SOL — Celestial Observatory

Sun, Moon, planets, and space weather from Mukilteo's latitude
47.9063°N 122.2816°W · Puget Sound · Salish Sea
The same Moon that Artemis II will fly behind rises over Possession Sound every night. The same Sun that powers the SLS solar arrays sets behind the Olympics from this latitude. SOL tracks the celestial mechanics that connect the sky above Mukilteo to the missions beyond it.

Moon Phase

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Illumination: -- Rise: -- Set: --
Sun & Moon
Live celestial data for 47.9°N

Day Cycle

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Rise: -- Set: -- Day: --

Daylight Progress

Dawn Sunrise Noon Sunset Dusk Now: --

Sun Today — March 31, 2026

Sunrise6:49 AM PDT
Solar Noon1:13 PM PDT
Sunset7:39 PM PDT
Day Length12h 52m
Civil Twilight6:18 AM – 8:09 PM
Nautical Twilight5:40 AM – 8:47 PM
Astronomical Twilight5:00 AM – 9:26 PM
Latitude Effect+3m 12s/day (gaining light)

Moon Today

PhaseWaxing Gibbous
Illumination98%
Next Full MoonApril 1, 7:12 PM PDT
Moonrise6:33 PM PDT
Moonset6:12 AM PDT
Distance~384,400 km

Space Weather

Kp Index2.0 (G0 — Quiet)
Aurora Risk (PNW)None
Solar Wind Speed404 km/s
Solar Wind Density2.8 p/cm³
Solar Wind Temp51,000 K
Solar CycleCycle 25 (ascending)
Static data

Artemis II — Lunar Connection

LaunchApril 1, 3:24 PM PDT
CountdownT-32h
Moon at LaunchFull Moon (100%)
Closest Approach6,513 km from far side
Orion Max Distance392,650 km from Earth
KSC WeatherClear, 25°C, GO
Live TrackerOpen Tracker →
Full Moon on Launch Day. Artemis II launches April 1 as the Moon reaches 100% illumination. The crew will fly behind the Moon 4 days later — by then, it will be a waning gibbous as seen from Earth, but the far side they pass will be in full sunlight. The same Moon rising tonight over Possession Sound is where they're going.

The Sun G2V main-sequence star, 4.6 billion years

Solar Basics

ParameterValue
Distance from Earth149,597,870.7 km (1 AU)
Light travel time8 minutes 19 seconds
Radius696,340 km (109 Earths)
Mass1.989 × 10³&sup0; kg (333,000 Earths)
Surface temperature5,778 K (5,505°C)
Core temperature~15,700,000 K
Luminosity3.828 × 10²&sup6; W
Spectral classG2V (yellow dwarf)
Rotation period~25.4 days (equator), ~34.4 days (poles)
Age4.603 billion years
Expected lifetime~10 billion years total

Solar Structure

LayerDepthTemperatureNotes
Core0 – 0.25 R~15.7 MKpp-chain fusion, 99% of energy output
Radiative Zone0.25 – 0.7 R7 – 2 MKPhoton random walk: ~170,000 years to cross
Tachocline~0.7 R~2 MKShear layer, origin of magnetic dynamo
Convective Zone0.7 – 1.0 R2 MK – 5,778 KConvection cells visible as granulation
PhotosphereSurface5,778 KVisible "surface," sunspots form here
Chromosphere+2,000 km~20,000 KVisible during eclipses as pink rim
Corona+millions km1 – 3 MKCoronal heating problem: hotter than surface

Solar Cycle 25

We are in Solar Cycle 25, which began December 2019. Solar maximum is expected 2025–2026, making this an active period for sunspots, solar flares, and coronal mass ejections. The Kp index measures geomagnetic disturbance driven by solar wind interaction with Earth's magnetosphere.

Kp 0–3: quiet. Kp 4: unsettled. Kp 5+ triggers aurora visible from Washington state. During Solar Cycle 25's peak, aurora has been visible from Mukilteo multiple times.

For Artemis II: Space weather affects crew radiation exposure and communications. The O2O optical system is less affected by solar radio interference than S-band. Current Kp 2.0 is benign.

Solar Cycle 25 Activity

Sunspot number tracks the 11-year solar magnetic cycle. Cycle 25 has exceeded initial predictions, with observed sunspot numbers consistently above the forecast curve since late 2023. The current ascending phase means increased flare probability and more frequent geomagnetic storms.

