{"id":64,"date":"2018-08-15T16:59:06","date_gmt":"2018-08-15T20:59:06","guid":{"rendered":"https:\/\/people.bsu.edu\/rberring\/?page_id=64"},"modified":"2021-01-24T22:33:36","modified_gmt":"2021-01-25T03:33:36","slug":"nsvs-3792718","status":"publish","type":"page","link":"https:\/\/people.bsu.edu\/rberring\/variable_star_research\/nsvs-3792718\/","title":{"rendered":"NSVS 3792718"},"content":{"rendered":"<p>&nbsp;<\/p>\n<table style=\"width: 100%\">\n<tbody>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\">Researcher: <a href=\"https:\/\/people.bsu.edu\/rberring\/people\/alec-neal\/\">Alec Neal<\/a><\/p>\n<p>Observations suggest that NSVS 3792718 is an eclipsing variable star of W Ursae Majoris type. This star is located at <a href=\"http:\/\/simbad.u-strasbg.fr\/simbad\/sim-basic?Ident=nsvs+3792718&amp;submit=SIMBAD+search\">\u03b1=00:50:46.7 \u03b4=+41:50:15.4<\/a> and has the following alternate stellar designations: \u00a0<a href=\"http:\/\/cds.u-strasbg.fr\/cgi-bin\/Dic-Simbad?2MASS\">2MASS<\/a> J00504670+4150154, <a href=\"http:\/\/cds.u-strasbg.fr\/cgi-bin\/Dic-Simbad?CRTS\">CRTS<\/a> J005046.7+415015, <a href=\"http:\/\/cds.u-strasbg.fr\/cgi-bin\/Dic-Simbad?%5bGGM2006%5d\">[GGM2006]<\/a> 3792717. \u00a0Star field with the target star and comparison stars used in ensemble differential photometry are shown in Figure 1.<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\"><img decoding=\"async\" class=\"alignright size-full wp-image-65\" src=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2018\/08\/10094328\/9.23.2015_V.jpg\" alt=\"Star Field\" width=\"50%\" srcset=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2018\/08\/10094328\/9.23.2015_V.jpg 1254w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2018\/08\/10094328\/9.23.2015_V-150x150.jpg 150w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2018\/08\/10094328\/9.23.2015_V-297x300.jpg 297w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2018\/08\/10094328\/9.23.2015_V-768x775.jpg 768w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2018\/08\/10094328\/9.23.2015_V-1014x1024.jpg 1014w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2018\/08\/10094328\/9.23.2015_V-891x900.jpg 891w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2018\/08\/10094328\/9.23.2015_V-396x400.jpg 396w\" sizes=\"(max-width: 1254px) 100vw, 1254px\" \/><\/p>\n<p style=\"line-height: 1.3\"><span style=\"font-size: medium\"><strong>Figure 1:<\/strong> Star field with ensemble stars used for differential photometry marked. The variable star NSVS 3792718 is marked by the green target (T1). All ensemble stars are marked by the red apertures and designated the labels C2-C12. If a B band magnitude is known, it is given with each comparison. Field scale is given along the top and on the left side of the image. Image is a representative image taken with the BSUO 20-inch telescope. Further details for each comparison star are given below in Table 1. Further details regarding the telescope and detector used can be found on our <a href=\"https:\/\/people.bsu.edu\/rberring\/observing-facilities\/\">BSU Observatory page<\/a>.<\/span><\/p>\n<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 95%;border: 1px solid white\">\n<table style=\"width: 95%;text-align: center\">\n<tbody>\n<tr>\n<th style=\"width: 10%;border: 0px solid white;text-align: center\"><\/th>\n<th style=\"width: 20%;border: 0px solid white;text-align: center\">Identification<\/th>\n<th style=\"width: 30%;border: 0px solid white;text-align: center\" colspan=\"2\">Position (J2000.0)<\/th>\n<th style=\"width: 35%;border: 0px solid white;text-align: center\" colspan=\"3\">Magnitudes<\/th>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<th style=\"width: 10%;border: 0px solid white;text-align: right\"><strong>ID<\/strong><\/th>\n<th style=\"width: 20%;border: 0px solid white;text-align: center\"><strong>Catalog<\/strong><\/th>\n<th style=\"width: 15%;border: 0px solid white;text-align: center\"><strong>\u03b1<\/strong><\/th>\n<th style=\"width: 15%;border: 0px solid white;text-align: center\"><strong>\u03b4<\/strong><\/th>\n<th style=\"width: 15%;border: 0px solid white;text-align: center\"><strong>V<\/strong><\/th>\n<th style=\"width: 15%;border: 0px solid white;text-align: center\"><strong>B<\/strong><\/th>\n<th style=\"width: 5%;border: 0px solid white;text-align: center\"><strong>R<sub>c<\/sub><\/strong><\/th>\n<\/tr>\n<tr>\n<td style=\"width: 10%;border: 0px solid white;text-align: right\">C2<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><a href=\"http:\/\/simbad.u-strasbg.fr\/simbad\/sim-id?Ident=TYC+2806-966-1&amp;NbIdent=1&amp;Radius=2&amp;Radius.unit=arcmin&amp;submit=submit+id\">TYC 2806-966-1<\/a><\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">00:50:57.21<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">+41:50:29.60<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">11.43 \u00b1 0.09<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.25 \u00b1 0.15<\/td>\n<td style=\"width: 5%;border: 0px solid white;text-align: center\">\u2014<\/td>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 10%;border: 0px solid