| A Manual to Accompany Software for the Inductory Astronomy
Lab Exercise
Contemporary Laboratory Experiences in Astronomy Photoelectric Photometry of the Pleiades Document SM 2: Version 1 Department of Physics Gettysburg College Gettysburg, PA 17325 Telephone: (717) 337-6028 email: clea@gettysburg.edu Document modified for online use by Mariet Hofstee on 4/1/03. |
You will use this instrument to collect data on 24 stars in the region of the Pleiades star cluster. The apparent magnitudes will be measured for each star, in the Blue (B) and Visible (V) colors. We will assume all of these stars are approximately the same distance away. This is a necessary assumption, and reasonable because all of the stars are members of the same cluster. If we did not make this general assumption, the apparent magnitudes of the stars would also depend on their individual distances, an effect we cannot easily take into account in this lab.
From this information you will plot a Hertzsprung-Russell (H-R) diagram which will display the apparent magnitude of the cluster of stars as a function of their color index. The color index, B-V, is the apparent blue magnitude (B) minus the apparent visual magnitude (V). All the data will be recorded in the Photoelectric Photometry Data Sheet. This excel file has a graph included that is all set up to display your data. The first datapoint is already recorded and the resulting graph is shown below in figure 1.
| The y axis on the left side corresponds to the calibration data from the Main Sequence. The y-axis on the right side is for your data. Once you have recorded all your data points, you will need to adjust the right hand axis in order for your data to fall on top of the callibration data. To adjust the right hand scale, right click the right hand y-axis of the plot and select 'Format Axis'. You will then get a pop up window like the one on the left. Select the 'Scale' tab and adjust the minimum and maximum values by the same amount to shift your data points up or down. Once the two data sets are alligned, you will be able to relate the apparent magnitude (right hand scale) of a cluster star to an absolute magnitude (M, left hand scale) from the main sequence plot. For example in the case of figure 1, M=0 and m=5. |
Knowing the apparent and absolute magnitude of a star, you can determine its distance (in parsecs) from the equation:
Finally, a few stars will be measured, and their distance compared to data in the Hipparcos catalogue.
You will use this program in the following order:
| DOME | Opens and closes the observatory dome. Open the dome to activate the controls |
| TRACKING | Turns on/turns off the telescope drive. Turning tracking ON causes the telescope to counteract the effect of the Earth’s rotation and is necessary in order to take measurements. Turning tracking OFF allows the star field to drift through the field of view as the Earth turns. |
| SLEW RATE | Controls the rate of telescope movement when the N, E, S, W direction controls are pressed. The slew rate can be set to 1, 2, 4, 8, or 16. The larger the number, the faster the movement rate. Slow speeds are useful for centering a star image. Faster rates are useful for quickly moving from star to star. |
| N, S, E, W | Directional controls. Click one of these buttons to cause the telescope to move north, south, east, or west. When the telescope is moving, a red light next to the direction button glows. Movement in the selected direction continues until the same button is clicked again, or a different direction button is similarly selected. |
| RIGHT ASCENSION | Displays the celestial coordinates of the center of the field of view. Right Ascension is displayed in hours, minutes and seconds. |
| DECLINATION | Declination is displayed in degrees, minutes and seconds. |
| MONITOR | Click to select the FINDER mode or the INSTRUMENT mode. Select FINDER to see a wide angle view of the stars. The red square identifies the field of view when in the PHOTOMETER mode. The PHOTOMETER mode shows a close-up of the star field. It is necessary to select the PHOTOMETER mode to use the photometer. The numbers directly beneath the MONITOR button display the field of view of the screen, that is , how much of the sky is being viewed. |
| SET COORDINATES | When the dome is open, you can click on this button and enter a desired Right Ascension and Declination to move to. After you have entered the coordinates, clicking on OK moves the telescope to the new location in the sky. |
| FILTER | Clicking this button cycles the color filters through U (ultraviolet) , B (blue) and V (visible). |
| SECONDS | Selects the duration of any given integration, or how long light is collected for each reading. The time can be set from 0.1 to 10 seconds. The dimmer a star, the longer the integration time will have to be in order to get an accurate measure of the light. |
| INTEGRATIONS | Adjusts the number of times a measurement is repeated. Multiple readings are averaged. |
| TAKE READING | When the dome is open and the MONITOR is set to the PHOTOMETER mode, clicking this button begins a set of measurements, (how many is determined by the setting of INTEGRATIONS), of a particular time each (how long for each measurement is determined by the setting SECONDS), through the filter selected by the FILTER button. |
NOTE: Before you can start taking readings of stars you must first take initial “sky” readings through all three colored filters. If you forget to take a sky reading, an error message is displayed and a real reading is not taken.
Some additional information is displayed once a reading of the sky or
a star is taken:
| OBS UT | The UTC, or Universal Coordinated Time, at the prime meridian at Greenwich, England. |
| JD | The Julian Date of the OBS UT. The Julian Date is a continuous count of the number of days and fractions of a day since the year -4712. The new Julian Day starts at noon UTC. |
| ELAPSED | The number of SECONDS that have elapsed since any particular reading began. |
| COMPLETED | The number of INTEGRATIONS done so far in the sequence of readings being taken. |
| RAW COUNTS | The photometer simulates a photon-counting photometer. The count of the number of photons captured during the individual reading. |
| SN RATIO | We assume that the only error in the counting if the photons is their randomness defined by quantum mechanics. The square root of the sum of the RAW COUNTS is the fractional error in the reading. A SN RATIO of 100 is needed for a fractional error of 1% (which is 0.01 magnitude). The higher the SN RATIO the lower the fractional error. The SN RATIO, if not high enough, can be raised by increasing the SECONDS or the number of INTEGRATIONS. |
| MEAN SKY COUNT/SEC | The number of MEAN counts contributed by the sky through a particular filter (determined when the sky reading is taken) divided by the SECONDS, giving a normalized photon rate in counts per second. |
| MAGNITUDE | The apparent magnitude of the star, through a particular color filter, based on the MEAN of the counts adjusted by the appropriate MEAN SKY COUNTS/SEC. |