Sunspot number timeline — Cycle 24 (2008-2019) to Cycle 25 (2019-present)

Data source: NOAA SWPC · WDC-SILSO (Royal Observatory of Belgium)

Latitude 47.9°N — What the Sun Does Here

At Mukilteo's latitude, the day length swings from 8h 21m (winter solstice) to 16h 02m (summer solstice) — a 7h 41m range. Today (March 31) is just past the equinox, gaining ~3 minutes of daylight per day. The Sun reaches a maximum altitude of ~65° at summer solstice, never directly overhead.

The marine layer, Olympic rain shadow, and Cascade convergence zone all interact with solar heating to create Mukilteo's microclimate — fog burns off later here than 10 miles inland.

Solar Altitude Through the Year at 47.9°N

The Sun's maximum altitude at solar noon varies with the seasons due to Earth's 23.44° axial tilt:

DateEventNoon AltitudeDay Length
June 20Summer Solstice65.5°16h 02m
Mar 20 / Sep 22Equinoxes42.1°12h 10m
Dec 21Winter Solstice18.7°8h 21m

The low winter sun angle means solar panels at this latitude are most efficient tilted 40-50° from horizontal. The long summer days compensate for lower per-hour insolation, giving Mukilteo surprisingly good annual solar potential (~4.2 kWh/m²/day average).

The Moon 384,400 km mean distance

Lunar Basics

ParameterValue
Mean distance from Earth384,400 km (center-to-center)
Perigee (closest)~363,300 km
Apogee (farthest)~405,500 km
Light travel time1.282 seconds (one-way)
Radius1,737.4 km (0.273 Earths)
Mass7.342 × 10²² kg (1.2% Earth)
Surface gravity1.62 m/s² (16.5% Earth)
Orbital period (sidereal)27.322 days
Synodic month (phase cycle)29.531 days
Orbital eccentricity0.0549
Orbital inclination5.145° to ecliptic
Recession rate3.8 cm/year (moving away from Earth)

Lunar Surface Composition

FeatureCoverageCompositionAge
Highlands (terrae)~83% of surfaceAnorthosite (Ca-feldspar)4.4 – 4.0 Ga
Maria (dark plains)~17% of surfaceBasalt (Fe, Ti-rich)3.9 – 3.1 Ga
RegolithEntire surfacePulverized rock, 2–20 m deepOngoing
South Pole (Artemis III target)CratersWater ice in permanently shadowed regionsAncient

The far side that Artemis II will overfly has almost no maria — its crust is thicker, preventing magma from reaching the surface. The crew will see a dramatically different landscape from what is visible from Earth.

Tidal Locking & the Far Side

The Moon is tidally locked — it rotates exactly once per orbit, so the same face always points toward Earth. The far side (not "dark side" — it gets equal sunlight) was unseen by humans until Luna 3 photographed it in 1959, and unseen by human eyes until Apollo 8 in 1968.

Artemis II will fly 6,513 km above the far side surface, the first humans to see it directly since Apollo 17 in 1972. During the flyby, there will be a communication blackout — the Moon blocks line-of-sight to Earth. The crew will be on their own for approximately 30 minutes.

Moon & Tides at Mukilteo

Puget Sound experiences mixed semidiurnal tides — two highs and two lows per day, with unequal heights. The Moon's gravitational pull is the primary driver, with the Sun contributing ~46% as much tidal force. Spring tides (highest range) occur at full and new moon; neap tides at quarter phases.

Today's tides at Everett (Station 9447659): High 3.37m at 4:51 AM, Low 0.77m at 10:59 AM, High 3.01m at 5:04 PM, Low 0.72m at 10:57 PM. With the Moon nearly full, tidal range is near its spring maximum.

Live tide data →

Planets Visible Tonight

Evening Sky — March 31, 2026

From Mukilteo at 47.9°N, the evening sky after sunset (7:39 PM) offers:

PlanetVisibilityNotes
VenusMorning star (pre-dawn)Brightest object after Moon, low east before sunrise
MarsEvening, westIn Gemini, dimming as Earth moves away
JupiterEvening, west-southwestSetting earlier each night, in Taurus
SaturnNot visible (conjunction)Too close to Sun this month

Approximate visibility from 47.9°N latitude. Actual visibility depends on atmospheric conditions and obstructions. The nearly-full Moon will wash out fainter objects tonight.