white;text-align: right\">C3<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><a href=\"http:\/\/simbad.u-strasbg.fr\/simbad\/sim-id?Ident=TYC+2806-586-1&amp;NbIdent=1&amp;Radius=2&amp;Radius.unit=arcmin&amp;submit=submit+id\">TYC 2806-586-1<\/a><\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">00:50:43.70<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">+41:53:04.42<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">11.78 \u00b1 0.13<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.60 \u00b1 0.20<\/td>\n<td style=\"width: 5%;border: 0px solid white;text-align: center\">\u2014<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 10%;border: 0px solid white;text-align: right\">C4<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><a href=\"http:\/\/simbad.u-strasbg.fr\/simbad\/sim-id?Ident=TYC+2805-916-1&amp;submit=submit+id\">TYC 2805-916-1<\/a><\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">00:49:49.51<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">+41:49:09.72<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">10.91 \u00b1 0.06<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.29 \u00b1 0.18<\/td>\n<td style=\"width: 5%;border: 0px solid white;text-align: center\">\u2014<\/td>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 10%;border: 0px solid white;text-align: right\">C5<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><a href=\"http:\/\/simbad.u-strasbg.fr\/simbad\/sim-id?Ident=TYC+2806-852-1&amp;submit=submit+id\">TYC 2806-852-1<\/a><\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">00:50:12.86<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">+42:00:00.96<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.37 \u00b1 0.17<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.27 \u00b1 0.12<\/td>\n<td style=\"width: 5%;border: 0px solid white;text-align: center\">\u2014<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 10%;border: 0px solid white;text-align: right\">C6<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><a href=\"http:\/\/simbad.u-strasbg.fr\/simbad\/sim-id?Ident=TYC+2806-26-1&amp;submit=submit+id\">TYC 2806-26-1<\/a><\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">00:50:20.29<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">+41:37:49.01<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">11.48 \u00b1 0.08<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.08 \u00b1 0.11<\/td>\n<td style=\"width: 5%;border: 0px solid white;text-align: center\">\u2014<\/td>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 10%;border: 0px solid white;text-align: right\">C7<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><a href=\"http:\/\/simbad.u-strasbg.fr\/simbad\/sim-id?Ident=TYC+2806-260-1&amp;submit=submit+id\">TYC 2806-260-1<\/a><\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">00:51:27.73<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">+41:39:56.88<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">11.36 \u00b1 0.08<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.35 \u00b1 0.17<\/td>\n<td style=\"width: 5%;border: 0px solid white;text-align: center\">\u2014<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 10%;border: 0px solid white;text-align: right\">C8<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><a href=\"http:\/\/simbad.u-strasbg.fr\/simbad\/sim-id?Ident=TYC+2806-742-1&amp;submit=submit+id\">TYC 2806-742-1<\/a><\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">00:51:40.03<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">+41:42:43.93<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.04 \u00b1 0.15<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.51 \u00b1 0.18<\/td>\n<td style=\"width: 5%;border: 0px solid white;text-align: center\">\u2014<\/td>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 10%;border: 0px solid white;text-align: right\">C9<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><a href=\"http:\/\/simbad.u-strasbg.fr\/simbad\/sim-id?Ident=TYC+2806-150-1&amp;submit=submit+id\">TYC 2806-150-1<\/a><\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">00:51:08.59<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">+41:44:27.88<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.58 \u00b1 0.19<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.96 \u00b1 0.23<\/td>\n<td style=\"width: 5%;border: 0px solid white;text-align: center\">\u2014<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 10%;border: 0px solid white;text-align: right\">C10<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><a href=\"http:\/\/simbad.u-strasbg.fr\/simbad\/sim-id?Ident=TYC+2806-691-1&amp;submit=submit+id\">TYC 2806-691-1<\/a><\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">00:51:27.59<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">+41:37:57.65<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">11.58 \u00b1 0.10<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.31 \u00b1 0.15<\/td>\n<td style=\"width: 5%;border: 0px solid white;text-align: center\">\u2014<\/td>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 10%;border: 0px solid white;text-align: right\">C11<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><a href=\"http:\/\/simbad.u-strasbg.fr\/simbad\/sim-id?Ident=TYC+2805-38-1&amp;submit=submit+id\">TYC 2805-38-1<\/a><\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">00:49:47.69<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">+41:44:59.38<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.09 \u00b1 0.14<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.60 \u00b1 0.18<\/td>\n<td style=\"width: 5%;border: 0px solid white;text-align: center\">\u2014<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 10%;border: 0px solid white;text-align: right\">C12<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><a href=\"http:\/\/simbad.u-strasbg.fr\/simbad\/sim-id?Ident=TYC+2805-1503-1&amp;submit=submit+id\">TYC 2805-1503-1<\/a><\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">00:49:27.27<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">+41:37:06.74<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.02 \u00b1 0.14<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">12.77 \u00b1 0.19<\/td>\n<td style=\"width: 5%;border: 0px solid white;text-align: center\">\u2014<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p><!-- end table for comparison list data--><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\">\n<p style=\"line-height: 1.3\"><span style=\"font-size: medium\"><strong>Table 1:<\/strong> List of comparison stars used in differential ensemble photometry analysis. First column gives the comparison designation. Columns 2 &amp; 3 give the Right Ascension (\u03b1) and Declination (\u03b4) of the comparison in J2000.0. Columns 3-6 report measured Johnson B (B), Johnson V (V) and Cousins R (R<sub>c<\/sub>) band magnitudes. Magnitudes are used to calibrate the magnitudes of the target star. Calibrated magnitudes are used to determine magnitudes in the Johnson-Cousins system.<\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-532\" src=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18012553\/NSVS_3792718_obnights.png\" alt=\"\" width=\"1920\" height=\"521\" srcset=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18012553\/NSVS_3792718_obnights.png 1920w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18012553\/NSVS_3792718_obnights-300x81.png 300w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18012553\/NSVS_3792718_obnights-1024x278.png 1024w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18012553\/NSVS_3792718_obnights-768x208.png 768w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18012553\/NSVS_3792718_obnights-1536x417.png 1536w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18012553\/NSVS_3792718_obnights-1000x271.png 1000w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18012553\/NSVS_3792718_obnights-1400x380.png 1400w\" sizes=\"auto, (max-width: 1920px) 100vw, 1920px\" \/><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\">We have observed this star with the Ball State University Observatory (BSUO) 20-inch (0.5m) telescope in the B, V, and\u00a0R<sub>c<\/sub> band passes. \u00a0All stellar photometry is performed by the <a href=\"http:\/\/www.astro.louisville.edu\/software\/astroimagej\/\">AstroImageJ (AIJ) software package<\/a>. \u00a0All photometry is performed with similar ensemble stars. \u00a0If a calibrated magnitude for a comparison star is known, then it is used by AIJ to calibrate the magnitude for the target star. \u00a0Folded light curves for Johnson V and (B-V) color are shown in <strong>Figure<\/strong> <strong>2<\/strong>.<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\"><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter wp-image-568 \" src=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022719\/NSVS3792718_colortemp.png\" alt=\"\" width=\"1231\" height=\"1458\" srcset=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022719\/NSVS3792718_colortemp.png 1612w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022719\/NSVS3792718_colortemp-253x300.png 253w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022719\/NSVS3792718_colortemp-865x1024.png 865w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022719\/NSVS3792718_colortemp-768x909.png 768w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022719\/NSVS3792718_colortemp-1297x1536.png 1297w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022719\/NSVS3792718_colortemp-760x900.png 760w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022719\/NSVS3792718_colortemp-338x400.png 338w\" sizes=\"auto, (max-width: 1231px) 100vw, 1231px\" \/><\/p>\n<p style=\"line-height: 1.5\"><span style=\"font-size: medium\"><strong>Figure 2:<\/strong> Folded color light curve for NSVS 3792718. All photometry is differential multi-aperture photometry performed by the AstroImageJ (AIJ) software package. Top panel shows folded V-band curve. Bottom panel shows folded (B-V) color curve. All magnitudes are calibrated by the known magnitudes of the ensemble stars. Error bars are not shown for clarity.