Calculator assumptions: Primary brighter than 9.0, the secondary is brighter than 13.0, the secondary is between 0 magnitudes and 7 magnitudes dimmer than the primary.
S = 1.033 * 10 ^ [ 1/n * ( Abs(delta mag) - 0.1 ) ] * rho
Aperture Dmm | Aperture index | Obstruction ratio | Obstruction index | Seeing - suprious disk | Seeing index |
---|---|---|---|---|---|
<75 | 4 | 0 | 4 | I<0.25p | 4 |
75-150 | 3 | 0.1 | 3 | II>0.25p | 3 |
151-300 | 2 | 0.2 | 2 | III<0.50p | 2 |
301-450 | 1 | 0.33 | 1.5 | IV<1.00p | 1 |
451-600 | 0.5 | 0.4 | 1 | V>1.50p | 0.5 |
600 | 0.5-0.25 | 0.5 | 0.5 |
Although not explicited stated in Lord's 1994 paper, the following computational restrictions are added to this calculator for computational convenience and to assure valid results always are returned to the user:
Tung's proposal for continuous indices, implemented in this calculator, are:
nD = (2.4 - (D_mm/150)) {Eq. 1}
nE = (2.0 - (5*obstruction_fraction)) {Eq. 2}
nS = (2.3 - (8*FWHM*(D_mm/lambda_nm))) {Eq. 3}, where FWHM is in arcseconds and D_mm and lambda_nm their unadjusted values, not reduced to common units of meters
Lord, Chris. 1994. Nomogram for Telescopic Resolution of Unequal Binaries. Brayebrook Observatory.
Lord, Chris. 1994. A Report on the Analysis of the Telescopic Resolution of Unequal Binaries. Brayebrook Observatory.
Lord, Chris. Jan. 2008. Personal Communication.
Tung, Brian. 8/14/2006. Personal Communication
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Prepared K. Fisher fisherka@csolutions.net org. 7/2006 rev. 2/3/2008