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Special Geotechnical Features

Soil Dynamics and Special Design Aspects

Click on the link above to download.

MIL-HDBK-1007/3
15 November 1997

Supersedes NAVFAC DM 7.3, April 1983

SOIL DYNAMICS

  • BASIC DYNAMICS
    • Vibratory Motions
    • Mass, Stiffness, Damping
    • Amplification Function
    • Earthquake Ground Motions
  • SOIL PROPERTIES
    • Soil Properties for Dynamic Loading
    • Types of Soils
    • Dry and Partially Saturated Cohesionless Soils
    • Saturated Cohesionless Soils
    • Saturated Cohesive Soils
    • Partially Saturated Cohesive Soils
    • Measuring Dynamic Soil Properties
    • Field Measurements of Dynamic Modulus
    • Laboratory Measurement of Dynamic Soil Properties
  • MACHINE FOUNDATIONS
    • Analysis of Foundation Vibration
    • Machine Foundations
    • Impact Loadings
    • Characteristics of Oscillating Loads
    • Method of Analysis
    • Dynamic Soil Properties Design to Avoid Resonance
    • High-Speed Machinery
    • Low-Speed Machinery
    • Coupled Vibrations
    • Effect of Embedment
    • Proximity of a Rigid Layer
    • Vibration for Pile Supported Machine
    • Foundation Bearing Capacity and Settlements Vibration Transmission, Isolation, and Monitoring
    • Vibration Transmission
    • Vibration and Shock Isolation
    • Vibration Monitoring
  • DYNAMIC AND VIBRATORY COMPACTION
    • Soil Densification
    • Vibro-Densification
    • Dynamic Compaction Applications of Vibroflotation
    • Compaction Grout
  • PILE DRIVING RESPONSE
    • Wave Equation Analysis
    • Wave Propagation in Piles
    • Wave Equation Application
    • Dynamic Testing of Piles
    • Results From Dynamic Testing
    • Pile Dynamic Measurement Applications
    • Apparatus for Applying Impact Force
    • Impact Force Application
    • Apparatus for Obtaining Dynamic Measurement
    • Signal Transmission
    • Apparatus for Recording, Reducing, and Displaying Data

EARTHQUAKE ENGINEERING

  • EARTHQUAKE, WAVES, AND RESPONSE SPECTRA
    • Earthquake Mechanisms
    • Wave Propagation
    • The Response Spectrum
  • SITE SEISMICITY
    • Site Seismicity Study
    • Ground Motion Estimates Analysis Techniques
  • SEISMIC SOIL RESPONSE
    • Seismic Response of Horizontally Layered Soil Deposits
    • Evaluation Procedure Analysis Using Computer Program
  • DESIGN EARTHQUAKE
    • Design Parameters
    • Factors Affecting Ground Motion
    • Ground Motion Parameters
    • Site Specific Studies
    • Earthquake Magnitude
    • Design Earthquake Magnitude
    • Selection of Design Earthquake
    • Intensity Peak
    • Horizontal Ground Acceleration
    • Seismic Coefficients
    • Magnitude and Intensity Relationships
    • Reduction of Foundation Vulnerability to Seismic Loads
  • SEISMIC LOADS ON STRUCTURES
    • Earthquake Induced Loads
    • Foundation Loads
    • Wall Loads
    • Base Shear
  • LIQUEFACTION AND LATERAL SPREADING
    • Liquefaction Considerations
    • Factors Affecting Liquefaction
    • Evaluation of Liquefaction Potential
    • Simplified Empirical Methods
    • Peak Horizontal Acceleration
    • Laboratory Tests and Site Response
    • Method Slopes
    • Pseudostatic Design
    • Strain Potential Design
    • Lateral Spreading From Liquefaction
    • Lateral Deformation
    • Evaluation Procedure
    • Application
  • FOUNDATION BASE ISOLATION
    • Seismic Isolation Systems
    • System Definitions
    • Passive Control Systems
    • Active Control Systems
    • Hybrid Control Systems
    • Mechanical Engineering Applications
    • Historical Overview of Building Applications
    • Design Concept
    • Device Description
    • Elastometer Systems
    • Sliding System
    • Hybrid Systems
    • Application
    • Examples of Applications

