Motors and Rumble · Volume 3

Linear Resonant Actuators and Voice-Coil Exciters — Crisp, Quiet, and Sized for Something Smaller Than a Gun

How a spring-mounted magnet makes vibration, why a resonant actuator is strong only at one frequency and an exciter only above one, what the published parts deliver on a 1.3 kg shell, and the case for using one on a floating grip panel rather than on the whole gun

3.1 One mechanism, two kinds of part

A linear resonant actuator and a voice-coil exciter are the same machine: a coil and a permanent magnet, one of them carried on a spring or suspension, the other fixed to the thing to be shaken. Current in the coil pushes the moving part one way; reversing the current pushes it back. The reaction on the fixed part is the vibration. Nothing rotates, so there are no brushes, no commutator noise and no start-up lag of a rotor coming up to speed.

The difference is the spring. In a linear resonant actuator (LRA) the spring is stiff and the moving mass small, so the system has a sharp resonance, usually somewhere between about 125 and 300 Hz, and it is driven at that resonance where a little power gives a lot of motion. In a voice-coil exciter the suspension is soft enough, or the moving mass large enough, that the resonance sits at one edge of a wide useful band, and the part is driven like a loudspeaker by an audio amplifier.

3.2 How a linear resonant actuator works

The cycle of operation, for a typical coin-shaped LRA:

  1. A magnet and a tungsten or steel mass hang on a flat spring inside a sealed can; a coil is fixed to the can’s base below them.
  2. The driver applies an AC voltage at the spring-mass resonance. Each half-cycle the coil’s field pushes the magnet up or pulls it down.
  3. At resonance the spring’s stiffness and the mass’s inertia cancel, and the motion builds until the energy the coil puts in each cycle equals what damping takes out. The reaction on the can, and so on whatever the can is glued to, is the vibration, along one axis, perpendicular to the coin’s face.
  4. Off resonance the output falls steeply, because the coil is fighting the spring (below) or the mass (above).
  5. Removing the drive leaves the mass ringing down at its own rate. A driver that reverses the phase for a cycle or two (Volume 4) stops it in a few milliseconds.

Because the useful band is narrow, and because the resonance moves with the part’s tolerance, its temperature and how it is mounted, a good LRA driver tracks the resonance: it watches the back-EMF of the moving magnet and keeps its drive in phase. TI’s DRV2605L does this for LRAs between 125 and 300 Hz, a range its datasheet narrowed from an earlier “50 Hz” minimum in a revision.1 Volume 4 covers the drivers.

3.3 A real LRA, from its datasheet

The best-documented hobby-available LRA is the 10 mm coin part sold today as the Vybronics VG1040003D, whose predecessor was the Jinlong G1040003D. SparkFun hosts the Jinlong datasheet:2

Table 1 — A real LRA, from its datasheet

ParameterG1040003D
Rated input2.5 V r.m.s. AC sine; range 0.1–2.5 V r.m.s.
Input frequency150–200 Hz; resonance f0 170 ±5 Hz
Rated current170 mA r.m.s. maximum
Acceleration (minimum)0.9 G r.m.s. at 150 Hz; 1.0 G r.m.s. at 200 Hz; 1.8 G r.m.s. at f0
Test fixture100 g “dummy jig”, 15 × 45 × 105 mm, on a sponge, with a Brüel & Kjær 4393 accelerometer, vibrating along its 15 mm direction
Rise time≤ 10 ms to 50 % of normal
Brake time≤ 50 ms to 10 % of normal
Noise≤ 50 dB(A)
Life1,000,000 cycles of 2 s on, 1 s off

Three things stand out. First, the rise is fast: 10 ms to half amplitude, against 40 ms of lag before a coin ERM even begins to move (Volume 2). That is the LRA’s real advantage. Second, the band is narrow: half the output at 150 Hz, 20 Hz below the resonance. Read as three points on one curve, the minimum figures are consistent with a quality factor of about 5 to 6. Third, the strength is a phone’s: 1.8 G r.m.s. on 100 g is about 5.1 G peak-to-peak, the same order as a 9 mm coreless ERM.

