IS 13372 Part 21992AI Search Enabled✦ AI Generated

Code of practice for seismic testing of rock mass, Part 2: Between the borehole

IS 13372 Part 2:1992 specifies the code of practice for seismic testing of rock masses between boreholes, commonly known as the crosshole seismic method. It guides engineers in measuring P and S wave velocities and attenuation to evaluate dynamic elastic properties and rock mass quality, essential for geotechnical and earthquake engineering applications. This standard is applicable to professionals conducting seismic investigations to assess rock mass characteristics and mechanical properties in situ.

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1992Edition
Rock MechanicsCategory
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What This Standard Covers

IS 13372 Part 2:1992 specifies the code of practice for seismic testing of rock masses between boreholes, commonly known as the crosshole seismic method. It guides engineers in measuring P and S wave velocities and attenuation to evaluate dynamic elastic properties and rock mass quality, essential for geotechnical and earthquake engineering applications. This standard is applicable to professionals conducting seismic investigations to assess rock mass characteristics and mechanical properties in situ.

Who Uses This Standard

  • Geotechnical Engineers
  • Rock Mechanics Specialists
  • Seismologists
  • Civil Engineers
  • Geologists
  • Earthquake Engineering Consultants
  • Construction Project Managers

Key Topics Covered

Crosshole seismic testing methodology
Measurement of P and S wave velocities
Seismic source and receiver equipment specifications
Borehole drilling and positioning requirements
Data acquisition and signal recording techniques
Calculation of dynamic elastic moduli
Quality factor (Q) and wave attenuation
Interpretation of seismic velocity variations
Reporting requirements and documentation
Wave types and particle motion characteristics
Surveying and borehole alignment accuracy
Use of triaxial receiver arrays
Frequency response and sensitivity of equipment

Table of Contents

1Scope

IS 13372 Part 2: Scope - Key Specifications & Tables

Scope Summary:

  • Defines seismic testing between boreholes for rock mass evaluation.
  • Covers apparatus, measurement methods, data reporting, and evaluation.
  • Applicable to seismic wave velocity measurement (P, SH, SV waves).

Key Tables & Formulas

Table 1: Seismic Sources for Crosshole Measurement

Wave TypeSource Examples
P-waveAir gun, explosives, sparker, downhole hammer, piezoelectric vibrator, magnetostrictive source
SH-waveDownhole hammer, piezoelectric vibrator
SV-waveExplosives, air gun, sparker, downhole hammer, piezoelectric vibrator

Apparatus Requirements (Clause 4.1)

  • Seismic Source: Select based on wave type (see Table 1).
  • Seismic Receiver:
    • Geophone (velocity-sensitive, 10 Hz–2 kHz)
    • Piezoelectric accelerometer (acceleration-sensitive, 10 Hz–60 kHz)
    • Hydrophone (pressure-sensitive, water-filled boreholes only)
  • Receiver Array: Triaxial (1 vertical + 2 horizontal) for wave identification.
  • Data Acquisition System:
    • Amplifier (Gain 70–130 dB, freq. 4 Hz–2 kHz)
    • Signal enhancement for noisy environments
    • Timing device (0.1, 1, or 10 ms intervals)
    • Time break unit (separate channel)
    • Recorder (analog/digital visual record)

Reporting Requirements (Clause 7)

Reports must include:

  • Borehole details: location, length, diameter, inclination, casing.
  • Drawings: seismic source/receiver positions with coordinates.
  • Equipment specs & measurement methods.
  • Waveforms for each source-receiver pair.
  • Average propagation velocities between points.
  • Dynamic elastic modulus tabulation.
  • Equations and assumptions used.
  • Geotechnical interpretation if required.

Velocity & Elastic Modulus Relation (General)

[ E_d = \rho V_p^2 (1 + \nu)(1 - 2\nu) / (1 - \nu) ]

Where:

  • (E_d) = Dynamic elastic modulus
  • (\rho) = Rock density
  • (V
2Definitions

IS 13372 Part 2: Key Definitions, Formulas & Tables


1. Definitions (Clause 2.0)

  • The standard defines terms related to seismic testing between boreholes.
  • Key terms include seismic source types, receivers, wave velocities, and dynamic elastic parameters.

