[ TERC VHS-1 Sun Photometer ] [ Manual TOC ]
You will use the data from your Langley test to find what's called the extraterrestrial constant, the signal the TERC VHS-1 would give at the top of the atmosphere (4). In other words, if you took the TERC VHS-1 along on a trip into Earth orbit in the Space Shuttle, the signal you would measure using the TERC VHS-1 during a space walk should be very close to what you measure on the ground using the Langley method.
There are several ways to analyze your data to find the extraterrestrial or ET constant, all of which should yield the same result. After you find your instrument's ET constant, you will insert it in a formula that will give you a standardized measurement of haze known as aerosol optical thickness (AOT).
When you made your Langley measurements for a range of Sun angles, each time the angle changed the thickness of the atmosphere (the air mass) between you and the Sun changed (see Fig. 6.). When the Sun is straight overhead, its light passes through one thickness of atmosphere or one air mass. The air mass (m) increases as the Sun moves closer to the horizon. The m for each of your measurements is 1 divided by the sine of the Sun's angle (<) above the horizon or m = 1/sun<.
If you make a graph of the natural logarithm (ln) of the signal you measured versus m when you made the measurement, the data points should fall along a straight line out to an m of 10 or so, assuming the sky conditions were stable during your measurement period. If you extend the straight line, the ET constant will be where the line crosses the air mass axis at m = 0. When m = 0, there is no air mass, which means this is the signal the TERC VHS-1 will give if you could take it to the top of the atmosphere.
Several methods are available for extracting the ET constant from your Langley test data. They should all give similar or nearly identical results. All three methods perform what is called a linear regression on your data. Briefly, a linear regression fits the equation for a straight line, in this case, ln of signal = a + (b x air mass), to your data. You then use this equation to find the signal for m = 0.
The first two methods require that you determine the air mass for each measurement. The TERC VHS-1 spreadsheet does this automatically, and can be downloaded from: ftp://ftp.concord.org/pub/haze/vhs1-download/ The methods given in the Appendix require that you use a calculator to convert the Sun angles to the respective air masses. The air mass is the reciprocal of the Sun's angle above the horizon, so enter the angle and press the SIN key. Then press the 1/x key to get the air mass.
The TERC VHS-1 spreadsheet program (5) automatically determines the air mass for each data point. You can then use a scientific calculator, the spreadsheet's regression function or curve-fitting software to find the formula for the best fit through the points. The TERC VHS-1 spreadsheet can be downloaded from: ftp://ftp.concord.org/pub/haze/vhs1-download/
Fig. 8 shows a computer-generated graph of the all the data from the first Langley test of a TERC VHS-1. Notice how the data begin to curve when the air mass exceeds about 10? This established that the upper air mass limit for this instrument is m = 10. Fig. 9 shows a second computer-generated graph for only the data up to m = 10. Notice how the points appear to form a straight line?
Figure 10 shows that the points in Fig. 9 form a very straight line indeed. This graph was made with a powerful curve-fitting program called TableCurve (Jandel Scientific). In only seconds, this program fitted the data to hundreds of mathematical functions. It then drew the graph in Fig. 10 for the straight line formula (y = a + bx). The program also gave the coefficients for the formula and the value of the Sun signal for m = 0 (the ET constant). The ET constant for the prototype TERC VHS-1 is 1.2946, the same number provided a little more slowly by a standard scientific calculator using the same data.