September 2025

Oceanography | Vol. 38, No. 3

82

MECHANICAL DESIGN: OCEAN DRIFTER DYNAMICS

Using the curriculum, students learn that drifter motion is

shaped by water movement, wind drag, wave action, and buoy-

ancy. To track surface currents accurately, they explore how min-

imizing wind drag improves performance. Instead of relying on

mass or inertia, students design their drifters to be highly sensi-

tive to water flow.

Specifically, the motion of a surface drifter subject to oceanic

and atmospheric forcing can be described by Newton’s second law:

m dv

dt = Fdrag + Fwind + Fbuoyancy + Fgravity + FCoriolis + Fpressure,

(1)

where v is the drifter velocity and m is its mass. For small, low-​

inertia drifters, Coriolis and pressure gradient forces may be negli-

gible over short timescales (Niiler et al., 1987; Furnans et al., 2008).

BUOYANCY AND GRAVITY

To maintain surface tracking, the drifter is designed to be slightly

positively buoyant (ρwV > m; Bjørnestad et al., 2021):

Fbuoyancy = ρwgV,

(2)

Fgravity = mg,

(3)

where ρw is the density of seawater, V is the displaced volume, and

g is gravitational acceleration.

HYDRODYNAMIC AND WIND DRAG

The primary forces affecting horizontal motion are drag from both

water and air:

Fdrag, water = ½Cd,wρwAw(v – uw)2,

(4)

Fdrag, wind = ½Cd,aρaAa(ua – v)2,

(5)

where uw and ua are the water and wind velocities, Cd is the drag

coefficient, A is the effective cross-sectional area, and subscripts w

and a refer to water and air, respectively.

MINIMIZING WIND SLIPPAGE

Niiler et al. (1987) showed that to keep wind-induced slip under

1 cm s–1 when the wind speed is 10 m s–1, the drag area ratio (R)

should be greater than 40.

R = Aw

Aa

,

(6)

≈ 6.6 · 10–4 ·

Fwind

|ua|

Fwater

|uw|

(7)

A higher R ensures the water drag force dominates over the drag

from wind forces. The area ratio of the drifter provided as an exam-

ple to the students is approximately 40.

INERTIAL RESPONSE TIME

The drifter’s responsiveness to transient currents is governed by a

time constant:

τ =

meff

ρwCd,w Aw(vsteady state − uw)

(8)

where meff includes added mass from the surrounding fluid, an

important concept in hydrodynamics (Stelson and Mavis, 1957).

Increasing the water drag area lowers the τ values, yielding better

TABLE 1. List of provided materials.

PART NAME

PURPOSE

COST

USD

COMMERCIAL GPS SYSTEM

LandAirSea GPS tracker

Commercial cellular GPS tracker

$28

Cellular antenna

Replacement antenna for Cellular GPS tracker

$8

SHARED DRIFTER MATERIALS

Cotton canvas fabric

Underwater drogue

$2

3 mm thick jute rope

Frame construction and parts attachment

$2

Cork

Surface flotation

$4

20 mm dia by 1.6 m wooden dowel

Frame construction

$5

4 x 8 mm dia by 0.5 m wooden dowel

Frame construction

$3

Iron fishing weights

Counterbalance

$1

Cylindrical bamboo container

Electronic stack container

$8

Shellac

Waterproofing coating

$2

Coconut wax

Waterproof potting material

$2

CUSTOM GPS SYSTEM (OPTIONAL)

Lilygo T-sim7000g

Custom GPS cellular development board

$35

18650 Li-ion battery 1300 mAh

Custom GPS unit battery

$4

BMP390 breakout board

Barometric pressure and altimeter

$13

NTC 3950

Waterproof temperature sensor

$2

LTE-M SIM card

Cellular service provider

$20