2. Seismic Source Types (Table 1, Clause 4.1)

Wave TypeTypical Sources
P waveAir gun, explosives, sparker, downhole hammer, piezoelectric vibrator, magnetostrictive source
SH waveDownhole hammer, piezoelectric vibrator
SV waveExplosives, air gun, sparker, downhole hammer, piezoelectric vibrator

3. Dynamic Elastic Parameters (Clause 6.4)

Given:

  • ( P ) = density of rock (kg/m³)
  • ( V_p ) = P-wave velocity (m/s)
  • ( V_s ) = S-wave velocity (m/s)

Formulas:

[ \textbf{Dynamic Poisson's ratio, } \nu = \frac{(V_p/V_s)^2 - 2}{2((V_p/V_s)^2 - 1)} ]

[ \textbf{Dynamic modulus of rigidity, } G_d = P V_s^2 = \frac{E_d}{2(1 + \nu)} ]

[ \textbf{Dynamic bulk modulus, } K_d = P \left(V_p^2 - \frac{4}{3} V_s^2 \right) = \frac{E_d}{3(1 - 2\nu)} ]

[ \textbf{Dynamic Young's modulus, } E_d = 2 G_d (1 + \nu) = 3 K_d (1 - 2\nu) ]


4. Reporting Velocity (Clause 2.5, Table 7)

  • Typical velocity for reporting: 3.5 km/sec (3,500 m/s)

5. Seismic Testing Setup (Clause 4.1)

  • Use triaxial receivers (vertical + two horizontal at right angles).
  • Frequency range: 10 Hz to 2 kHz (general purpose).
3Principle of Test Method

IS 13372 Part 2: Principle of Test Method (Seismic Testing Between Boreholes)

Key Concept:

  • Measure seismic wave velocity between boreholes by generating waves at a source borehole and recording arrival times at receiver boreholes.
  • Compare measured velocities with expected values to evaluate rock mass properties (Clause 6.6).

Apparatus & Sources (Clause 4.1 & Table 1):

Wave TypeSeismic Source Examples
P-waveAir gun, explosives, sparker, downhole hammer, piezoelectric vibrator, magnetostrictive source
SH-waveDownhole hammer, piezoelectric vibrator
SV-waveExplosives, air gun, sparker, downhole hammer, piezoelectric vibrator

Receivers:

  • Geophone: Voltage ∝ particle velocity (10 Hz–2 kHz), natural freq < ½ predominant wave freq.
  • Piezoelectric accelerometer: Voltage ∝ acceleration (10 Hz–60 kHz), natural freq ≥ 2× predominant wave freq.
  • Hydrophone: For water-filled boreholes, voltage ∝ water pressure (10 Hz–60 kHz).

Basic Formula for Velocity:

[ V = \frac{L}{t} ]

  • V: Wave velocity (m/s)
  • L: Distance between source and receiver (m)
  • t: Travel time of seismic wave (s)

Reporting Requirements (Clause 7):

  • Borehole details (location, length, diameter, inclination)
  • Seismic source & receiver positions and coordinates
  • Equipment specs & frequency characteristics
  • Waveforms and computed average velocities (see Fig. 3)
  • Dynamic elastic modulus tabulation
  • Equations and assumptions used
  • Geotechnical interpretation considering geology

Summary Diagram:

flowchart LR
    A[Seismic Source in Borehole] --> B[Seismic Wave Propagation]
    B --> C[Receivers in Other Boreholes]
    C --> D[Record Arrival Times]
    D --> E[Calculate Velocity V = L/t]
    E --> F[Evaluate Rock Mass Properties]

Note: Use a triaxial array of receivers (vertical + 2 horizontal) for wave identification. Frequency band typically 10 Hz–2 kHz for general crosshole tests.

4Apparatus

IS 13372 Part 2: Apparatus for Seismic Testing

Key Apparatus and Specifications (Clause 4.1):

ApparatusDetails
Seismic SourceSelect based on wave type:
- P waveAir gun, explosives, sparker, downhole hammering device, piezoelectric vibrator, magnetostrictive source
- SH waveDownhole hammering device, piezoelectric vibrator
- SV waveExplosives, air gun, sparker, downhole hammering device, piezoelectric vibrator
Seismic ReceiverTypes:
- GeophoneVoltage ∝ particle velocity; freq. range 10 Hz–2 kHz; natural freq. < 0.5 × predominant wave freq.
- Piezoelectric accelerometerVoltage ∝ particle acceleration; freq. range 10 Hz–60 kHz; natural freq. ≥ 2 × predominant wave freq.
- HydrophoneVoltage ∝ water pressure; freq. range 10 Hz–60 kHz; only for water-filled boreholes
Receiver ArrayTriaxial array: 1 vertical + 2 horizontal receivers at right angles for wave identification
Mounting EquipmentFor source/receiver installation and borehole surveying (spacing, depth, deviation)
Data Acquisition SystemIncludes:
- AmplifierGain 70–130 dB; flat freq. response 4 Hz–2 kHz
- Signal enhancementFor noisy environments or wide spacing
- Timing deviceTime marks at 0.1, 1, or 10 ms intervals
- Time break unitSeparate channel for wave generation instant
- RecorderAnalog/digital visual record; electromagnetic oscillograph common