SPECIAL DESIGN ASPECTS

  • SEISMIC DESIGN OF ANCHORED SHEET PILE WALLS
    • Design of Sheet Pile Walls for Earthquake
    • Design Procedures
    • Example Computation
    • Anchorage System
    • Ground Anchors
    • Displacement of Sheet Pile Walls
  • STONE COLUMNS AND DISPLACEMENT PILES
    • Installation of Stone Columns
    • Parameters Affecting Design Consideration
    • Soil Density
    • Coefficient of Permeability
    • Coefficient of Volume Compressibility
    • Selection of Gravel Material
    • Vibro-Replacement (Stone Columns)
    • Vibroflotation and Vibro-Replacement
  • DYNAMIC SLOPE STABILITY AND DEFORMATIONS
    • Slope Stability Under Seismic Loading
    • Seismically Induced Displacement
    • Slopes Vulnerable to Earthquakes
    • Deformation Prediction From Acceleration Data
    • Computation Method
    • Sliding Rock Analogy

Soil Dynamics

(Click on the above title to download)

Also available: Software for Soil Dynamics (zip format, Windows)

Arnold Verruijt
Univerisity of Delft, The Netherlands

A complete treatment on this subject, whose coverage in the literature is woefully inadequate. Topics include the following:

  • Vibrating Systems
  • Theory of Consolidation
  • Plane Waves in Porous Media
  • Waves in Piles
  • Earthquakes in Soft Layers
  • Cylindrical Waves
  • Spherical Waves
  • Elastostatics of a Half Space
  • Elastodynamics of a Half Space
  • Foundation Vibrations
  • Moving Loads on an Elastic Half Plane

We also offer for download the software that accompanies the text.

Dynamic Bridge Substructure Evaluation and Monitoring

Larry D. Olson, P.E.
FHWA-RD-03-089
September 2005

This research project was funded to investigate the possibility that, by measuring and modeling the dynamic response characteristics of a bridge substructure, it might be possible to determine the condition and safety of the substructure and identify its foundation type (shallow or deep). Determination of bridge foundation conditions with this approach may be applied to quantify losses in foundation stiffness caused by earthquakes, scour, and impact events. Identification of bridge foundation type may be employed to estimate bridge stability and vulnerability under dead and live load ratings, particularly for unknown bridge foundations.

A Frequency-Dependent Soil Propagation Model

Hal Amick
Colin Gordon & Associates, San Mateo, California USA
July 1999

Vibration analyses of advanced technology facilities typically must consider frequency as well as amplitude of vibration. A soil propagation model is proposed which will allow the use of site-specific, measurable, frequency dependent attenuation characteristics. A method is given which allows in-situ determination of those frequency-dependent properties. This approach is applied to the estimation of setback distances for various items of construction equipment at a particular site.

Geotechnical Earthquake Engineering for Highways

Click here for information relating to seismic design of waterfront retaining structures, and current earthquake activity.

FHWA-SA-97-076
May 1997

This document provides information on how to apply principles of geotechnical earthquake engineering to planning, design, and retrofit of highway facilities. Geotechnical earthquake engineering topics discussed in this document include:

  • deterministic and probablistic seismic hazard assessment;
  • evaluation of design ground motions;
  • seismic and site response analyses;
  • evaluation of liquafaction potential and seismic settlements;
  • seismic slope stability and deformation analyses; and
  • seismic design of foundations and retaining structures

Included are basic principles and analyses, with reference to where detailed information on these analysis can be obtained.

Introduction to the Computation of Response Spectrum for Earthquake Loading

Robert M. Ebeling
U.S. Army Corps of Engineers
Technical Report ITL-92-4
June 1992

This technical report presents an introduction to the computation of a linear response spectrum for earthquake loading and defines the terms associated with response spectra. A response spectrum is a graphical relationship of maximum values of acceleration, velocity, and/or displacement response of an infinite series of elastic single degree of freedom (SDOF) systems subjected to time dependent dynamic excitation.

This report reviews the formulation and solution of the equation of motion for a damped linear SDOF system subjected to time dependent dynamic excitation. Due to the irregular nature of the acceleration time histories that have been recorded during earthquakes, numerical methods are used to compute the response of SDOF systems during the course of developing response spectra. The fundamentals of the solution of the equation of motion for SDOF systems are also described.

