example 1
Action | Time (Minutes) | Explanation |
Orbit 1 | ||
Initial guide star acquisition | 6.5 | Needed at start of observation of a new target |
WFC overhead for the first exposure | 4.0 | Includes filter change, camera set-up, and readout |
Spacecraft slew | 0.5 | |
First science exposure | 20.0 | |
WFC overhead for the subsequent science exposure in the series | 2.5 | Includes readout |
The next science exposure in the series | 20.0 | |
Total time for science exposures | 40.0 | |
Total used time in the orbit | 53.5 |
Thus, the two WFC exposures totaling 2400 seconds make full use of the typically available time in one orbit. The exposure times can be adjusted if the actual target visibility time differs from the derived total used time.
8.3.2 Sample Orbit Calculation 2
This example illustrates the orbit calculation for a WFC observation with the ACS box pattern, which implements imaging at four offset pointings. The goal of the observation is to obtain a dithered image of a field in such a way that would allow us to bridge the 50 pixel interchip gap between the WFC CCDs in the combined image. Given the WFC plate scale 0.05 arcseconds/pixel, this requires that the offsets in the dithering pattern are larger than 2.5 arcseconds. Each offset will then take 0.5 minutes to move the spacecraft from one pointing in the pattern to another. We have determined that the exposure time necessary to reach the desired signal-to-noise ratio is 80 minutes. The orbit calculation will involve a series of 8 exposures (two exposures at each of the four pointings in the dithering pattern) split across two orbits. Slew time below is only applicable for slews <10 arc seconds. For longer slews overhead time may increase. If the exposure time of each image is less than 337 seconds, extra time for the buffer dump will be needed:
Table 8.4: Orbit Calculation for Example 2
Action | Time (Minutes) | Explanation |
Orbit 1 | ||
Initial guide star acquisition | 6.5 | Needed at start of observation of a new target |
WFC overhead for the first exposures | 4.0 | Includes camera set-up, and readout |
WFC overhead for the second exposures | 3.0 | Includes filter change, and readout |
Spacecraft slew | 0.5 | |
WFC overhead for the third and fourth exposures | 2 × 3.0 = 6.0 | Includes filter change and readout |
Four science exposures | 4 × 8.0 = 32.0 | |
Total used time in the orbit | 52.0 | |
Orbit 2 | ||
Guide star re-acquisition | 6.5 | Needed at start of observation |
WFC overhead for the first and second exposures | 2 × 3.0 = 6.0 | Includes camera set-up and readout |
Spacecraft slew | 0.5 | |
WFC overhead for the third and fourth exposures | 2 × 3.0 = 6.0 | Includes filter change and readout |
Four science exposures | 4 × 8.0 = 32.0 | |
Total used time in the orbit | 51.0 |
8.3.3 Sample Orbit Calculation 3
This example illustrates the orbit calculation for a simple 30 minute WFC grism spectroscopic observation broken with a series of two dithered exposures.
Table 8.5: Orbit calculation for example 3.
Action | Time (Minutes) | Explanation |
Orbit 1 | ||
Initial guide star acquisition | 6.5 | Needed at start of observation of a new target |
Predefined imaging exposure for grism spectroscopy | 7.0 | Needed to co-locate the targets and their spectra in the FOV |
WFC overhead for the first science exposure in the series | 4.0 | Includes filter change, camera set-up, and readout |
Spacecraft slew | 0.5 | |
WFC overhead for the subsequent science exposure in the series | 2.5 | Includes readout |
Two science exposures | 2 × 15.0 = 30.0 | |
Total science exposure time | 30.0 | |
Total used time in the orbit | 50.5 |
Unlike similar imaging exposures, here we have to take into account an additional imaging exposure before the sequence of spectroscopic exposures, which takes 10 minutes off the available orbit time.
8.3.4 Sample Orbit Calculation 4
This example deals with the orbit calculation for an observation of a relatively faint extended object using the SBC. The target has to be observed using two filters, F150LP and F165LP. The ETC shows that the required S/N for the observations are achieved in 3200 seconds and 2000 seconds for the F150LP and the F165LP filters, respectively. There is no readout noise associated with SBC exposures; therefore, the observations can be split into four equally long dither pointings. Since the average visibility time for the target is ~55 minutes, the images can be taken in two orbits, as shown in Table 8.6. The standard ACS-SBC-DITHER-BOX pattern, which allows for the rejection of most artifacts, is suitable for these observations. Here are the details of the orbit calculation:
Table 8.6: Orbit calculation for example 4.