Typical Frequency Band:

  • General crosshole: 10 Hz – 2 kHz
  • Detailed studies: Higher frequencies required

Table 1: Seismic Sources for Crosshole Testing

Wave TypeSources
P waveAir gun, explosives, sparker, downhole hammer, piezoelectric vibrator, magnetostrictive source
SH waveDownhole hammer, piezoelectric vibrator
SV waveExplosives, air gun, sparker, downhole hammer,
5Test Procedure

IS 13372 Part 2 - Seismic Test Procedure Key Points

Apparatus (Clause 4.1)

  • Seismic Sources (Table 1):
Wave TypeSources
P waveair gun, explosives, sparker, downhole hammer, piezoelectric vibrator, magnetostrictive source
SH wavedownhole hammer, piezoelectric vibrator
SV waveexplosives, air gun, sparker, downhole hammer, piezoelectric vibrator
  • Receivers:

    • Geophone: voltage ∝ particle velocity, freq. range 10 Hz–2 kHz, natural freq < 0.5 × predominant freq.
    • Piezoelectric accelerometer: voltage ∝ acceleration, freq. range 10 Hz–60 kHz, natural freq ≥ 2 × predominant freq.
    • Hydrophone: voltage ∝ water pressure, freq. range 10 Hz–60 kHz (water-filled boreholes only).
    • Use triaxial arrays (1 vertical + 2 horizontal receivers at right angles) for wave identification.
  • Data Acquisition System:

    • Amplifier gain: 70–130 dB, flat freq. response 4 Hz–2 kHz.
    • Signal enhancement for noisy areas.
    • Timing device: time marks at 0.1, 1, or 10 ms intervals.
    • Time break unit: separate channel for wave generation instant.
    • Recorder: analog/digital visual record (electromagnetic oscillograph preferred).

Reporting (Clause 7)

Reports must include:

  • Borehole details (location, length, diameter, inclination, casing).
  • Layout drawings with source/receiver coordinates.
  • Equipment specs and frequency characteristics.
  • Waveforms for all source-receiver pairs.
  • Average propagation velocities (see Fig. 3 schematic).
  • Dynamic elastic modulus tabulation.
  • Equations and assumptions used.
  • Geotechnical interpretation if required.

Formula for Velocity (basic):

[ V = \frac{D}{t} ]

  • (V) = seismic wave velocity (m/s)
  • (D) = distance between source and receiver (m)
  • (t) = travel time of wave (s)

Simplified Mermaid Diagram of Setup

graph LR
  A[Seismic Source] --> B[B
6Calculation and Interpretation

IS 13372 Part 2: Calculation and Interpretation Summary

Key Points from Clause 6 (Calculation and Interpretation):

  • Signal Recording: Signals from receivers must be recorded on magnetic media or displayed visually with adequate amplitude and travel time for accurate reading.
  • Velocity Calculation: Average seismic wave velocities are computed between shot points and receiving points, including between boreholes.
  • Rock Properties: Compare measured velocities with specimen velocities to evaluate rock mass properties.
  • Dynamic Elastic Modulus: Compute and tabulate dynamic elastic modulus values from seismic velocities.

Important Formulas & Tables:

ParameterFormula / Notes
Average Velocity (V)( V = \frac{L}{t} ) where L = distance (m), t = travel time (s)
Dynamic Elastic Modulus (E_d)( E_d = \rho V^2 (1 + \nu)(1 - 2\nu) / (1 - \nu) ) (for isotropic materials) where: <br> (\rho) = density, (\nu) = Poisson's ratio
Reporting VelocityTypical P-wave velocity ~ 3.5 km/s (Table 2.5)

Reporting Requirements (Clause 7):

  • Borehole details (location, length, diameter, inclination)
  • Positions and coordinates of seismic sources and receivers
  • Measurement methods and equipment specs
  • Waveforms and average velocities (see Fig. 3 schematic)
  • Dynamic elastic modulus tabulation
  • Equations and assumptions used
  • Geotechnical interpretation considering geology

Schematic Concept (Fig. 3):

flowchart LR
    A[Shot Point] -->|Seismic Wave| B[Receiver Point]
    B -->|Travel Time t| C[Calculate Velocity V = L/t]
    C --> D[Compare with Specimen Velocity]
    D --> E[Evaluate Rock Mass Properties]

Summary: Use travel time and distance to calculate seismic velocities, then derive dynamic elastic modulus to interpret rock mass properties. Report comprehensive data including borehole info, equipment, waveforms, velocities, and analysis assumptions.

