The Stress-Velocity Relationship

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Presentation transcript:

The Stress-Velocity Relationship for Shock & Vibration By Tom Irvine

Introduction The purpose of this presentation is to give an overview of the velocity-stress relationship metric for structural dynamics Build upon the work of Hunt, Crandall, Chalmers, Gaberson, Bateman et al. But mostly Gaberson!

Develop a method for . . . paperppppppssss Project Goals Develop a method for . . . paperppppppssss Predicting whether an electronic component will fail due to vibration fatigue during a test or field service

Infinite Rod, Longitudinal Stress-Velocity for Traveling Wave Compression zone Rarefaction zone Direction of travel The stress  is proportional to the velocity as follows  is the mass density, c is the speed of sound in the material, v is the particle velocity at a given point The velocity depends on natural frequency, but the stress-velocity relationship does not.

Finite Rod, Longitudinal Stress-Velocity for Traveling or Standing Wave Direction of travel Same formula for all common boundary conditions Maximum stress and maximum velocity may occur at different locations Assume stress is due to first mode response only Response may be due to initial conditions, applied force, or base excitation

Beam Bending, Stress-Velocity Distance to neutral axis E Elastic modulus A Cross section area Mass per volume I Area moment of inertia Again, Same formula for all common boundary conditions Maximum stress and maximum velocity may occur at different locations Assume stress is due to first mode response only Response may be due to initial conditions, applied force, or base excitation

Bateman’s Formula for Stress-Velocity where is a constant of proportionality dependent upon the geometry of the structure, often assumed for complex equipment to be To do list: come up with case histories for further investigation & verification

MIL-STD-810E, Shock Velocity Criterion An empirical rule-of-thumb in MIL-STD-810E states that a shock response spectrum is considered severe only if one of its components exceeds the level Threshold = [ 0.8 (G/Hz) * Natural Frequency (Hz) ] For example, the severity threshold at 100 Hz would be 80 G This rule is effectively a velocity criterion MIL-STD-810E states that it is based on unpublished observations that military- quality equipment does not tend to exhibit shock failures below a shock response spectrum velocity of 100 inches/sec (254 cm/sec) Equation actually corresponds to 50 inches/sec. It thus has a built-in 6 dB margin of conservatism  Note that this rule was not included in MIL-STD-810F or G, however

V-band/Bolt-Cutter Shock The time history was measured during a shroud separation test for a suborbital launch vehicle.

SRS Q=10 V-band/Bolt-Cutter Shock

Space Shuttle Solid Rocket Booster Water Impact The data is from the STS-6 mission. Some high-frequency noise was filtered from the data.

SRS Q=10 SRB Water Impact, Forward IEA

SR-19 Solid Rocket Motor Ignition The combustion cavity has a pressure oscillation at 650 Hz.

SRS Q=10 SR-19 Motor Ignition

RV Separation, Linear Shaped Charge The time history is a near-field, pyrotechnic shock measured in-flight on an unnamed rocket vehicle.

SRS Q=10 RV Separation Shock

El Centro (Imperial Valley) Earthquake The magnitude was 7.1.

SRS Q=10 El Centro Earthquake North-South Component

SRS Q=10, Half-Sine Pulse, 10 G, 11 msec

Maximum Velocity & Dynamic Range of Shock Events Pseudo Velocity (in/sec) Velocity Dynamic Range (dB) RV Separation, Linear Shape Charge 526 31 SR-19 Motor Ignition, Forward Dome 295 33 SRB Water Impact, Forward IEA 209 26 Half-Sine Pulse, 50 G, 11 msec 125 32 El Centro Earthquake, North-South Component 12 Half-Sine Pulse, 10 G, 11 msec 25 V-band/Bolt-Cutter Source Shock 11 15 But also need to know natural frequency for comparison.

Sample Material Velocity Limits (psi)   (lbm/in^3) Rod Vmax (in/sec) Beam Plate Douglas Fir 1.92e+06 6450 0.021 633 366 316 Aluminum 6061-T6 10.0e+06 35,000 0.098 695 402 347 Magnesium AZ80A-T5 6.5e+06 38,000 0.065 1015 586 507 Structural Steel 29e+06 33,000 0.283 226 130 113 High Strength Steel 100,000 685 394 342

Project Goals Develop a method for . . . Predicting whether an electronic component will fail due to vibration fatigue during a test or field service

Project Goals Develop a method for . . . Predicting whether an electronic component will fail due to vibration fatigue during a test or field service

Project Goals Develop a method for . . . Predicting whether an electronic component will fail due to vibration fatigue during a test or field service

PUT IN YOUR OWN BEAM BENDING EXAMPLE Project Goals PUT IN YOUR OWN BEAM BENDING EXAMPLE Predicting whether an electronic component will fail due to vibration fatigue during a test or field service

Advantages Global maximum stress can be calculated to a first approximation with a course-mesh finite element model

Areas for Further Development of Velocity-Stress Relationship Only gives global maximum stress Cannot predict local stress at an arbitrary point Does not immediately account for stress concentration factors Essentially limited to fundamental mode response only Great for simple structures but may be difficult to apply for complex structure such as satellite-payload with appendages Unclear whether it can account for von Mises stress, maximum principal stress and other stress-strain theory metrics

Related software & tutorials may be freely downloaded from http://vibrationdata.wordpress.com/ The tutorial paper include derivations. Or via Email request tom@vibrationdata.com tirvine@dynamic-concepts.com

Conclusions Stress-velocity relationship is useful, but further development is needed including case histories, application guidelines, etc. Dynamic stress is still best determined from dynamic strain This is especially true if the response is multi-modal and if the spatial distribution is needed The velocity SRS has merit for characterizing damage potential Tripartite SRS format is excellent because it shows all three amplitude metrics on one plot