<br \/>\nBy analyzing the B-V at quadrature (\u03a6 = \u00b1 0.25) and accounting for interstellar reddening (Av=0.181), the color index of the system was determined to be (B-V)<sub>0<\/sub> = 0.463 \u00b1 0.067, corresponding to a primary star surface temperature of 6439 \u00b1 288 K, and a spectral type of about <a href=\"http:\/\/articles.adsabs.harvard.edu\/\/full\/1970A%26A.....4..234F\/0000236.000.html\">F6<\/a> V. This temperature was calculated using the polynomial coefficients given in <a href=\"http:\/\/articles.adsabs.harvard.edu\/\/full\/1996ApJ...469..355F\/0000363.000.html\">Flower 1996<\/a>.<\/span><\/p>\n<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\" bgcolor=\"#BA0C2F\">\n<h3 style=\"width: 100%;text-align: center\"><span style=\"color: #ffffff\">Observed Minus Calculated (O-C) Time of Minimum Analysis<\/span><\/h3>\n<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\">Times of minimum light were determined for the nights observed, and are given in the following table along with Observed minus calculated (O-C) times of minimum. All reported errors are 1\u03c3 error bars.<br \/>\n<!-- begin table for times of minimum data--><\/p>\n<table class=\" aligncenter\" style=\"width: 70%;text-align: center\">\n<tbody>\n<tr>\n<th style=\"width: 52%;border: 0px solid white;text-align: center\" colspan=\"2\">[HJD]<\/th>\n<th style=\"width: 8%;border: 0px solid white;text-align: center\"><\/th>\n<th style=\"width: 40%;border: 0px solid white;text-align: center\" colspan=\"2\">[days]<\/th>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<th style=\"width: 32%;border: 0px solid white;text-align: right\">Time of Minimum<\/th>\n<th style=\"width: 20%;border: 0px solid white;text-align: left\">Error<\/th>\n<th style=\"width: 8%;border: 0px solid white;text-align: center\">Eclipse<\/th>\n<th style=\"width: 20%;border: 0px solid white;text-align: right\">(O-C)<\/th>\n<th style=\"width: 20%;border: 0px solid white;text-align: left\">Error<\/th>\n<\/tr>\n<tr>\n<td style=\"width: 32%;border: 0px solid white;text-align: right\">2457288.80898<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: left\">\u00b1 0.00024<\/td>\n<td style=\"width: 8%;border: 0px solid white;text-align: center\">primary<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: right\">0<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: left\">\u00b1 0.00024<\/td>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 32%;border: 0px solid white;text-align: right\">2457287.71474<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: left\">\u00b1 0.00022<\/td>\n<td style=\"width: 8%;border: 0px solid white;text-align: center\">secondary<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: right\">0.00124<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: left\">\u00b1 0.00034<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 32%;border: 0px solid white;text-align: right\">2457313.78437<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: left\">\u00b1 0.00024<\/td>\n<td style=\"width: 8%;border: 0px solid white;text-align: center\">primary<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: right\">-0.00139<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: left\">\u00b1 0.00032<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p><!-- end table for times of minimum data--><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\">&nbsp;<\/p>\n<p style=\"line-height: 1.3\"><span style=\"font-size: medium\"><strong>Table 2:<\/strong> Heliocentric Julian dates [HJD] for times of minimum (<em>first column<\/em>) are reported along with 1\u03c3 errors bars (<em>second column<\/em>). All times of minimum light are first determined for each filter (B, V, and R) light curve, and are determined by the method described by Kwee &amp; van Woorden (1976). Similar times of minimum for differing filter light curves are averaged together and reported in column <strong>Times of Minimum<\/strong>. Eclipses are designated by <em>primary<\/em> for the primary eclipse and <em>secondary<\/em> for the secondary eclipse in the <strong>Eclipse<\/strong> column (<em>third\/middle column<\/em>). Values of <strong>(O-C)<\/strong> (<em>fourth column<\/em>) are given in units of days along with 1\u03c3 errors (<em>fifth column<\/em>).<\/span><\/p>\n<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\">An observed minus calculated (O-C) time of minimum light analysis was performed and is shown in <strong>Figure 3<\/strong>. The analysis was performed using the reported times of minimum light given in table 2. The O-C values are determined by the following linear ephemeris and are given in the above table.<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\"><!-- begin table for ephemeris--><\/p>\n<table style=\"width: 100%;text-align: center\">\n<tbody>\n<tr>\n<td style=\"width: 25%;border: 1px solid white;text-align: right\">T<sub>min<\/sub> [HJD] =<\/td>\n<td style=\"width: 20%;border: 1px solid white;text-align: center\">2457288.808977<\/td>\n<td style=\"width: 5%;border: 1px solid white;text-align: left\">+<\/td>\n<td style=\"width: 20%;border: 1px solid white;text-align: left\">0.438189<\/td>\n<td style=\"width: 10%;border: 1px solid white;text-align: left\">\u00b7 E<\/td>\n<td style=\"width: 20%;border: 1px solid white;text-align: left\">(1)<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 25%;border: 1px solid white;text-align: right\"><\/td>\n<td style=\"width: 20%;border: 1px solid white;text-align: center\">\u00b10.000236<\/td>\n<td style=\"width: 5%;border: 1px solid white;text-align: left\"><\/td>\n<td style=\"width: 20%;border: 1px solid white;text-align: left\">\u00b10.000706<\/td>\n<td style=\"width: 10%;border: 1px solid white;text-align: left\"><\/td>\n<td style=\"width: 20%;border: 1px solid white;text-align: left\"><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p><!