DigiKey lists the current part as “VIBRATION LRA MOTOR 170HZ 2G”, 2.5 V AC (part 1670-VG1040003D-ND), according to a search of its pages; the page itself could not be read on the day, and no price was captured. Whether the Vybronics revision carries the same acceleration table as the Jinlong sheet was not confirmed.

3.4 Wideband actuators

A second class of linear actuator is built with a lower Q and a wider band, so that the waveform can change frequency: a game can play a 90 Hz thump and a 300 Hz click through the same part. Renesas’ DA7280 driver supports both narrowband and “wideband” LRAs; its product page gives resonance tracking up to 300 Hz and a wideband drive from 25 Hz to 1 kHz.3

PUI Audio’s HD-VA3222 is a flat actuator sold in this space. Its datasheet gives:4

Table 2 — Wideband actuators

ParameterHD-VA3222
Maximum input1.5 V r.m.s.
DC resistance; impedance8.3 Ω; 8.4 ±0.9 Ω
Resonance; frequency range133 ±13 Hz; 80–500 Hz
Acceleration”Max Acceleration (@133 Hz) 2.52 Gp-p”; at 0.5 V, 2.52 G at 133 Hz, 0.41 G at 300 Hz, 0.33 G at 400 Hz, 0.28 G at 500 Hz
Rise (0–90 %) / fall (100–10 %)46 ms / 36 ms
Mass8.5 g

The sheet does not state the test mass, so the acceleration cannot be compared with the 100 g figures; it gives the same 2.52 G both as the maximum and as the 0.5 V figure, which is inconsistent; and its rise time is far slower than the narrowband LRA’s. Its resonance at 133 Hz sits in the hand’s best band, which is the attraction. Its availability was unclear: DigiKey’s listing appeared active in a search, PUI’s own page said stock was unavailable, and one broker marked it obsolete.

3.5 Voice-coil exciters and tactile transducers

An exciter is a loudspeaker motor with no cone, made to turn a panel into a speaker. Fixed to a gun’s shell it shakes the shell instead. Dayton Audio, whose exciters are the common hobby part, gives these figures on its own pages:567

Table 3 — Voice-coil exciters and tactile transducers

PartSizeResonance (free air)Impedance; powerMSRP
DAEX13CT-8 coin exciterØ26.3 × 9.5 mm775 Hz8 Ω (Re 7.3 Ω); 3 W r.m.s.$5.99
DAEX25CT-4 coin exciterØ48 × 15 mm306 Hz4 Ω (Re 3.6 Ω); 10 W r.m.s.$15.99
TT25-8 PUCK tactile transducer3½ in diameter × 1 in (89 × 25 mm)40 Hz; “usable” 20–80 Hz8 Ω (Re 7.7 Ω, Le 1.30 mH); 15 W r.m.s., 30 W max$23.99

Dayton’s own pages warn that an exciter’s response “is completely dependent” on the surface it drives, so the free-air resonance is a starting point only.

Figure 1 — Dayton Audio DAEX25CT-4, a 25 mm coin-type exciter: a voice coil and magnet in a 48 mm steel housing with solder tabs, made to be glued to a panel. Its free-air resonance is 306 Hz, above the hand'…
Figure 1 — Dayton Audio DAEX25CT-4, a 25 mm coin-type exciter: a voice coil and magnet in a 48 mm steel housing with solder tabs, made to be glued to a panel. Its free-air resonance is 306 Hz, above the hand's most sensitive band. Photo: Dayton Audio.
Figure 2 — Dayton Audio TT25-8 PUCK, a tactile transducer for gaming chairs and furniture: an 89 mm disc rated 15 W r.m.s. into 8 ohms, with a 40 Hz resonance and a usable band of 20 to 80 Hz. It is the right…
Figure 2 — Dayton Audio TT25-8 PUCK, a tactile transducer for gaming chairs and furniture: an 89 mm disc rated 15 W r.m.s. into 8 ohms, with a 40 Hz resonance and a usable band of 20 to 80 Hz. It is the right kind of device for a heavy, low shake, and far too large for the inside of an MP7. Photo: Dayton Audio.

The coin exciters are built to make sound, and their resonances (306 and 775 Hz) sit well above the band the gripping hand feels best. The PUCK is built to make furniture shake, with exactly the low, heavy band a rumble wants, and is twice the width of the gun.