Action | Time (Minutes) | Explanation |
Orbit 1 | ||
Initial guide star acquisition | 6.5 | Needed at start of observation of a new target |
SBC overhead for the first exposure | 1.4 | Includes filter change and camera setup |
SBC overhead for each of the following three exposures | 3 × 1.0 | Includes filter change (3 × 0.4 minutes) |
Spacecraft slew | 0.3 | Slew performed between the second and third exposures in this orbit |
Exposures with filter F150LP | 2 × 13.3 = 26.6 | Exposures at the first two pointings of the dither pattern |
Exposures with filter F165LP | 2 × 8.3 = 16.6 | Exposures at the first two pointings of the dither pattern |
Total time used in the orbit | 54.4 | |
Orbit 2 | ||
Guide star re-acquisition | 6.5 | Needed at start of new orbit to observe the same target |
SBC overhead for each of the following three exposures | 4 × 1.0 | Includes filter change (4 × 0.4 minutes) |
Spacecraft slew | 0.3 | Slew performed between the second and third exposures in this orbit |
Exposures with filter F150LP | 2 × 13.3 = 26.6 | Exposures at the first two pointings of the dither pattern |
Exposures with filter F165LP | 2 × 8.3 = 16.6 | Exposures at the first two pointings of the dither pattern |
Total time used in the orbit | 54.0 |
The total time is slightly shorter in the second orbit because of the shorter time required for SBC overheads. There is also ~1 min of visibility available in the first orbit that can be used for the observations. However, we recommend dithered observations in each filter using the same exposure time for each pointing.
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ACS Instrument Handbook
- • Acknowledgments
- • Change Log
- • Chapter 1: Introduction
- Chapter 2: Considerations and Changes After SM4
- Chapter 3: ACS Capabilities, Design and Operations
- Chapter 4: Detector Performance
- Chapter 5: Imaging
- Chapter 6: Polarimetry, Coronagraphy, Prism and Grism Spectroscopy
-
Chapter 7: Observing Techniques
- • 7.1 Designing an ACS Observing Proposal
- • 7.2 SBC Bright Object Protection
- • 7.3 Operating Modes
- • 7.4 Patterns and Dithering
- • 7.5 A Road Map for Optimizing Observations
- • 7.6 CCD Gain Selection
- • 7.7 ACS Apertures
- • 7.8 Specifying Orientation on the Sky
- • 7.9 Parallel Observations
- • 7.10 Pointing Stability for Moving Targets
- Chapter 8: Overheads and Orbit-Time Determination
- Chapter 9: Exposure-Time Calculations
-
Chapter 10: Imaging Reference Material
- • 10.1 Introduction
- • 10.2 Using the Information in this Chapter
-
10.3 Throughputs and Correction Tables
- • WFC F435W
- • WFC F475W
- • WFC F502N
- • WFC F550M
- • WFC F555W
- • WFC F606W
- • WFC F625W
- • WFC F658N
- • WFC F660N
- • WFC F775W
- • WFC F814W
- • WFC F850LP
- • WFC G800L
- • WFC CLEAR
- • HRC F220W
- • HRC F250W
- • HRC F330W
- • HRC F344N
- • HRC F435W
- • HRC F475W
- • HRC F502N
- • HRC F550M
- • HRC F555W
- • HRC F606W
- • HRC F625W
- • HRC F658N
- • HRC F660N
- • HRC F775W
- • HRC F814W
- • HRC F850LP
- • HRC F892N
- • HRC G800L
- • HRC PR200L
- • HRC CLEAR
- • SBC F115LP
- • SBC F122M
- • SBC F125LP
- • SBC F140LP
- • SBC F150LP
- • SBC F165LP
- • SBC PR110L
- • SBC PR130L
- • 10.4 Geometric Distortion in ACS
- • Glossary