-- end table for ephemeris--><img decoding=\"async\" class=\"aligncenter\" title=\"NSVS_3792718_ephemeris\" src=\"https:\/\/latex.codecogs.com\/svg.latex?\\begin{align*}&amp;space;T_{\\textup{min}}[\\textup{HJD}]&amp;space;&amp;=2457288.808977&amp;plus;0.438189\\times&amp;space;E\\\\&amp;space;&amp;&amp;space;\\;\\;\\;\\;\\pm&amp;space;0.000236&amp;space;\\;\\;\\;\\;\\;\\;\\;\\;\\pm&amp;space;0.000236&amp;space;\\end{align}&amp;space;\\indent\\indent\\indent\\indent\\indent\\indent\\indent\\indent(1)\" \/><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 50%;border: 1px solid white\"><img decoding=\"async\" class=\"wp-image-328 alignleft\" src=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/04\/01170432\/NSVS_3792718_oc.png\" alt=\"NSVS 3792718 Observed minus Calculated\" width=\"50%\" srcset=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/04\/01170432\/NSVS_3792718_oc.png 2299w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/04\/01170432\/NSVS_3792718_oc-300x156.png 300w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/04\/01170432\/NSVS_3792718_oc-768x398.png 768w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/04\/01170432\/NSVS_3792718_oc-1024x531.png 1024w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/04\/01170432\/NSVS_3792718_oc-1000x518.png 1000w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/04\/01170432\/NSVS_3792718_oc-771x400.png 771w\" sizes=\"(max-width: 2299px) 100vw, 2299px\" \/><\/p>\n<p style=\"line-height: 1.3\"><span style=\"font-size: medium\"><strong>Figure 3:<\/strong> Observed time of minimum minus calculated time of minimum (O-C) plot with best-fit linear linear line (solid line) versus epoch number (E). Error bars are 1\u03c3 error bars assuming the period of the system is known with out errors. All O-C values are given in units of days and are determined by the linear ephemeris given in equation (1). Best-fit linear line is determined by an unweighted linear least squares analysis. Slope of best-fit line represents a negligible correction to the ephemeris given in equation (1).<\/span><\/p>\n<p>&nbsp;<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\" bgcolor=\"#BA0C2F\">\n<h3 style=\"width: 100%;text-align: center\"><span style=\"color: #ffffff\">Best fitting Wilson-Devinney (WD) Models<\/span><\/h3>\n<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\">All modeling is performed using the <a href=\"http:\/\/phoebe-project.org\/\">PHysics Of Eclipsing BinariEs (PHOEBE)<\/a> (v0.31a) software package. \u00a0PHOEBE is a graphical user interface (gui) to the <a href=\"ftp:\/\/ftp.astro.ufl.edu\/pub\/wilson\">WD code<\/a> that is used to model binary stars. \u00a0Figure 4 shows the best fit WD model. \u00a0No spots were included in the best-fit model. Figure 5 shows a graphical representation of the stellar surface.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter wp-image-569 size-full\" src=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022818\/NSVS3792718_LCs.png\" alt=\"\" width=\"3667\" height=\"4427\" srcset=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022818\/NSVS3792718_LCs.png 3667w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022818\/NSVS3792718_LCs-248x300.png 248w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022818\/NSVS3792718_LCs-848x1024.png 848w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022818\/NSVS3792718_LCs-768x927.png 768w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022818\/NSVS3792718_LCs-1272x1536.png 1272w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022818\/NSVS3792718_LCs-1696x2048.png 1696w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022818\/NSVS3792718_LCs-745x900.png 745w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/12\/10022818\/NSVS3792718_LCs-331x400.png 331w\" sizes=\"auto, (max-width: 3667px) 100vw, 3667px\" \/><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white\"><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter wp-image-465 size-full\" src=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/12\/20001534\/NSVS_3792718_LC_collage2.png\" alt=\"\" width=\"2250\" height=\"750\" srcset=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/12\/20001534\/NSVS_3792718_LC_collage2.png 2250w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/12\/20001534\/NSVS_3792718_LC_collage2-300x100.png 300w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/12\/20001534\/NSVS_3792718_LC_collage2-1024x341.png 1024w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/12\/20001534\/NSVS_3792718_LC_collage2-768x256.png 768w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/12\/20001534\/NSVS_3792718_LC_collage2-1536x512.png 1536w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/12\/20001534\/NSVS_3792718_LC_collage2-2048x683.png 2048w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/12\/20001534\/NSVS_3792718_LC_collage2-1000x333.png 1000w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/12\/20001534\/NSVS_3792718_LC_collage2-1200x400.png 1200w\" sizes=\"auto, (max-width: 2250px) 100vw, 2250px\" \/><\/p>\n<p><strong>Figure 4:<\/strong> Best-fit WD model fit with no spots (<em>red solid curve<\/em>) to the folded light curve for differential Johnson B (<em>left panel<\/em>), V (<em>center\/middle panel<\/em>), and Cousins R (<em>right panel<\/em>) band magnitudes.