Title: Improving the inverse of Carrington longitude to corresponding central meridian crossing time: A nec
1Improving the inverse of Carrington longitude to
corresponding central meridian crossing time A
necessary step to estimate the effect of
differential rotation
21. Introduction
- Synoptic charts of the photospheric
magnetograms - have been used as a proxy of the entire
solar-surface - distribution of the photospheric magnetic field.
- Because of the differential rotation of
magnetic - features, the synoptic charts actually cannot
cover entire - solar surface at any single time of solar
rotations, though - the large-scale photospheric magnetic field
might be - assumed to be time-independent in one solar
rotation - Ulrich and Boyden, 2006 Zhao et al., 2009.
3- To correct the synoptic charts for the effect
of - the differential rotation and construct the
- "snapshot heliographic map" or the "synchronic
- map" that covers entire solar surface at a
- specific time, a concept of "Carrington time" has
- been introduced to approximately estimate the
- time difference corresponding to two Carrington
- longitudes so that the effect of differential
rotation - can be estimated on the basis of the
differential - rotation formula (Ulrich and Boyden, 2006).
42. Rogers method and the variable synodic
rotation period of the Sun
- The Carrington time is measured in Carrington
rotation units, and for - a Carrington longitude, L, in Carrington
rotation number N, the - Carrington time may be simply calculated as
Tc1-L/360, and the time - difference from L1 to L2 can be calculated as
follows - dt (Tc2 -
Tc1)27.2753 (1) - Here 27.2753 days is the Carrington rotation
period, or the average of - the synodic rotation period. Because of the
eccentricity of the Earth's - orbit, the synodic rotation period of the Sun,
snp, varies from one - rotation to the next, can be estimated
- snp srp (Ve srp)/(Rse 2Pi/srp) srp
(Ve/Rse)(srp2/2PI), (2) - where srp denotes sidereal rotation period, 25.38
days, Rse the - Sun-Earth distance, Ve the Earths speed when the
Earth is located at - Rse.
5Figure 1. Synodic rotation period of Sun in
2008. The maximum and minimum are 27.34 and
27.20 days, occurred near winter and summer
solstices.
6- Figure 1, which is calculated on the basis
of - the date of commencement of each Carrington
- rotation from CR2065 to CR2079 (See
- Astronomical Almanac 2008), shows the variation
- of the synodic rotation period between
- 2007.12.29.05 and 2009.01.13.94. It shows that
- the maximum and minimum synodic period
- occured around winter and summer solstice, it is
- consistent with the fact that the Earth moves in
- winter solstice faster than in summer solstice
(see - Eqation (2).
73. Improved Rogers method
- By replacing the Carrington period with variable
synodic - periods, i.e.,
- dt (Tc2 - Tc1) snp (3)
- the calculated time difference is expected to be
more - accurate than that obtained using formula (1).
The - dashed blue line and solid blue curve in Figure 2
show the - results estimated by Eqs (1) and (3). The
maximum and - minimum time difference between Carrington
longitudes - of 150.550 and 190.505 degrees do occur at the
winter - and summer solstice, respectively.
8Figure 2. Comparison of different methods of
inverting Carrington longitude to central
meridian crossing time.
94. Iteration method
- The black curve in Figure 2 is obtained using the
- basic formula for calculating Carrington
longitude - from time and the iteration algorithm. The blue
- curve matches the black curve better than the
blue - dashed line. Figure 3 shows results of iteration
- method using different code black is xuepus
code, - and green is suninfo. The difference between
- black and green is slight, though the computation
- time using xuepus code is significantly smaller
than - the suninfo in IDL system.
10Figure 4. Comparison of results from different
method.
11Figure 2. Comparison of different methods of
inverting Carrington longitude to central
meridian crossing time.