3.6 Where each delivers its force

The force an inertial actuator puts on its mounting, for a constant drive, follows the response of a spring-mounted mass: it rises as the square of frequency below the resonance, peaks at the resonance by a factor set by the Q, and settles to a constant above it.

Figure 3 — Relative force on the mounting at constant drive, against frequency, for three linear actuators, each scaled to 1 at its own peak, with the hand's most sensitive band shaded. The LRA (resonance 170…
Figure 3 — Relative force on the mounting at constant drive, against frequency, for three linear actuators, each scaled to 1 at its own peak, with the hand's most sensitive band shaded. The LRA (resonance 170 Hz, Q about 5.5, fitted to the G1040003D datasheet's three minimum figures, shown as circles) is strong only within about 20 Hz of its resonance. The coin exciter DAEX25CT-4 (306 Hz) delivers a third or less of its peak force anywhere in the hand's band. The tactile transducer TT25-8 (40 Hz) is flat across the band. The squares are PUI's published points for the HD-VA3222, relative to its 133 Hz figure. The exciter curves use an assumed Q of 2. Own work.

The chart is the argument of this volume in one picture:

  • An LRA is a tuning fork. Driven at its resonance it is efficient and fast; 30 Hz either side it gives half or less. Its resonance is fixed by its construction, and the common parts sit at 170 Hz or higher, just above the hand’s best band.
  • A coin exciter is a tweeter. Below its resonance its force falls as the square of frequency, so a 306 Hz exciter gives about a ninth of its plateau force at 100 Hz.
  • A tactile transducer is the right shape of curve, at a size that does not fit.

3.7 On a gun: the mass problem again, and a way round it

Scaled to a 1.3 kg gun as in Volume 2, the G1040003D’s 1.8 G r.m.s. on 100 g becomes about 0.14 G r.m.s., 1.4 m/s² r.m.s., at 170 Hz: the same group as the small ERMs, and well short of the 34 mm ERM. Every LRA and coin exciter on sale is sized for a phone or a controller, and none of them shakes a 1.3 kg gun hard.

There is a way round this that the ERM does not offer as neatly. Shake less of the gun. If the actuator is mounted not to the receiver but to a grip panel or a backstrap insert carried on soft mounts (silicone grommets, a TPU frame), the moving mass is the panel, tens of grams, and the hand’s palm is on exactly the part that moves. Volume 1’s third finding from the hand research applies: the Pacinian channel sums over area, so the panel should be large (the whole grip side, not a button-sized patch), and the rest of the gun should not be a rigid surround pressing on the same skin.

On a 50 g floating panel, the same LRA would give in the region of 1.8 × 0.1 / 0.05 ≈ 3.6 G r.m.s., an estimate that ignores the soft mount’s own stiffness and the hand’s damping. That is stronger at the palm than the 34 mm ERM shaking the whole gun, from a part that starts in 10 ms, makes no brush noise, and draws 170 mA. The costs are mechanical: a grip that moves relative to the gun, gaps that must not pinch, and a realism question, since the real MP7’s grip is one moulding with the receiver.

This is a local cue channel, not a rumble: crisp, quiet, fast, suited to “reload”, “click” and menu cues and to a per-shot tap in quiet play. The whole-gun shake for explosions and damage still wants an ERM (Volume 2). The two can coexist, with OpenFIRE’s single rumble output driving one and the fork’s serial commands the other (Volume 6).

3.8 Where to buy, and what it costs

Prices as read on 19 October 2026:

Table 4 — Prices as read on 19 October 2026

PartSellerPriceNote
SparkFun Qwiic Haptic Driver DA7280 (ROB-17590), LRA fittedSparkFun$11.50 (10+ $10.93; 25+ $10.35; 100+ $9.78)8The cheapest way to try an LRA with a tracking driver; page showed both “In stock” and “Backorder”
Vybronics VG1040003D LRADigiKey (1670-VG1040003D-ND)not capturedPage not readable on the day
PUI HD-VA3222DigiKeynot capturedAvailability unclear (3.4)
Dayton DAEX13CT-8Dayton Audio$5.99 MSRP
Dayton DAEX25CT-4Dayton Audio$15.99 MSRPA Parts Express category page showed $17.99
Dayton TT25-8 PUCKDayton Audio$23.99 MSRP
Figure 4 — SparkFun's Qwiic Haptic Driver: a Renesas DA7280 driver with a coin linear resonant actuator already mounted on the board, two Qwiic I²C connectors and breakout pads. Photo: SparkFun Electronics.
Figure 4 — SparkFun's Qwiic Haptic Driver: a Renesas DA7280 driver with a coin linear resonant actuator already mounted on the board, two Qwiic I²C connectors and breakout pads. Photo: SparkFun Electronics.