\u00a0 In each panel the top panel shows the folded light curve for B, V, or R bands, and the bottom panel shows the deviation of the observed values from the best-fit WD model.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter wp-image-538\" src=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18220642\/NSVS_3792718_BVR-comphalf.png\" alt=\"\" width=\"980\" height=\"1396\" srcset=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18220642\/NSVS_3792718_BVR-comphalf.png 2950w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18220642\/NSVS_3792718_BVR-comphalf-211x300.png 211w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18220642\/NSVS_3792718_BVR-comphalf-719x1024.png 719w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18220642\/NSVS_3792718_BVR-comphalf-768x1094.png 768w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18220642\/NSVS_3792718_BVR-comphalf-1078x1536.png 1078w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18220642\/NSVS_3792718_BVR-comphalf-1438x2048.png 1438w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18220642\/NSVS_3792718_BVR-comphalf-632x900.png 632w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/08\/18220642\/NSVS_3792718_BVR-comphalf-281x400.png 281w\" sizes=\"auto, (max-width: 980px) 100vw, 980px\" \/><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 70%;border: 1px solid white\"><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter wp-image-578 size-full\" src=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2021\/01\/24221802\/NSVS_3792718_supercollage.png\" alt=\"\" width=\"4812\" height=\"4689\" srcset=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2021\/01\/24221802\/NSVS_3792718_supercollage.png 4812w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2021\/01\/24221802\/NSVS_3792718_supercollage-300x292.png 300w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2021\/01\/24221802\/NSVS_3792718_supercollage-1024x998.png 1024w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2021\/01\/24221802\/NSVS_3792718_supercollage-768x748.png 768w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2021\/01\/24221802\/NSVS_3792718_supercollage-1536x1497.png 1536w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2021\/01\/24221802\/NSVS_3792718_supercollage-2048x1996.png 2048w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2021\/01\/24221802\/NSVS_3792718_supercollage-924x900.png 924w, https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2021\/01\/24221802\/NSVS_3792718_supercollage-410x400.png 410w\" sizes=\"auto, (max-width: 4812px) 100vw, 4812px\" \/><\/p>\n<p><strong>Figure 5:<\/strong> Stellar visualizations showing best-fit stellar models for the light curves shown in Figure 4. The phases show the system through the first half of the orbit.\u00a0 Because of the symmetry, these phases represent mirror images of the other half (-\u03a6). Spots were not used for the final best-fit model. The diagram was plotted by applying the star&#8217;s best-fit mass ratio, inclination, and surface potential, given in Table 3 below, to the standard Roche model for close binaries.<\/p>\n<p>Below is a cool animation of NSVS 3792718 created by Alec Neal that helps to visualize the orbit of the system as viewed from the Earth.\u00a0 The animation was created by the <a href=\"https:\/\/ezgif.com\/\">EZGif Animated Gif Maker<\/a>.\u00a0 Orbital phase is given at the bottom of the frame.<\/p>\n<p><img decoding=\"async\" class=\"aligncenter wp-image-334 size-full\" title=\"NSVS3792718_animation_12fps\" src=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/04\/15170537\/12fps_phi_name.gif\" alt=\"\" width=\"60%\" \/><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>&nbsp;<\/p>\n<table style=\"width: 100%;text-align: center;border: 1px solid white\">\n<tbody>\n<tr>\n<td style=\"border: 1px solid white\" bgcolor=\"#BA0C2F\">\n<h5 style=\"width: 100%;text-align: center\"><span style=\"color: #ffffff\"><strong>Best-fit Model Parameters<\/strong><\/span><\/h5>\n<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;border: 1px solid white;text-align: left\">Below is a table of parameters and their values derived in the analysis of this system via the methods discussed above.<\/p>\n<p><!