Past Week's Recap

I've been calling last weekend a "genie wish" storm -- we got what we asked for, but not necessarily what we wanted. This was by far and away the largest winter storm cycle we've seen in the Cascades this winter, and the result was lost power, pass closure, and powder so deep it was nearly impossible to get anywhere. Even the lowlands got in on the action with 3 inches recorded at Sea-Tac on Friday, although this was a narrow band, with little to no snow measured south of Tacoma and north of Everett.

Kona Low (red "L") northwest of Hawaii with the plume of moisture and the "mega-death" ridge over the southwest.
All our lovely cold air began to shut off on Sunday as a robust ridge continued to build to the southwest. This directed a mean old plume of moisture directly at us from the subtropics, putting us on a true Pineapple Express, with the moisture source being directed straight from Hawaii. This moisture plume been stationary over the region since Tuesday with freezing levels reaching 10,000 feet. Although integrated vaport transport has not been crazy high, the entended time period of this moisture supply put it in the AR3 (strong) category.
The stationary front (red half circles and blue triangles) sitting over the north end of Vancouver Island as of Thursday morning.

As an aside, this past week brought intense rain to the Hawaiian Islands and record heat to the southwest. In Hawaii, over a meter (!!) of rain fell at some high elevation locations in the past week as a deep and powerful "Kona Low" impacted the region with deep troughing over the central Pacific. Further east (U.S. Southwest), a "mega-death ridge" built in place with record-breaking heat with many locations experiencing record-setting March temperatures.
Precipitation over the southern Hawaiian island between March 10 and March 19. Measurements shown are in inches.

🧙‍♂️ Forecast Discussion

Short-term (Friday-Sunday)

A pretty boring forecast as we return to the normal AR roller coaster. As the current AR weakens and the cold front moves through Friday, a weak transient ridge builds overhead. As the weekend begins, freezing levels will drop sharply towards more manageable levels (read below 5000 ft). However, the moisture tap will be turned off, although there may be some lingering convergence zone or convective activity that may drop some preciptiation in the central to northern Sound region. In the east part of the Northern Cascades, snow may be able to build up a bit through Friday into Saturday as the cold air and residual moisture look to interact a little bit.

Weekend snow accumulation totals from the 4-km UW WRF model initialized on 19 March.
Patchy clouds and periods of sun under seasonably cool conditations should make for some pleasant time outside. By the end of Sunday, temperatures will be on the rise again as the next AR approaches.


A freezing level roller-coaster as they move up and dow

Medium-Term (Monday-Wednesday)

The medium term looks much the same with an AR passing through on Tuesday with moderately high freezing levels to drop more rain on the mountains.Nevertheless, after this passes, there is an intruiging system arriving Wednesday developing with some decent model agreement on a solid dose of snow.

CW3E AR ensemble outlook for Seattle for Mar 12 - Mar 18
Check out the timing of Wednesday the 25th's system with lots of ensemble spread, but decent totals for a vast majority of members. Note 00Z is the equivalent of 4pm on the previous day.

🧙🔮🧙‍♂️ Reading the crystal ball - 7+ day outlook

There is a decent amount of uncertainty in the next week as we sit at the interface between the big, nasty ridge to our south and cooler Gulf of Alaska troughing to our north. This leaves us at the mercy of a bit of atmospheric randomness that makes longer term forecasts for our area a bit challenging. However, there is decent agreement we likely won't be suffering under a mega-ridge. So we'll take that as a win.

CW3E AR ensemble outlook for Seattle for Mar 12 - Mar 18
EPS 5-day 850 hPa temperature anomaly outlook. We lie at the interface of hot and cold.