An Introduction to Wave Propagation in Pavements and Soils--Theory and Practice

R. Scott Ganin, P.E.
Alaska Dept. of Transportation & Public Facilities
AK-RD-91-02
February 1991

This paper introduces the physics and analysis of wave propagation in pavement and soils. The study of wave propagation in soils can yield useful results to engineers concerned with the resilient characteristics of a particular site, dynamic soil-structure interaction (e.g., pavements or soils), and earthquake analysis. Types of waves considered here are those resulting from forced impulses and ground penetrating radar. Background of the development in measuring waves in soils beginning in the late 1930's to the present is given. Practical and useful applications are presented along with equipment necessary to obtain results. Use of wave measuring equipment may expedite soil exploration in the future.

The Mechanism of Liquifaction in Layered Soils

Gregg L. Fiegel and Bruce L. Kutter
Naval Civil Engineering Laboratory CR 92.009
August 1992

Results from six centrifuge model tests are presented. Four of the model tests involve layered soil deposits subject to base shaking; two model tests involve uniform soil deposits of sand subject to base shaking. The layered soil models consisted of a saturated liquefiable fine sand overlain by a layer of relatively impermeable silica flour (silt). Pore water pressures, accelerations, and settlements were measured during all six tests. Results from the model tests involving layered soils suggest that during liquefaction, a water interlayer or very loose zone of soil develops between the sand and the silt due to the difference in permeabilities. Soil volcanos or boils were seen on the surface for all four of these layered model tests. The locations of these boils, in each test, were found concentrated in the weakest zones of the over-lying silt layer; cracking of the weak silt zones provided a release or a vent for the excess pore water pressure generated as a result of particle rearrangement in the liquefiable fine sand.

Models for Prediction of Surface Vibrations from Pile Driving Records

Brent R. Robinson
North Carolina State University
August 2006

This study compares high strain dynamic testing measurements taken near the top of a driven pile to peak particle velocities on the ground surface and sound levels detected in the air some distance from the pile during driving. Based on a sample of installation records from 16 piles driven at the Marquette Interchange Project in Milwaukee, Wisconsin, a series of peak particle velocity plots versus distance, energy and scaled distance were created using traditional horizontal distance and rated hammer energy. These plots were modified using the seismic distance, the diesel hammer potential energy from the calculated stroke, and the energy transferred to the pile top. Incorporating these measurements tended to reduce some of the scatter in the data. More importantly, it was also discovered that components of peak particle velocity in the ground can be well correlated to the total pile resistance measured by dynamic testing. A plot of total resistance versus depth often independently yields the same shape curve as a plot of at least one component of peak particle velocity versus depth. A simple mathematical attenuation model is proposed as an initial step toward utilizing this relationship to predict at least one component of ground motions. Measured peak overpressure (noise) in the air correlated less directly to the quantities measured on the pile, but a conservative and simple mathematical model can still be proposed based on the dynamic testing-measured velocity near the pile top and idealized sound generation and attenuation theories.

a vulcanhammer.net special

Soil Motions Under Vibrating Foundations

This dissertation was co-directed by Spencer J. Buchanan, Distinguished Professor of Soil Mechanics and Foundation Engineering at Texas A&M and before that founder and Chief of the Soil Mechanics Division of the U.S. Army Waterways Experiment Station. The Spencer Buchanan Lecture at Texas A&M, an important lecture in geotechnical engineering, is named in his honour.

John V. Perry taught Mechanical Engineering at Texas A&M for many years. On a lighter note, his department head, C.M. Simmang (who signed off on the dissertation,) was commenting to his class on a visit by the late President Gerald Ford to San Antonio in 1976. Shaking his head in disbelief, he said, "At least I had enough sense to shuck the tamale before I ate it."

John Vivian Perry, Jr.
Texas A&M University
August 1963

This research was undertaken to determine the amount and extent of soil motions under vibrating foundations. The test soil was standard 20-30 Ottawa sand, ASTM C-190, that was contained in a one-meter cubical box. A force generator was mounted above the soil and applied dynamic loads to a circular footing. These were harmonic forces and were applied at frequencies between five and fifty cycles per second.