All Planets — Current Positions

PlanetDistance from SunDistance from EarthMagnitudeConstellationStatus
Mercury0.39 AU~1.2 AU+0.5PiscesLost in twilight
Venus0.72 AU~1.4 AU-4.0AquariusMorning star, brilliant
Mars1.52 AU~1.6 AU+1.2GeminiEvening, fading
Jupiter5.20 AU~5.8 AU-2.1TaurusEvening, prominent
Saturn9.54 AU~10.4 AU+1.0PiscesSolar conjunction
Uranus19.19 AU~20.0 AU+5.8TaurusBinocular object, near Jupiter
Neptune30.07 AU~30.9 AU+7.9PiscesTelescope required

Distances and magnitudes are approximate for late March 2026. Inner planet positions change rapidly; outer planets shift slowly.

Celestial Mechanics — The Math Behind the Sky

Why the Moon Appears to Change Size

The Moon's orbit is elliptical (eccentricity 0.0549). At perigee (~363,300 km) its angular diameter is 33.5 arcminutes; at apogee (~405,500 km) it shrinks to 29.4 arcminutes — a 14% difference. "Supermoons" occur when full moon coincides with perigee.

Angular diameter formula: θ = 2 × arctan(R / d) ≈ 2R/d radians, where R = 1,737.4 km and d is the distance.

Synodic vs. Sidereal Month

The sidereal month (27.322 days) is the time for the Moon to orbit 360° relative to the stars. The synodic month (29.531 days) is the time between identical phases (e.g., full moon to full moon). The synodic month is longer because Earth has moved ~27° around the Sun during one lunar orbit, so the Moon needs ~2.2 extra days to "catch up" to the same Sun-Earth-Moon geometry.

Lagrange Points & the JWST Connection

The Sun-Earth system has five Lagrange points where gravitational and centripetal forces balance. L1 (sunward, 1.5M km) hosts DSCOVR/SOHO for solar monitoring. L2 (anti-sunward, 1.5M km) hosts JWST and Gaia. L4/L5 (60° ahead/behind Earth) collect Trojan dust.

The Earth-Moon system also has Lagrange points. Earth-Moon L2 (behind the far side) is where the Queqiao relay satellite operates for Chang'e missions. A future relay at EM-L2 could eliminate the communication blackout that Artemis II will experience during the far-side flyby.

Formula for L1/L2 distance: r ≈ R × (m2 / 3m1)1/3, where R is the orbital radius and m1, m2 are the two masses.

Sphere of Influence

The Moon's gravitational sphere of influence extends ~66,000 km from its center. Inside this boundary, the Moon's gravity dominates over Earth's for trajectory calculations. Artemis II enters this sphere on Day 3-4 outbound, and the free-return trajectory uses the Moon's gravity to redirect the spacecraft homeward without an engine burn.

Formula: rSOI = a × (mMoon/mEarth)2/5 = 384,400 × (0.0123)0.4 ≈ 66,183 km

Full worked examples →

Orbital Resonances in the Solar System

Orbital mechanics produces elegant integer ratios throughout the solar system. These resonances stabilize (or destabilize) orbits over millions of years:

BodiesRatioTypeEffect
Moon (rotation:orbit)1:1Spin-orbitTidal locking, same face to Earth
Mercury (rotation:orbit)3:2Spin-orbit3 rotations per 2 orbits
Io:Europa:Ganymede1:2:4LaplaceMutual tidal heating (Io volcanism)
Pluto:Neptune2:3Mean-motionPrevents close approaches
Jupiter:Saturn~2:5Near-resonanceGrand Tack migration theory

Data Sources

SourceDataUpdate Frequency
USNO (aa.usno.navy.mil)Sun/Moon rise/set, twilight, phaseDaily
sunrise-sunset.orgSun times, day length, twilightDaily
NOAA SWPCKp index, solar wind, aurora forecast5 minutes
NOAA TidesTide predictions (Station 9447659)Daily
JPL HorizonsMoon distance, planetary ephemerisOn demand
NOAA DSCOVR/EPICEarth imagery from L1Hourly (when available)

Deep Research — Science & Education Hub

Artemis II Mission

Local Observatories

Knowledge Graph

SOL connects celestial mechanics to mission education. The same Moon tracked here is where Artemis II is going. The same Sun drives the microclimate patterns measured at Mukilteo. The tides in Possession Sound are pulled by lunar gravity. Everything connects.