October 1968 lunar eclipse explained
bgcolor=#e7dcc3 colspan=2 | Total lunar eclipse October 6, 1968 |
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(No photo) |
The moon passes west to east (right to left) across the Earth's umbral shadow, shown in hourly intervals. |
align=center bgcolor=#c0d0e0 | Series | 136 (17 of 72) |
align=center bgcolor=#c0d0e0 | Gamma | 0.36054 |
align=center bgcolor=#c0d0e0 | Magnitude | 1.16913 |
align=center bgcolor=#c0b0e0 colspan=2 | Duration (hr:mn:sc) |
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align=center bgcolor=#b0a0e0 | Totality | 01h02m58.1s |
align=center bgcolor=#c0a0e0 | Partial | 03h33m57.9s |
align=center bgcolor=#d0d0e0 | Penumbral | 05h52m07.1s |
align=center bgcolor=#a0d0e0 colspan=2 | Contacts (UTC) |
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align=center bgcolor=#d0d0e0 | P1 | 08:45:55.0 |
align=center bgcolor=#c0a0e0 | U1 | 09:54:55.4 |
align=center bgcolor=#b0a0e0 | U2 | 11:10:25.7 |
align=center bgcolor=#a0a0e0 | Greatest | 11:41:56.0 |
align=center bgcolor=#b0a0e0 | U3 | 12:13:23.8 |
align=center bgcolor=#c0a0e0 | U4 | 13:28:53.3 |
align=center bgcolor=#d0d0e0 | P4 | 14:38:02.1 | |
A total
lunar eclipse took place on Sunday, October 6, 1968, the second of two total eclipses in 1968, the first was on
April 13, 1968. The tables below contain detailed predictions and additional information on the total lunar eclipse of October 6, 1968.
! colspan=2 align=center bgcolor=white | Eclipse characteristics |
Parameter | Value |
Penumbral magnitude | 2.22423 |
Umbral magnitude | 1.16913 |
Gamma | 0.36054 |
Epilson | 0.3345º | |
! colspan=3 align=center bgcolor=white | Opposition times |
Event | Calendar date & time | Julian date |
Greatest eclipse | 1968 Oct 06 at 11:42:35.0 TD (11:41:56.0 UT1) | 2440135.987453 |
Ecliptic opposition | 1968 Oct 06 at 11:46:44.1 TD (11:46:05.2 UT1) | 2440135.990337 |
Equatorial opposition | 1968 Oct 06 at 12:05:11.4 TD (12:04:32.4 UT1) | 2440136.003153 | |
! colspan=3 align=center bgcolor=white | Geocentric coordinates of Sun and Moon |
! colspan=3 align=center bgcolor=white | 1968 Oct 06 at 11:42:35.0 TD (11:41:56.0 UT1) |
Coordinate | Sun | Moon |
Right ascension | 12h48m51.9s | 00h48m13.3s |
Declination | -05°14'36.0" | +05°32'13.0" |
Semi-diameter | 16'00.2" | 15'10.1" |
Eq. hor. parallax | 08.8" | 0°55'39.9" | |
! colspan=2 align=center bgcolor=white | Geocentric libration of Moon |
Angle | Value |
l | 4.6° |
b | -0.4° |
c | -21.4° | |
! colspan=2 align=center bgcolor=white | Earth's shadows |
Parameter | Value |
Penumbral radius | 1.2062° |
Umbral radius | 0.6728° | |
! colspan=2 align=center bgcolor=white | Prediction parameters |
Parameter | Value |
Ephemerides | JPL DE406 |
ΔT | 39.0 s |
Shadow rule | Danjon |
Shadow enlargement | 1.010 |
Saros series | 136 (17/72) | |
Visibility
It was completely visible over Asia, Australia, and North America, seen rising over central Asia, and setting over central North America.
Related lunar eclipses
Saros series
It was part of Saros series 136.
Tritos series
Tzolkinex
Half-Saros cycle
A lunar eclipse will be preceded and followed by solar eclipses by 9 years and 5.5 days (a half saros).[1] This lunar eclipse is related to two total solar eclipses of Solar Saros 143.
See also
Notes and References
- Mathematical Astronomy Morsels, Jean Meeus, p.110, Chapter 18, The half-saros