time HA tau HA(calc) tau(calc) 21:00 23:49:33 1.008 23.739 1.008 1688 23:00 1:49:52 1.073 25.739 1.067 1585 1 3:50:12 1.350 3.805 1.344 1525 2 4:50:21 1.634 4.805 1.625 1464 3 5:50:32 2.118 5.805 2.104 1397 3:30 6:20:37 2.493 6.305 2.476 1304 vega RA=18:36:56 dec=38:47:01 wiki observator: 45:34:30 & 94:23:47 sept 1-> D=244 * @hmmss.cal * let lat=f(45.3430)*pi/180 * let dec=f(38.4701)*pi/180 * let long=f(94.2347)/15 * let day=244 * let RA=f(18.3656) * ? 21+.0657*day+(5-long)+f(6.37)-RA 23.73881851851852 * let HA=res*pi/12 * ? 1/(cos(lat)*cos(dec)*cos(HA)+sin(lat)*sin(dec)) 1.008361097397202 ? 23+.0657*day+(5-long)+f(6.37)-RA let HA=res*pi/12 ? 1/(cos(lat)*cos(dec)*cos(HA)+sin(lat)*sin(dec)) 25.73881851851852 1.066761081564735 ? 1+.0657*(day+1)+(5-long)+f(6.37)-RA let HA=res*pi/12 ? 1/(cos(lat)*cos(dec)*cos(HA)+sin(lat)*sin(dec)) 3.804518518518517 1.344126787154939 ? 2+.0657*(day+1)+(5-long)+f(6.37)-RA let HA=res*pi/12 ? 1/(cos(lat)*cos(dec)*cos(HA)+sin(lat)*sin(dec)) 4.804518518518517 1.625118945785555 ? 3+.0657*(day+1)+(5-long)+f(6.37)-RA let HA=res*pi/12 ? 1/(cos(lat)*cos(dec)*cos(HA)+sin(lat)*sin(dec)) 5.804518518518517 2.104142999214284 ? 3.5+.0657*(day+1)+(5-long)+f(6.37)-RA let HA=res*pi/12 ? 1/(cos(lat)*cos(dec)*cos(HA)+sin(lat)*sin(dec)) 6.304518518518517 2.475942012115166 An analysis of data submitted by computer: on 14-SEP-2018 at 14:39 indicates that a function of the form: --Exponential-- y=A exp(Bx) can fit the 6 data points with a reduced chi-squared of 0.86 FIT PARAMETER VALUE ERROR A = 1906. 63. B = -0.1538 0.20E-01 NO x-errors y-errors based on formula: SQRT(Y) ACTUAL ERROR IN CALCULATED DEVIATION POINT X Y Y Y FROM FIT 1 1.01 0.169E+04 +- 41. 0.163E+04 55.9 2 1.07 0.158E+04 +- 40. 0.162E+04 -32.4 3 1.34 0.152E+04 +- 39. 0.155E+04 -24.9 4 1.62 0.146E+04 +- 38. 0.148E+04 -20.3 5 2.10 0.140E+04 +- 37. 0.138E+04 18.1 6 2.48 0.130E+04 +- 36. 0.130E+04 1.80 see 364t104.pdf #1 (but with nu) lets consider a bin between .49e-6 & .51e-6 m there are 17 photons in this bin which has frequency width * ? c*(1/.49e-6-1/.51e-6) 23992993837534.98 seek photons per second per area per bin-size ? 17/600/(pi/4*1^1)/res .1503568945102904E-14 !1/(sec*m^2*Hz) it was not requested but might seek energy flux (17 photons each with E=h*nu) ? h*c/.5e-6*res .5973516504707997E-33 in terms of Jansky: Jy=(1E-26 W/m^2/Hz) ? res/1e-26 .5973516504707997E-07 !or 60 nJy Remark: while the flux of photons is of course much reduced light years from the star, the distribution of the received photons should match what was emitted, so we concentrate on measures of that distribution (mean, median, mode) rather than the absolute flux. (Using the measured flux would be possible if we knew the distance --and hence how much the flux was reduced-- but we don't.) from class: (where x=h nu/kT) mode: x=1.59362 median: x=2.35676 average: x=2.70118 in spreadsheet calculate: h*c/k*(1/cells) =x*T for all 1000 cells, find median and/or average of these, equate to above * ? h*c/(kb*1e-6) .1438777353827720E5 0.03284879803259635E6 =median = median(x)*T; T= 0.03284879803259635E6/2.35676 = 13938 0.03833068594121622E6 =average = average(x)*T; T=0.03833068594121622E6/2.70118 = 14190 The statistical language R finds modes: D=read.csv("1000_lambda.txt",sep="",header=F,skip=1) d=as.vector(unlist(D)) di=1/d > mean(di) [1] 2.664115 > median(di) [1] 2.283105 dd=density(di) dd$x[dd$y==max(dd$y)] 1.302463 h*c*1e6*1.302463/k=mode(x)*T; T=h*c*1e6*1.302463/1.59362/kb; T=11759 (low)