7Reporting of the Results

IS 13372 Part 2: Reporting of Results (Clause 7)

The report for seismic testing between boreholes must include:

  • Borehole details: Location, length, diameter, direction, inclination, casing/cement details.
  • Drawings: Positions of seismic sources and receivers with coordinates.
  • Equipment & Methods: Description, specifications, and frequency characteristics.
  • Waveforms: For each source-receiver pair.
  • Average propagation velocities: Between shot and receiver points (see Fig. 3 schematic).
  • Dynamic elastic modulus: Tabulated computed values.
  • Equations & assumptions: Used beyond the standard method.
  • Geotechnical interpretation: Geological context and analysis (if required).

Key Formula for Dynamic Elastic Modulus (E_d):

[ E_d = \rho V_p^2 (1 + \nu)(1 - 2\nu) / (1 - \nu) ]

Where:

  • ( \rho ) = density of rock mass
  • ( V_p ) = P-wave velocity
  • ( \nu ) = Poisson's ratio

Table: Seismic Source Types (from Clause 4.1)

Wave TypeSources
P-waveAir gun, explosives, sparker, downhole hammer, piezoelectric vibrator, magnetostrictive source
SH-waveDownhole hammer, piezoelectric vibrator
SV-waveExplosives, air gun, sparker, downhole hammer, piezoelectric vibrator

Fig. 3 Concept: Average Velocity Calculation

flowchart LR
    A[Shot Point] -->|Seismic Wave| B[Receiver Point]
    B -->|Travel Time t| C[Calculate Velocity V = Distance / t]
    C --> D[Tabulate Average Velocities]

Note: Use magnetic recording for signal accuracy (Clause 5.5). Include time break signals for precise travel time measurement.

This structured reporting ensures consistency, clarity, and facilitates geotechnical interpretation of seismic test results.

Popular Questions About IS 13372 Part 2

?What types of seismic sources are recommended for crosshole testing?

Recommended Seismic Sources for Crosshole Testing (IS 13372 Part 2, Clause 4.1 & Table 1):

Wave TypeRecommended Sources
P-waveAir gun, explosives, sparker, downhole hammering device, piezoelectric vibrator, magnetostrictive source
SH-waveDownhole hammering device, piezoelectric vibrator
SV-waveExplosives, air gun, sparker, downhole hammering device, piezoelectric vibrator

Key Points:

  • Source selection depends on wave type required (P, SH, or SV).
  • Sources can be explosive, mechanical, or electrical.
  • Crosshole testing typically uses frequencies from 10 Hz to 2 kHz.
  • Receivers should have matching frequency response and sensitivity.

Summary:

  • Use explosives or air guns for strong P and SV waves.
  • Use downhole hammering or piezoelectric vibrators for SH waves.
  • Choose source based on site conditions, wave type, and desired frequency content.
Loading diagram...

This ensures effective generation of required seismic waves for crosshole velocity measurements.

?How are P and S wave velocities measured between boreholes?

Measurement of P and S Wave Velocities Between Boreholes (IS 13372 Part 2)

  • Travel Time Measurement (Clause 6.1):

    • Measure time from the time break to the first break of P and S waves on the seismogram.
    • For multiple receivers on the same ray path, measure time difference between their first breaks.
    • For S waves, use the predominant phase travel time.
  • Velocity Calculation (Clause 6.2):
    [ V = \frac{D}{t} ] where:

    • (V) = average velocity (P or S wave)
    • (D) = distance between source and receiver or between receivers
    • (t) = measured travel time between these points
  • Borehole Setup (Clause 5.1 & 5.4):

    • Preferably use uncased boreholes or low-velocity PVC casing, well-grouted for good contact.
    • Borehole spacing affects wave type detected; larger spacing may capture refracted waves.
    • Survey hole positions accurately to determine coordinates of sources and receivers.
    • Measurement intervals (source/receiver spacing) typically 0.5–5.0 m for accuracy.
Loading diagram...

This method ensures accurate estimation of seismic wave velocities between boreholes for subsurface characterization.

?What equipment is required for accurate seismic data acquisition?