❄️ Snowfall

Weekend Snow Accumulation Forecast

Site Through 4am Saturday Through 4am Sunday Weekend Snow Accumulation (4pm Thursday through 4am Monday 16 Mar)
Mt. Baker (4500')0-2"0-2"0-2"
Washington Pass3-6"3-6"3-6"
Stevens Pass (4500')0"0"0"
Hurricane Ridge0-1"0-1"0-1"
Blewett Pass0"0"0"
Snoqualmie Pass0"0"0"
Crystal (5000')0"0"0"
Paradise0-2"0-2"0-2"
White Pass (5000')0"0"0"

🧊 Freezing Level

  • Friday: 7000-9000 feet (strong north-south gradient)
  • Saturday: 2000-4000feet
  • Sunday: 2000-4000 feet (rise in evening)

🎿 Our Recommendations

Best Choice This Weekend: Southern British Columbia

After this week of rain nuked any good, accessible snow, it's time to head a bit north. While driving far into thr Canadian coastal range or Rockies will be the best bet, there may be some fun to be had at Whistler on Saturday. I also have a hunch that there could be a bit of snow to play around with in Manning Park, just north of North Cascades National Park. Check it out if you're willing to drive!

Runner-Up: Washington Pass

It's risky given access limitations (unless you have a sled), but Washington Pass might be in the right location to see a decent coating on top of the mush. I can't say the snow will be good to ski, but it might be servicable.

Before we go, a quick detour to ask does rain actually melt our snowpack?

This week's AR dumped an egregious amount of rain on the snowpack we built last weekend — and yes, snow definitely melted. But is the rain directly to blame? Not really. The physics are counterintuitive enough to be worth a quick detour.

Rain heat input vs. condensation latent heat

During a rain on snow event, the snowpack is a cold surface sitting in warm, saturated air. Ignoring net radiation (which is a rather big assumption here, but stick with me), there are two other ways energy reaches it: the heat carried by the rain itself, and the latent heat released when water vapor condenses directly onto the snow surface. The second one wins by a mile.

Using rough estimates for a site at ~1,500 m elevation with 5°C air, 100% humidity, 1 mm/hr of rain, and 3 m/s winds:

Rain heat input (Qr). One millimeter of rain per hour is 1 kg of water at 5°C landing on 0°C snow. Cooling through a 5 K temperature difference doesn't yield much:

Qr = 1 kg/m²/hr × 4,186 J/kg·K × 5 K = ~21,000 J/m²/hr → 0.06 mm w.e./hr melt

Condensation latent heat (QE). Warm saturated air at 5°C has a vapor pressure of ~872 Pa; the 0°C snow surface sits at ~611 Pa. That gradient, stirred by wind, drives vapor to condense directly onto the snow. When it does, every kilogram of condensed vapor releases 2,500,000 J — the latent heat of vaporization. That's ~600× the energy per kilogram compared to simply cooling liquid water by one degree:

Δq = 0.622 × (872 − 611) Pa / 84,100 Pa ≈ 0.0019 kg/kg
QE = 1.05 × 2,500,000 × 0.002 × 3 m/s × 0.0019 = ~30 W/m² → 0.33 mm w.e./hr melt
Rain heat input
0.06
mm w.e./hr melt
Baseline — 1×
Condensation latent heat
0.33
mm w.e./hr melt
~5× more melt than rain
Rain heat input
0.06
mm w.e./hr
Condensation
0.33
mm w.e./hr
What about turbulent sensible heat? The wind also transfers heat directly from warm air to the snowpack (QH), contributing another ~32 W/m² under these conditions — roughly comparable to the condensation term. So rain is actually the smallest of the three melt drivers during a warm, windy AR event. That's left for a separate post.

The bottom line: melt during rain-on-snow events is driven by warm, humid, windy air — not precipitation volume. The rain is just along for the ride.

Estimates use a bulk aerodynamic approach (Ce = 0.002, neutral stability), standard atmosphere at 1,500 m (P = 84,100 Pa), and Magnus formula saturation vapor pressures. Rough numbers — intended as illustration, not a precise forecast.

⚠️ Safety & Travel Notes

  • For avalanche forecasts: Check NWAC.us before any backcountry travel.
  • Road Conditions: For latest road conditions, check WSDOT for current conditions.