Three hundred and sixty-seven test runs were recorded on an electromagnetic oscillograph from signals generated by an acceIerometer buried in the soil. This acceIerometer was located at various depths beneath the center of a footing and, at other times, it was located beneath and offcenter. Other variables were the footings which had different diameters and masses.

Three empirical equations were developed from the test results using dimensional analysis. These equations were for maximum values of acceleration, velocity and displacement, respect ively.

a vulcanhammer.net special

Specifications for Control of Vibrations During Blasting and Pile Driving

Pierre Santoni
Northwestern University
December 1993

Controlling environmental effects of civil engineering operations has always been of concern to all parties involved in the construction process. Since control is exercised through the responsibilities outlined in contract specifications, these details are important. This work specifically addresses specifications that incorporate recent developments in the control of external construction vibration effects. These technical vibration specifications are intended to establish controls for the protection of nearby structures from ground vibrations, permanent ground deformation, emission of projectiles, and low frequency air overpressures. Annoyance of neighbors from noise and vibration intrusion also must be taken into account.

An attempt is made in this thesis to present suitable specifications for all types of blasting encountered today in civil engineering projects: production rounds, controlled, close-in and demolition blasting, as well as blast densification of sands. Special chapters deal with vibrations and soil displacement caused by pile driving, and with air overpressures created by both blasting and piling engineering.

The following conclusions are advanced, among others, concerning the geotechnical, the procedural, and the management aspects of vibration control specifications. It is necessary to take vibration considerations into account in the design of the project. This can be accomplished by making preconstruction surveys, by incorporating frequency considerations, and by setting realistic particle velocity limits. The specification should ask the contractor to meet given requirements, but should leave the choice of the method to his ingenuity. Specialists of the operations carried out on the site should be hired by the contractor, and test programs should always be performed before the start of full scale activities. Monitoring of vibration effects, such as peak particle velocity and air overpressures, requires special schemes, especially for pile driving, where two threshold values of particle velocity should be introduced. The engineer should not be considered only as the control authority, but also as a skilled person whose advise on specific problems can be valuable.

a vulcanhammer.net special

Vertical Motion of Rigid Footings

This work is a classic for soil dynamics in general and the response of soil to the vibration of foundations in particular. Lysmer's simplification of the response equation was a major step forward in the rational analysis of this phenomenon.

Lysmer's Analogue--which reduced the soil response of a rigid circular foundation to a single degree of freedom spring-dashpot system--also has found application in pile toe response to pile driving, as was discussed in Closed Form Solution of the Wave Equation for Piles.

John Lysmer was for many years a Professor of Civil Engineering at the University of California at Berkeley. He passed away in 1999.

John Lysmer
U.S. Army Corps of Engineers Contract Report 3-115
University of Michigan
June 1965

This investigation includes a theoretical solution for a rigid footing, resting on an elastic half-space, which is subjected to steady-state vertical oscillation. It is shown how this steady-state solution can be used to describe the response of the footing to a transient pulse-type vertical loading.

After establishing the theoretical solution, and evaluating the approximations required for its development, it is further demonstrated that the theory permits evaluation of quantities which may represent spring constants and damping factors for use in the usual theory for vertical motion of a damped-one-degree-of freedom system. The agreement between the simple theory and elastic half-space theory is well within the limit required for engineering solutions.

The results of the study provide information from which the elastic dynamic response of rigid footings subjected to transient vertical loads may be evaluated. By taking advantage of such standard procedures as the phase-plane method, the dynamic response of footings may still be estimated even if the stresses in the soil extend into the inelastic range. A detailed discussion of the application of this method to inelastic settlements of vertically loaded footings will be presented in a subsequent report.

Finally, the theoretical developments included in this report for vertical oscillations may serve as a guide to develop similar theoretical evaluations of the dynamic response of rigid footings in other uncoupled modes of oscillation.