-- begin table for parameter data--><\/p>\n<table class=\"aligncenter\" style=\"width: 100%;text-align: center\">\n<tbody>\n<tr>\n<th style=\"width: 30%;border: 0px solid white;text-align: center\">(1)<\/th>\n<th style=\"width: 20%;border: 0px solid white;text-align: center\">(2)<\/th>\n<th style=\"width: 30%;border: 0px solid white;text-align: center\">(3)<\/th>\n<th style=\"width: 20%;border: 0px solid white;text-align: center\">(4)<\/th>\n<\/tr>\n<tr>\n<th style=\"width: 30%;border-bottom: 1px solid #000000;text-align: center\"><strong>Parameter<\/strong><\/th>\n<th style=\"width: 20%;border-bottom: 1px solid #000000;text-align: center\"><strong>Symbol [unit]<\/strong><\/th>\n<th style=\"width: 30%;border-bottom: 1px solid #000000;text-align: center\"><strong>Value<\/strong><\/th>\n<th style=\"width: 20%;border-bottom: 1px solid #000000;text-align: center\"><strong>Error<\/strong><\/th>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\">Period<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">P [days]<\/td>\n<td style=\"width: 30%;border: 0px solid white;text-align: center\">0.438168<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">0.000147<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\">Epoch<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">T<sub>0<\/sub> [HJD]<\/td>\n<td style=\"width: 30%;border: 0px solid white;text-align: center\">2457288.809054<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">0.000330<\/td>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\">Inclination<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><em>i<\/em> [\u00b0]<\/td>\n<td style=\"width: 30%;border: 0px solid white;text-align: center\">80.61<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">0.07<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\">Surface Temp.<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><em>T<\/em><sub>eff,1<\/sub> [K]<\/td>\n<td style=\"width: 30%;border: 0px solid white;text-align: center\">6498<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">77<\/td>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\"><\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><em>T<\/em><sub>eff,2<\/sub> [K]<\/td>\n<td style=\"width: 30%;border: 0px solid white;text-align: center\">6340<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">77<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\">Surface Potential<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">\u03a9<sub>1,2<\/sub> [-]<\/td>\n<td style=\"width: 30%;border: 0px solid white;text-align: center\">2.35<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">0.02<\/td>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\">Mass Ratio<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">q [-]<\/td>\n<td style=\"width: 30%;border: 0px solid white;text-align: center\">0.269<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">0.011<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\">Distance<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\"><em>d<\/em> [pc]<\/td>\n<td style=\"width: 19%;border: 0px solid white;text-align: center\">820<\/td>\n<td style=\"width: 14%;border: 0px solid white;text-align: center\">86<\/td>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\">Filling Factor<\/td>\n<td style=\"width: 15%;border: 0px solid white;text-align: center\">F [-]<\/td>\n<td style=\"width: 19%;border: 0px solid white;text-align: center\">0.28<\/td>\n<td style=\"width: 14%;border: 0px solid white;text-align: center\">0.056<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\">Stellar Mass<sup>\u2021<\/sup><\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><em>M<\/em><sub>1<\/sub> [M<sub>\u2609<\/sub>]<\/td>\n<td style=\"width: 30%;border: 0px solid white;text-align: center\">1.31<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">0.09<\/td>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\"><\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><em>M<\/em><sub>2<\/sub> [M<sub>\u2609<\/sub>]<\/td>\n<td style=\"width: 30%;border: 0px solid white;text-align: center\">1.09<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">0.08<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\">Stellar Radius<sup>\u2021<\/sup><\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><em>R<\/em><sub>1<\/sub> [R<sub>\u2609<\/sub>]<\/td>\n<td style=\"width: 30%;border: 0px solid white;text-align: center\">1.36<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">0.10<\/td>\n<\/tr>\n<tr bgcolor=\"#eeeeee\">\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\"><\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><em>R<\/em><sub>2<\/sub> [R<sub>\u2609<\/sub>]<\/td>\n<td style=\"width: 30%;border: 0px solid white;text-align: center\">1.27<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">0.10<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 30%;border-right: 1px solid #000000;text-align: center\">Semi-major Axis<sup>\u2021<\/sup><\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\"><em>a<\/em> [R<sub>\u2609<\/sub>]<\/td>\n<td style=\"width: 30%;border: 0px solid white;text-align: center\">3.25<\/td>\n<td style=\"width: 20%;border: 0px solid white;text-align: center\">0.08<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p><strong>Table 3:<\/strong> System parameters of NSVS 3792718.