Puget Sound's Mixed Regime: Why Edmonds Coastal Currents Defy Standard Pacific Coast Models

Learn how to monitor Edmonds' coastal currents with ADCP. Discover equipment needs and selection.

Edmonds Waterfront vs. Open Coast: A Hydrodynamic Comparison

Measuring current velocities at the Edmonds waterfront isn't a standard exercise. Most engineers treat the Pacific Northwest coastline as a predictable system of swells and longshore drift. Edmonds is different. It sits in a complex intersection where the deep basins of the Puget Sound meet shallow, rocky littoral zones. This creates a chaotic mix of tidal fluxes and wind-driven surges that make standard coastal monitoring templates useless. If you apply a generic open-ocean model here, your data will be wrong. The interaction between the Strait of Juan de Fuca's inflow and the localized geometry of the Sound creates shear layers that can confuse a low-resolution sensor. To get a clean signal, we have to account for the specific way water piles up against the Snohomish County shoreline during high-tide events.

Baseline Conditions at Edmonds

Edmonds operates under a mixed tidal regime. You get two highs and two lows daily, but they aren't equal. Tidal ranges here can swing up to 15 feet. This isn't just a number on a chart. It means the water column depth changes drastically over a six-hour window. When the tide floods, water pushes into the bays with significant force. When it ebbs, it pulls back, often creating localized eddies around the waterfront parks and piers. Salinity varies wildly depending on the season. During the winter rains, freshwater runoff from the surrounding watershed dilutes the surface layer. This creates a stratified water column. We often see a sharp pycnocline where the salty ocean water slides under the fresh runoff. If you don't account for this stratification, your velocity profiles will look like noise.

How Edmonds Differs from Comparable Sites

Contrast Edmonds with the open beaches of La Push on the Olympic Peninsula. At La Push, you deal with massive Pacific swells and a relatively consistent longshore current. The energy is linear. At Edmonds, the energy is rotational. The Puget Sound's geography forces water to swirl and pivot. You don't get a steady stream; you get a pulsing system. Most ADCP deployments at La Push focus on wave-induced currents, but at Edmonds, the tide is the boss. Compare it to the currents in the San Francisco Bay. While both are estuaries, the Bay has a much more aggressive tidal prism and narrower bottlenecks. Edmonds is more open but suffers from "sloshing" effects. The water doesn't just flow in and out; it oscillates. I've seen data from the Sound where the current reverses direction faster than the tide tables predict because of wind-driven setup. This makes ground-truthing your data a nightmare if you rely solely on theoretical models.

Key Differences Identified

The primary divergence is the influence of the Strait of Juan de Fuca. This strait acts as a valve. Depending on the pressure gradient between the Pacific and the Sound, the baseline flow at Edmonds can shift. When the valve is open, we see stronger inflow. This overrides the local tidal signal. It's a layering effect: the tide provides the heartbeat, but the Strait provides the blood pressure. Then there is the bathymetry. The transition from the shallow rocky reefs near the shore to the deeper basins is abrupt. This creates vertical shear. Water at the surface might move east, while water 20 meters down moves west. This is a classic case of bin contamination if your ADCP blanking distance is set too short. You end up measuring the reflection from the seabed instead of the actual water movement. Wind also plays a disproportionate role here. The westerlies push surface water onshore. This creates a "pile-up" effect. In my experience, this often leads to anomalous surface velocities that don't match the deeper profiles. It's a surface-driven phenomenon that doesn't happen in the deeper, more stable waters of the open coast. Most technicians ignore the influence of the local piers and man-made structures. These act as baffles. They create micro-turbulences. If you place your sensor too close to a pier, you aren't measuring the coastal current; you're measuring the wake of the infrastructure. This is where most "noisy data" comes from in the Edmonds area. Finally, the biological load affects the signal. During salmon runs or herring blooms, the water is thick with organic matter. This is great for the ecosystem but tricky for acoustics. High biomass can cause signal attenuation. You might see a drop in the correlation magnitude, which tells you the signal is degrading. I usually suggest increasing the ping rate to maintain a lock on the particles.

Why These Differences Matter for Equipment Selection

You cannot just throw a generic current meter into the water at Edmonds and hope for the best. Because of the high tidal range and the risk of stratification, you need a high-frequency ADCP (Acoustic Doppler Current Profiler). I personally prefer a 600kHz unit for this environment. Why? Because it gives you the vertical resolution needed to see those shear layers without sacrificing too much range. A 300kHz unit is too blunt an instrument for the shallow-to-deep transitions found here. Mounting is the other critical failure point. Bottom-mounted frames are a gamble in the Sound due to shifting sands and rocky outcrops. I recommend a heave-compensated mooring or a fixed-pole installation with a precise depth offset. If your sensor tilts by even three degrees during a storm surge, your horizontal velocity components will be skewed. You'll spend weeks in the office trying to "fix" the data in post-processing when you should have just stabilized the mount. Avoid low-cost mechanical current meters. They can't handle the rapid reversals of the mixed tidal regime without significant lag. You need the instantaneous sampling of a Doppler system. Also, ensure the equipment has a robust anti-fouling system. The nutrient-rich waters of the Sound grow algae faster than you can blink. A fouled transducer face is the fastest way to get a garbage signal.

Analysis by Dr. Kenji Sato. Dr. Sato is a lead researcher in underwater acoustics with 20 years of experience deploying sonar instrumentation in complex estuarine environments. He specializes in high-resolution flow mapping for flood mitigation and coastal engineering.

Dr. Kenji Sato April 2, 2025
Archive
Why Port Gardner Bay's Tidal Asymmetry Outpaces Standard Puget Sound Flow Models
Learn how to monitor Everett's coastal currents with ADCP. Discover equipment needs and selection.