PHP RSS ReaderUSGS M5+ Earthquakes

Real-time, worldwide earthquake list for the past 7 days

M 5.3, eastern Sichuan, China

May 14, 2008 09:26:44 GMT

M 5.1, Sichuan-Gansu border region, China

May 14, 2008 05:54:59 GMT

M 5.4, eastern Sichuan, China

May 14, 2008 02:54:38 GMT

M 5.1, Molucca Sea

May 13, 2008 22:44:50 GMT

M 5.3, Luzon, Philippines

May 13, 2008 21:48:33 GMT

M 5.0, Kuril Islands

May 13, 2008 20:20:43 GMT

M 5.2, Luzon, Philippines

May 13, 2008 14:14:30 GMT

M 5.0, Sichuan-Gansu border region, China

May 13, 2008 12:51:38 GMT

M 5.4, northern Sumatra, Indonesia

May 13, 2008 10:29:19 GMT

M 5.0, Sichuan-Gansu border region, China

May 13, 2008 07:53:02 GMT

M 5.0, Sichuan-Gansu border region, China

May 13, 2008 07:19:16 GMT

M 5.8, eastern Sichuan, China

May 13, 2008 07:07:08 GMT

M 5.2, South Sandwich Islands region

May 13, 2008 03:37:11 GMT

M 5.0, eastern Sichuan, China

May 13, 2008 03:00:38 GMT

M 5.3, eastern Sichuan, China

May 12, 2008 23:54:47 GMT

M 5.4, eastern Sichuan, China

May 12, 2008 23:46:19 GMT

M 5.0, Taiwan region

May 12, 2008 22:57:46 GMT

M 5.3, eastern Sichuan, China

May 12, 2008 20:45:31 GMT

M 5.6, eastern Sichuan, China

May 12, 2008 20:08:48 GMT

M 5.1, eastern Sichuan, China

May 12, 2008 17:54:32 GMT

M 5.1, eastern Sichuan, China

May 12, 2008 15:28:53 GMT

M 5.1, eastern Sichuan, China

May 12, 2008 15:05:31 GMT

M 5.1, Sichuan-Gansu border region, China

May 12, 2008 14:46:07 GMT

M 5.1, Sichuan-Gansu border region, China

May 12, 2008 14:15:26 GMT

M 5.1, Kodiak Island region, Alaska

May 12, 2008 12:50:34 GMT

M 5.8, eastern Sichuan, China

May 12, 2008 11:11:02 GMT

M 5.1, eastern Sichuan, China

May 12, 2008 10:23:40 GMT

M 5.0, northern Mid-Atlantic Ridge

May 12, 2008 09:52:12 GMT

M 5.5, eastern Sichuan, China

May 12, 2008 09:42:25 GMT

M 5.1, eastern Sichuan, China

May 12, 2008 09:07:00 GMT

M 5.0, Sichuan-Gansu border region, China

May 12, 2008 08:47:25 GMT

M 5.2, eastern Sichuan, China

May 12, 2008 08:21:40 GMT

M 5.2, eastern Sichuan, China

May 12, 2008 08:10:59 GMT

M 5.4, eastern Sichuan, China

May 12, 2008 07:34:42 GMT

M 5.7, eastern Sichuan, China

May 12, 2008 06:54:18 GMT

M 6.0, eastern Sichuan, China

May 12, 2008 06:43:14 GMT

M 7.9, eastern Sichuan, China

May 12, 2008 06:28:01 GMT

M 5.0, northern Mid-Atlantic Ridge

May 11, 2008 21:01:08 GMT

M 5.3, Hindu Kush region, Afghanistan

May 11, 2008 20:57:07 GMT

M 5.1, Tonga

May 11, 2008 05:49:22 GMT

M 5.0, southern Greece

May 10, 2008 20:53:01 GMT

M 5.6, Taiwan region

May 10, 2008 19:41:58 GMT

M 5.1, Hokkaido, Japan region

May 10, 2008 18:24:02 GMT

M 5.0, Volcano Islands, Japan region

May 10, 2008 13:32:50 GMT

M 6.7, Guam region

May 09, 2008 21:51:29 GMT

M 5.5, near the east coast of Honshu, Japan

May 08, 2008 23:21:07 GMT

M 5.0, Andreanof Islands, Aleutian Islands, Alaska

May 08, 2008 14:12:55 GMT

M 5.0, northern Sumatra, Indonesia

May 08, 2008 11:31:29 GMT

M 5.2, Antofagasta, Chile

May 08, 2008 00:27:22 GMT

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