\u00a0 Column (1) gives the name of the parameter, (2) gives the parameter symbol and [unit], (3) and (4) give the parameter value and error, respectively. Any blanks in the table denote data which is, as of the most recent entry, unknown and\/or unavailable.<br \/>\n<sup>\u2021<\/sup><em>These values were calculated using the the equations in <a href=\"http:\/\/articles.adsabs.harvard.edu\/cgi-bin\/nph-iarticle_query?1988BAICz..39..329H&amp;amp;data_type=PDF_HIGH&amp;amp;whole_paper=YES&amp;amp;type=PRINTER&amp;amp;filetype=.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Harmanec (1988)<\/a>. These equations assume our star(s) are main sequence, which is suspect. We only include the values as crude estimates, as spectral and radial velocity data will be required to obtain more certain values.<\/em><br \/>\n<!-- end table for parameter data--><\/td>\n<\/tr>\n<\/tbody>\n<p><!--parameters end--><!--presentations begin--><\/p>\n<tbody>\n<tr>\n<td style=\"border: 1px solid white\" bgcolor=\"#BA0C2F\">\n<h3 style=\"width: 100%;text-align: center\"><span style=\"color: #ffffff\"><strong>Presentations<\/strong><\/span><\/h3>\n<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;text-align: left;border: 1px solid white\">Poster presentations and talks given by <a href=\"https:\/\/people.bsu.edu\/rberring\/people\/alec-neal\/\">Alexander J. Neal (Alec Neal)<\/a> at national, regional and local conferences for NSVS 3792718 are given below.<\/p>\n<ol>\n<li><em>A Photometric Analysis of the Eclipsing Binary Star NSVS 3792718<\/em>, Ball State University Physics &amp; Astronomy Annual Banquet Poster Presentation, Spring 2018.<\/li>\n<li><a href=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/04\/18193559\/NSVS_3792718_dec2018_ppt.pdf\" target=\"_blank\" rel=\"noopener noreferrer\"><em>Eclipsing Variable Star NSVS 3792718<\/em><\/a>,\u00a0Ball State University Physics &amp; Astronomy colloquium, December, 2018.<\/li>\n<li><a href=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2019\/04\/22192929\/NSVS_3792718-a-Spotless-W-Ursae-Majoris-Star2.pdf\" target=\"_blank\" rel=\"noopener noreferrer\"><em>NSVS 3792718, a Spotless W Ursae Majoris Star<\/em><\/a>, Indiana Academy of Science 134th Annual Meeting, March 30, 2019.<\/li>\n<li><em>Multi-Band Photometric Study of the W Ursae Majoris Star NSVS 3792718<\/em>, Ball State University Student Symposium, April 9, 2019.<\/li>\n<li>(Mentioned)\u00a0<em>NSVS 2854398 and Recent\u00a0<\/em><i>Developments<\/i>, Physics &amp; Astronomy colloquium. November 21, 2019.<\/li>\n<\/ol>\n<h3 style=\"text-align: center\">Publications<\/h3>\n<ol>\n<li><a href=\"https:\/\/bsu-wpe-people.s3.amazonaws.com\/wp-content\/uploads\/sites\/5\/2020\/11\/18131213\/NSVS3792718_mainbody.pdf\">Rough draft<\/a>, updated November 18, 2020.<\/li>\n<\/ol>\n<\/td>\n<\/tr>\n<p><!--presentations end--><!--contact info begin--><\/p>\n<tr>\n<td style=\"border: 1px solid white\">\n<hr \/>\n<h4 style=\"width: 100%;text-align: center\"><span style=\"color: #000000\"><strong>Contact Information<\/strong><\/span><\/h4>\n<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 100%;text-align: left;border: 1px solid white\">All <a href=\"https:\/\/people.bsu.edu\/rberring\/main\/variable_star_research\/variable_star_team\/\">members of the Variable Star Research group<\/a> are enthusiastic researchers with a passion for the work performed by the group. We are always happy to discuss any research projects and are always looking for like-minded and enthusiastic collaborators. For more information regarding any of the aforementioned research activities or the <a href=\"https:\/\/people.bsu.edu\/rberring\/main\/variable_star_research\/\">research activities<\/a> of the <a href=\"https:\/\/people.bsu.edu\/rberring\/main\/variable_star_research\/variable_star_team\/\">Variable Star Research Group<\/a>, please do not hesitate to contact <a href=\"https:\/\/people.bsu.edu\/rberring\/people\/robert-berrington\/\">Robert Berrington<\/a>.<\/td>\n<\/tr>\n<p><!--contact info end--><!--end page--><\/tbody>\n<\/table>\n","protected":false},"excerpt":{"rendered":"<p>&nbsp; Researcher: Alec Neal Observations suggest that NSVS 3792718 is an eclipsing variable star of W Ursae Majoris type. This star is located at \u03b1=00:50:46.7 \u03b4=+41:50:15.4 and has the following alternate stellar designations: \u00a02MASS J00504670+4150154, CRTS J005046.7+415015, [GGM2006] 3792717. \u00a0Star field with the target star and comparison stars used in ensemble differential photometry are shown [&hellip;]<\/p>\n","protected":false},"author":7,"featured_media":382,"parent":2,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"template-page\/page-full-width.php","meta":{"footnotes":""},"class_list":["post-64","page","type-page","status-publish","has-post-thumbnail","hentry"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v28.4 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>NSVS 3792718 - Berrington Research Group<\/title>\n<meta name=\"description\" content=\"An eclipsing variable (binary) star of the W Ursae Majoris type with a period of 0.4382 days and a surface temp. of 6440 K approx. 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