Equipment Required for Accurate Seismic Data Acquisition (IS 13372 Part 2)

  1. Seismic Source

    • Types depend on wave type (P, SH, SV).
    • Examples: explosives, air gun, sparker, downhole hammering device, piezoelectric vibrator, magnetostrictive source.
    • Select based on required wave type (see Table 1).
  2. Seismic Receivers

    • Geophones: Voltage ∝ particle velocity; frequency 10 Hz–2 kHz; natural frequency < ½ predominant frequency.
    • Piezoelectric accelerometers: Voltage ∝ particle acceleration; frequency 10 Hz–60 kHz; natural frequency ≥ 2× predominant frequency.
    • Hydrophones: For water-filled boreholes; voltage ∝ water pressure; frequency 10 Hz–60 kHz.
    • Use triaxial arrays (1 vertical + 2 horizontal receivers at right angles).
  3. Mounting & Surveying Equipment

    • For positioning sources and receivers in boreholes and surveying hole spacing, depth, direction, deviation.
  4. Data Acquisition System

    • Amplifier (gain 70-130 dB; flat 4 Hz–2 kHz).
    • Signal enhancement unit for noisy environments.
    • Accurate timing device (time marks at 0.1, 1, or 10 ms).
    • Time break unit (separate channel for wave generation instant).
    • Recorder (analog/digital/oscillograph).

Summary Table: Seismic Source vs Wave Type

Wave TypeTypical Sources
P waveAir gun, explosives, sparker, downhole hammer, piezo vibrator, magnetostrictive source
SH waveDownhole hammer, piezo vibrator
SV waveExplosives, air gun, sparker, downhole hammer, piezo vibrator

Loading diagram...

Note: Boreholes should be surveyed precisely; receivers must maintain firm

?How is the dynamic elastic modulus of rock mass calculated from seismic data?

According to IS 13372 Part 2 (Clause 6.4), the dynamic elastic modulus of rock mass is calculated from seismic data using P-wave velocity (Vp), S-wave velocity (Vs), and rock density (ρ). The key formulas are:

Key Parameters and Formulas:

  • Dynamic Poisson's ratio (ν):

[ \nu = \frac{(V_p/V_s)^2 - 2}{2[(V_p/V_s)^2 - 1]} ]

  • Dynamic modulus of rigidity (Shear modulus), ( G_d ):

[ G_d = \rho V_s^2 = \frac{E_d}{2(1 + \nu)} ]

  • Dynamic bulk modulus, ( K_d ):

[ K_d = \rho \left(V_p^2 - \frac{4}{3} V_s^2 \right) = \frac{E_d}{3(1 - 2\nu)} ]

  • Dynamic Young's modulus, ( E_d ):

[ E_d = G_d \times 2(1 + \nu) = 3 K_d (1 - 2\nu) ]

or directly from velocities:

[ E_d = \rho V_s^2 \times 2(1 + \nu) ]

Procedure Summary:

  • Measure Vp, Vs between boreholes using crosshole seismic testing.
  • Determine rock density ( \rho ).
  • Calculate Poisson's ratio ( \nu ) using velocities.
  • Calculate ( G_d ), ( K_d ), and finally ( E_d ) using above formulas.
  • Report values in MPa or GPa.

Visual summary:

Loading diagram...

This method provides a reliable estimate of rock mass dynamic elastic properties for geotechnical

?What are the best practices for borehole drilling and receiver placement in this method?

Best Practices for Borehole Drilling and Receiver Placement (IS 13372 Part 2)

  • Borehole Location & Drilling (Clause 5.1):

    • Drill test holes at suitable locations considering topography and geology.
    • Prefer uncased holes; if cased, use low-velocity casing (e.g., high-impact PVC) well-grouted for intimate contact.
    • Number and spacing depend on project nature; avoid excessive spacing to reduce refracted wave measurements.
    • Survey hole positions, directions, depths, and deviations precisely.
  • Receiver Placement (Clause 5.2):

    • Install seismic source in one borehole; receivers in others at required depths.
    • Receivers must be firmly in contact with hole walls, except in water-filled holes where suspension receivers may be used.
    • Use triaxial receiver arrays (vertical + two orthogonal horizontals) for wave identification.
  • Measurement Interval (Clause 5.4):

    • Interval (receiver spacing or relocation) generally 0.5–5.0 m, based on accuracy and efficiency requirements.

Summary Table for Borehole & Receiver Setup

AspectBest Practice
Hole casingPrefer uncased; if cased, use low-velocity PVC, well-grouted
Hole spacingDetermined by project; avoid too large spacing
Hole survey accuracyPrecisely survey position, depth, deviation
Receiver contactFirm contact with hole wall; suspension in water
Receiver arrayTriaxial (1 vertical + 2 horizontal)
Measurement interval0.5 to 5.0 m
Loading diagram...

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