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Vaughn Associates, Inc.

Mechanical Shock Testing: Pulses, Machines & MIL-STD-810/883

A practical guide to mechanical shock testing: classical pulses, free-fall vs. pneumatic machines, SRS, fixtures and how MIL-STD-810 and MIL-STD-883 differ.

Eric WoodsEric WoodsSales Engineer · Area Sales Manager
Published 6 min read
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Photo: Art Guzman / Pexels

Key takeaways

  • Classical shock pulses (half-sine, terminal-peak sawtooth and trapezoidal) are defined by peak acceleration and duration, which together set the velocity change.
  • Free-fall shock machines use gravity and drop height; pneumatic machines add stored gas energy to reach higher velocity changes and very high g levels.
  • A shock response spectrum (SRS) describes a shock by its effect on a range of single-degree-of-freedom systems, which is how MIL-STD-810 tailors many shock tests to measured environments.
  • MIL-STD-810 Method 516 addresses equipment-level shock across the life cycle; MIL-STD-883 Method 2002 applies short, very high-g half-sine pulses to microcircuits.
  • Fixture stiffness and accelerometer choice often decide whether the pulse on the test article matches the pulse the specification calls for.

Mechanical shock testing applies a short, controlled acceleration pulse to a product to prove it survives the impacts, drops and pyrotechnic events it will see in service. Most specifications define that pulse either as a classical waveform, such as an 11 ms half-sine, or as a shock response spectrum derived from measured field data. The standard you’re working to, the size of the test article and the required velocity change determine whether you need a free-fall machine, a pneumatic machine or a shaker.

What is mechanical shock testing?

Mechanical shock testing is a laboratory method for reproducing transient mechanical loads on hardware in a repeatable way. Shock events last from fractions of a millisecond to tens of milliseconds and excite the resonances of structures, circuit boards, connectors and mounts.

Engineers run shock tests to:

  • Qualify equipment to a contractual specification.
  • Find fragility limits during development.
  • Screen production parts for workmanship defects.
  • Validate packaging for handling and transportation.

What are classical shock pulses?

Classical shock pulses are simple waveforms defined by peak acceleration (g) and duration (ms). The area under the pulse is the velocity change (ΔV), which is the parameter that drives machine selection.

Pulse Shape Ideal velocity change Typical generation Notes
Half-sine Smooth rise and fall 2 × A × T ÷ π Elastomer programmers on drop or pneumatic machines The most widely specified classical pulse
Terminal-peak sawtooth Linear rise, rapid decay A × T ÷ 2 Crushable (for example, lead) programmers Produces a more uniform response across frequency than a half-sine
Trapezoidal (square wave) Fast rise, flat top, fast fall Approximately A × T Gas (pneumatic) programmers Delivers a large velocity change at a controlled g level

As a worked example, a 50 g, 11 ms half-sine (A = 490 m/s², T = 0.011 s) has an ideal velocity change of about 3.4 m/s, or 11.3 ft/s. Rebound off the programmer adds to that, which is why required drop height differs from simple free-fall math.

Free-fall vs. pneumatic shock machines: what’s the difference?

A free-fall shock machine raises a table and drops it onto a programmer, so velocity change comes from gravity and drop height. A pneumatic shock machine uses compressed gas to accelerate the table, reaching higher impact velocities and higher g levels in a compact frame.

Free-fall shock machine Pneumatic shock machine
Energy source Gravity (drop height) Stored gas pressure plus gravity
Velocity change Limited by practical drop height Higher for a given machine size
Peak g and duration Moderate g, longer pulses Very high g, short pulses
Typical use Equipment and component shock, package testing Microelectronics and high-g component qualification
Emerson Apparatus models FSM series, 5–5,000 lb payloads, tables from 4×4 in to 60×60 in PSM100–PSM2500, 100–2,500 lb payloads

Emerson Apparatus, which incorporated VST (Vibration & Shock Technologies) in 2019, lists its pneumatic machines for half-sine, square-wave, trapezoidal and terminal-peak sawtooth pulses, with closed-loop control, horizontal capability and ratings up to 30,000 g for MIL-STD-883 work. Achievable levels depend on payload and pulse. Shock amplifier options on both machine types extend peak g for very short pulses, and Emerson’s ShockTool software handles shock control and pulse analysis.

Electrodynamic shakers can also run shock tests. They excel at synthesizing SRS-based waveforms but are limited by stroke, velocity and force.

What is a shock response spectrum (SRS)?

A shock response spectrum shows the peak response that a series of single-degree-of-freedom oscillators, each tuned to a different natural frequency, would experience when their common base sees a given shock. It describes a shock by its damage potential across frequency rather than by the shape of the time history.

Key points for test engineers:

  • Q = 10 (5% damping) is the common analysis default.
  • The maximax absolute acceleration spectrum is the usual presentation.
  • Different time histories can share a similar SRS, so an SRS can’t be converted back to a unique waveform.
  • Tailored tests start with measured field data, reduce it to an SRS, then synthesize a lab waveform that envelops it within tolerance.

MIL-STD-810 vs. MIL-STD-883: how do they differ?

MIL-STD-810 is an environmental engineering standard for equipment of all sizes, built around tailoring tests to the life-cycle environment. MIL-STD-883 is a test method standard for microcircuits, where shock tests are fixed, very high-g screens.