3.9 Why this, and why not the others

Criteria: as Volume 2, plus speed of start and stop, and quietness for the cue channel.

Table 5 — Why this, and why not the others

CandidateForAgainstDecision
LRA on a floating grip panel (G1040003D class, on the SparkFun DA7280 board for the trial)Fast (≤ 10 ms rise), quiet, brushless, low current; strong at the palm if only a panel movesWeak on a whole gun; narrow band at 170 Hz; moving grip is a realism and pinch question; needs an AC driverTesting: a second, local cue channel (MR-2), after the ERM
LRA on the receiver (whole gun)As above, simpler≈ 1.4 m/s² r.m.s. on 1.3 kg: a tingleRejected
PUI HD-VA3222133 Hz, in the best band; widebandNo test mass; inconsistent sheet; slow rise; uncertain supplyRejected until a readable stock listing and a clearer sheet exist
DAEX13CT-8, DAEX25CT-4 excitersWideband, cheap, driven by any audio amplifierResonance 306–775 Hz, above the band; the 25 mm part is 48 mm acrossRejected
TT25-8 PUCKThe right band and strength89 mm across; the MP7 is 42 mm wideRejected for the gun; usable as a shaker under a seat or pedal, which is outside this dive

3.10 What could not be verified

  • Whether the Vybronics VG1040003D matches the Jinlong G1040003D sheet read here.
  • Prices for the Vybronics and PUI parts.
  • The Q of the exciters: assumed for the chart.
  • The floating-panel estimate: an arithmetic upper bound; the mount and the hand will reduce it. A bench test is in Volume 7.
  • Tactile Labs’ Haptuator, often used as a research reference actuator: no maker specification or price could be read, so it is left out.

Sources

Footnotes

  1. Texas Instruments, DRV2605L 2- to 5.2-V Haptic Driver for LRA and ERM With Effect Library and Smart-Loop Architecture, SLOS854D: Recommended Operating Conditions (LRA frequency range 125–300 Hz) and revision history. https://www.ti.com/lit/ds/symlink/drv2605l.pdf, read 2026-10-19. ↩

  2. Jinlong Machinery & Electronics, G1040003D linear vibrator specification (hosted by SparkFun). https://cdn.sparkfun.com/assets/d/0/4/c/d/G1040003D.pdf, read 2026-10-19. ↩

  3. Renesas, DA7280 product page. https://www.renesas.com/en/products/da7280, read 2026-10-19. ↩

  4. PUI Audio, HD-VA3222 data sheet, revision B, 25 October 2022. https://api.puiaudio.com/filename/HD-VA3222.pdf, read 2026-10-19. ↩

  5. Dayton Audio, “DAEX25CT-4 Coin Type 25mm Exciter 10W 4 Ohm”. https://daytonaudio.com/product/1175/daex25ct-4-coin-type-25mm-exciter-10w-4-ohm, read 2026-10-19. ↩

  6. Dayton Audio, “DAEX13CT-8 Coin Type 13mm Exciter 3W 8 Ohm”. https://www.daytonaudio.com/product/1173/daex13ct-8-coin-type-13mm-exciter-3w-8-ohm, read 2026-10-19. ↩

  7. Dayton Audio, “TT25-8 PUCK Tactile Transducer Mini Bass Shaker”. https://www.daytonaudio.com/product/1104/tt25-8-puck-tactile-transducer-mini-bass-shaker, read 2026-10-19. ↩

  8. SparkFun Electronics, “SparkFun Qwiic Haptic Driver - DA7280”, ROB-17590. https://www.sparkfun.com/sparkfun-qwiic-haptic-driver-da7280.html, read 2026-10-19. ↩

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