Simulated Spray Drift

100 ha Aerial Application Simulation

EDUCATIONAL SIMULATOR
SIMULATED SPRAY DRIFT
100 ha Spray Block · 1,000 × 1,000 m
READY
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8 km/hFrom W · travelling E
N
DepositionTrace
Heavy
Droplets4 target swathsOff-target
100 m
Forecast footprint · start to animate00:00
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From release point
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Of landed volume
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Sample maximum
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Outside 4-pass target
Full-run forecast · volume weightedAirborne at 180 s: 0%

Drift profile

Expand & inspect

Larger droplets settle close to release. Fine droplets form the drift tail.

What if you fly higher?

Current weather & droplet spectrum

Mean landed drift · metres

Droplet comparison

Current height & weather

Mean landed drift · metres

Drift profile · detailed analysis

Full-run forecast for your current aircraft, droplet and weather settings.

Follow the spray through the air

Hover over or tap a path to inspect that droplet. Use the time slider to follow it.

Initial size <200 µm200–299 µm≥300 µm○ Still airborne at 180 s

Droplet inspector

A representative volume parcel

Where does the spray end up?

Shares of all original spray volume across the four passes.

How much is height changing drift?

Compare your current release height with 3 m while keeping every other setting the same.

ScenarioMean driftAirborne at 180 s

Deposition distance distribution

Landed spray grouped by horizontal distance from its release point. Each percentage uses all emitted volume.

Why your profile has this shape

    Conditions behind this forecast

    How to read the expanded profile
    • All paths begin at the release point and your selected height above the crop. A path reaching 0 m represents deposition on the crop or ground.
    • The chart shows one horizontal component of motion. Average drift, deposition distance and maximum drift use total horizontal displacement, so they can be larger than the distance along the chart’s axis.
    • Each path colour represents its initial droplet diameter. The inspector shows how its diameter changes through evaporation. The enlarged map markers do not represent actual droplet size.
    • Open endpoints are still airborne at the 180-second limit. Their eventual landing positions remain unknown. Switching to the 95% view can hide the long tail; Full drift tail restores it.
    • Mean drift, the 90th percentile and mean landing time use only landed parcels. If a large fraction remains airborne, these statistics describe only the landed part of the spray.
    • The chart shows 128 representative paths from 2,048 source trajectories across four passes. Thousands of visible map droplets share these paths at different release positions. Their weights are divided to preserve original spray volume. Statistics cover all four passes; the selector and time slider also work without a mouse.
    • The horizontal and vertical axes have different scales. A curve’s visual angle is not the physical fall angle. The analysis is a full four-pass forecast, even if the map animation has only just started. Cross-track distance uses the first-pass heading as a fixed reference.
    Evaporation, settling and model assumptions

    The model uses a simplified D² evaporation law, a lognormal droplet-volume spectrum and sphere drag. Evaporation stops at a 1% nonvolatile volume residue. Water loss is not counted as lost chemical: reported spray fractions keep their original-volume weights.

    Stability and turbulence change illustrative eddy motion. This does not resolve temperature-inversion trapping, real aircraft vortices or downwash, terrain, nozzle geometry, droplet breakup or formulation-specific vapour drift. The numerical coefficients have not been calibrated to a particular aircraft or product.

    How this simulation works

    A controlled comparison of spray drift influences. These are conceptual estimates, not AgDRIFT®, AGDISP, buffer distances or operational guidance.

    Four consecutive spray passes

    The square block is exactly 1,000 m × 1,000 m (100 ha), split into two 50 ha halves. Four adjacent tracks run in alternating directions, beginning left of the centre line at the default heading. The heading control rotates the full plan. The intended target is the union of all four narrow swaths. The aircraft turns automatically with the spray off; droplets already released continue drifting. Turn paths are illustrative connections, not validated aircraft manoeuvres.

    The aircraft and spray markers are enlarged for visibility; map distances are to scale. Dotted contours measure distance from the first swath; bottom markers measure from the centre line. The smallest guides become readable when zoomed in.

    Droplets and settling

    Each pass uses 512 source trajectories sampling a lognormal volume distribution (log standard deviation 0.42) around the selected VMD. The 2,048 sources are weighted by the volume sprayed along each track. Each source is distributed into many visible droplets, sharing its motion at different release times and positions. Each marker carries part of its source weight, so extra visibility does not add spray volume or alter drift physics. Marker count is illustrative, not a count of real droplets. Up to 12,000 markers are drawn at once; all markers contribute to results. Category names are approximate examples; VMD alone does not establish a certified spray-quality class.

    Settling balances gravity against sphere drag using Reynolds-dependent drag (Schiller–Naumann approximation). A fixed 0.2 s model step integrates wind transport, settling and evaporation. Deterministic eddy variations produce different paths without changing the results on each run. A short, illustrative forward-motion term depends on aircraft speed. Aircraft vortices, downwash, breakup and nozzle geometry are not resolved.

    Evaporation, weather and canopy

    A simplified D² evaporation law uses K = 650 × vapour pressure deficit in µm²/s, with deficit in kPa. This coefficient is illustrative and uncalibrated. Temperature and relative humidity determine vapour pressure deficit. Evaporation stops at a fixed 1% nonvolatile volume residue; chemical mass is assumed retained. This is not a formulation-specific model and does not predict vapour drift.

    Release height is always above the selected canopy/target. Canopy changes near-surface wind attenuation, not the entered release height. Stability and turbulence change the illustrative eddy amplitude. Stable air mixes less; it does not switch gravity off. Inversion trapping, terrain, thermal structure and far-field transport are not resolved. A positive temperature difference activates the very-stable setting and warning.

    Read the results correctly

    Comparisons and score

    The fixed reference uses 3 m, 180 km/h, 350 µm VMD, 8 km/h wind from W, four alternating tracks starting northbound, 25°C, 60% RH, neutral stability, medium turbulence, a short crop and a 20 m swath. Height and droplet charts vary only their named setting, with 128 source trajectories per pass for each comparison point. A dagger (†) marks a result with more than 1% still airborne; landed-only means can understate that tail.

    The 0–100 index combines modeled mean drift, off-target deposition and unresolved airborne volume with wind, crosswind, release height, droplet size, evaporative demand and stability. It is an unvalidated teaching index, not a measure of legal compliance or a probability of harm.

    Controls

    Drag the map to pan; use the wheel or + / − to zoom. Fit restores the full field. Click or drag the compasses, or type a direction. Wind direction means from; the map arrow points where it is travelling. Changes recalculate the forecast and restart an active pass. Reset clears the current pass; Reset to baseline also restores every input. Playback speed changes animation time only.

    Background references

    The general relationships follow these references; the numerical implementation and teaching coefficients are independent and have not been validated by these organisations.

    References require internet access. The simulator itself makes no network requests.