MIL-STD-810H, Method 516 (Shock) MIL-STD-883, Method 2002 (Mechanical Shock)
Scope Equipment and subsystems across transport, handling and operation Microelectronic devices
Philosophy Tailor levels to measured or predicted environments Standard test conditions called out by the procurement document
Pulse definition SRS-based waveforms or classical pulses, as tailored Half-sine pulses
Levels Program-specific Lettered conditions from A (500 g, 1.0 ms) to G (30,000 g, 0.12 ms)
Typical equipment Shakers, drop and pneumatic shock machines, drop and pendulum rigs High-g pneumatic shock machines with small fixtures

Method 516 in MIL-STD-810H organizes testing into eight procedures: functional shock (I), transportation shock (II), fragility (III), transit drop (IV), crash hazard shock (V), bench handling (VI), pendulum impact (VII), and catapult launch and arrested landing (VIII). Pyroshock and gunfire shock are covered separately in Methods 517 and 519. Always work from the revision and procedure named in your contract or test plan.

Why do fixtures make or break a shock test?

A shock fixture must transmit the pulse to the test article without adding its own resonances. A flexible fixture rings, amplifying some frequencies and attenuating others, so the article sees a different shock than the control accelerometer reports.

Good fixture practice includes:

  • Stiffness first. Push the fixture’s first resonance above the frequency range of interest.
  • Light, stiff materials. Magnesium and aluminum are common; Emerson Apparatus builds cube, L and T fixtures in both, designed with FEA.
  • Axis coverage. Cube fixtures let one setup cover three axes and both directions.
  • Controlled mounting. Use specified bolt torque and mount the control accelerometer near the article’s attachment points.
  • Survey before qualifying. Run a low-level pulse and review the response before committing flight or production hardware.

What instrumentation do shock tests need?

Accurate shock data depends on the right accelerometer, sample rate and filtering. Piezoresistive accelerometers with DC response capture long-duration pulses and velocity change well, while piezoelectric sensors suit many high-frequency measurements but can show zero shift under severe metal-to-metal impacts. A common guideline is to sample at least ten times the highest frequency of interest, with appropriate anti-aliasing filtering.

Field measurement closes the loop on tailoring. Instrumented Sensor Technology (IST) builds self-contained recorders that capture real transport and handling shock:

  • EDR-5 series: built-in triaxial accelerometers from ±10 to ±200 g, up to 50,000 samples per second per channel, external IEPE inputs, and unattended deployments of hours to months.
  • SnapShock-PLUS: peak g, duration, velocity change and time stamp for each event, with a drop-height mode for package studies.
  • DynaMax Suite software: waveform, PSD and statistical analysis to turn field data into lab test profiles.

IST also rents recorders for one-off test programs.

Shock test support in Huntsville and across the Southeast

Huntsville’s concentration of missile, space and defense electronics programs makes shock qualification a daily concern for local test labs and contractors. From our Huntsville headquarters, Vaughn Associates helps engineers size shock machines, plan fixtures, upgrade controls on legacy machines and choose recorders for field measurement.

We represent Emerson Apparatus across all Vaughn territories and IST across our territories (Tennessee and Mississippi only in our Tennessee, Arkansas and North Mississippi territory; North Carolina only in our North Carolina, Virginia, Maryland and D.C. territory). Explore shock and vibration test equipment and shock and vibration data recorders, review the Emerson Apparatus and IST pages, or request application help.

Frequently asked questions

How do you calculate the velocity change of a half-sine shock pulse?

For an ideal half-sine pulse with no rebound, velocity change equals 2 × peak acceleration × duration ÷ π. A 50 g, 11 ms half-sine works out to about 3.4 m/s (11.3 ft/s). A terminal-peak sawtooth with the same peak and duration has an ideal velocity change of A × T ÷ 2, or about 2.7 m/s. Rebound off the programmer adds to the total velocity change, which is why actual drop heights vary by machine.

Can an electrodynamic shaker perform shock tests?

Yes, within limits. A shaker controller can reproduce classical pulses or synthesize waveforms to match a shock response spectrum, which is useful for tailored MIL-STD-810 testing. The shaker's stroke, velocity and force ratings cap the achievable velocity change and peak g, and pulses need compensation so the table ends with zero net displacement. High-g, large velocity-change shocks are better suited to dedicated shock machines.

What Q factor is used for a shock response spectrum?

Q = 10, which corresponds to 5% critical damping, is the most common choice for SRS analysis and is widely used in MIL-STD-810 practice. The Q value changes the height of the spectrum, so when comparing a lab test SRS with field data, both must be computed with the same Q, the same spectrum type (usually maximax absolute acceleration) and the same frequency spacing.

Is Emerson Apparatus the same company as VST?

Emerson Apparatus, a privately held equipment builder in Gorham, Maine, acquired Vibration & Shock Technologies (VST) around September 2019. VST products are now built and supported under the Emerson Apparatus name, and the old VST website redirects there. Emerson Apparatus is not related to Emerson Electric Co. It also retrofits controls on legacy M/RAD and VST machines and rebuilds AVEX shock machines.

Eric Woods

About the author

Eric Woods

Aerospace engineer turned sales engineer serving North Alabama, Georgia and South Carolina from Vaughn's Huntsville headquarters.

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