Astronomy Lab

Photometry of artificial star

OBJECTIVES

INTRODUCTION.  Photometry in astronomy means the measurement of stellar brightness.  Instruments include the human eye, phototubes and solid-state detectors, and the new CCD cameras.  The brightness of any given star seen from earth depends on two factors: the intrinsic brightness, or size, of the star, and the distance of the star from earth.  The intensity of starlight as a function of distance follows a well-known mathematical relationship.  This relationship will be investigated with an artificial star in the lab (a Light Emmiting Diode - LED) and a CCD camera.  Because other astronomical measurements, such as color, can determine a star's intrinsic brightness, the brightness seen from earth can be used to determine the distance of the star from earth.
 

WHAT DO YOU THINK?

Sketch a graph of distance from the star on the horizontal axis and the brightness as seen by an observer on the vertical axis.  Sketch a plot of what you think the brightness vs. distance will look like.
 

PROCEDURE

Artificial Star.  A LED will serve as an artificial star.  The LED is powered by an electronic battery.  The LED will be mounted in front of a black cardboard which serves as a dark sky background.  We use a Blue LED powered by 2.40 Volt and a 840 Ohm resistance in series.

Camera.  The CCD camera is fitted with a normal photographic lens rather than a telescope.  For astrophotography the telescope serves as the camera "lens", with a much longer focal length.  We will make electronic digital photographs of the LED "star" from several different positions.   We will also take a "Dark" image for each distance of the LED.  The dark image will be obtained by keeping all parameters identical and turning off the diode power.  The room is not completely dark, but that is OK.  We will later subtract the "dark" image.  Each image is saved with a filename that indicates the distance and the time exposure.  The camera is the color DSI and is controlled by the software "envisage", and the lens is a 50 mm FL attached through a T-Thread to C-Thread adapter.  The lens aperture is set to f/11.  The exposure times for the 1.0 meter distance is 0.04 sec.

Analysis.  Immediately after recording each image and the dark frame, both the image and several dark frames are loaded into the analysis software: MaximDL.  Since these are digital images, we can perform simple arithmetic on the images.  We will subtract the average dark frame from the original image to obtain the net image which is the image due to the diode alone.  We will measure the brightness of the star for each distance using a "Photometry" tool in MaximDL.  Set-up the radius of the aperture to 9 pixel radius, gap to 8 pixel, and sky annulus to 10 pixel thickness.  Enter your data in your notebook in a table similar to that shown below.  Do NOT use this paper for your data; use your data book!  Any hand-out with data on it will be torn-up by the instructor!   We will record data with the distance ranging from 1.5 m to 6.0 m.
 

Distance - LED to Camera (m) Exposure Time 
(sec)
Star Brightness
(ADU)
Star Intensity 
(ADU/sec)
Normalized Intensity
Inverse Square
6.0          

If you missed the lab and need the data, get the data from classmate.

Data Plot.  Plot the distances on the horizontal axis and the intensity on the vertical axis.  Be sure to plot each data value as a distinct symbol such as an "o" or an "x".  Connect the plotted points with a smooth curved line.  Compare the plotted graph with what you expected earlier.

Normalized plot.  This section requires a calculator and it requires extending the data table.  In order to observe the mathematical form of the intensity vs. distance we will first normalize the intensity.  This means divide each intensity by the largest intensity.  The largest normalized intensity will have the value of 1.0.  Make a new plot showing the normalized intensity vs distance.  It should look very similar to the first plot but the numbers will be different.

Inverse square plot.  It is hypothesized that intensity of a point source should diminish as the inverse square of the distance from the source.  To test this relationship we will plot an inverse square of the distance (normalized) vs distance as well as the normalized intensity.  For each of the data distances d, calculate the following quantity: (d0/d)2 where d0 is the smallest distance in the data set.  Make another column in the data table:  (d0/d)2 .  Plot this quantity on the same graph as the normalized intensity vs d.  Be sure to use different symbols for the inverse square plot.  If there is good agreement between the inverse square plot and the normalized intensity plot, then the intensity follows the inverse square law.  Be sure to write your conclusions in your notebook and summary.  In a later activity we will set up a computer spreadsheet to calculate these items and to plot using computers.

Note:  Your summary should include the expanded data table and it should  include 2 graphs:  1) the original data plot of intensity vs. distance.  2) the normalized plot and the inverse square plot overlaid on the same axes.  The graphs should be plotted by hand on graph paper.  The summary should describe the layout of the experiment and show a conclusion.