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.
Overview
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.
Audience
Contents
Structure
Scope Summary:
| Wave Type | Source Examples |
|---|---|
| P-wave | Air gun, explosives, sparker, downhole hammer, piezoelectric vibrator, magnetostrictive source |
| SH-wave | Downhole hammer, piezoelectric vibrator |
| SV-wave | Explosives, air gun, sparker, downhole hammer, piezoelectric vibrator |
Reports must include:
[ E_d = \rho V_p^2 (1 + \nu)(1 - 2\nu) / (1 - \nu) ]
Where:
IS 13372 Part 2: Key Definitions, Formulas & Tables
| Wave Type | Typical Sources |
|---|---|
| P wave | Air gun, explosives, sparker, downhole hammer, piezoelectric vibrator, magnetostrictive source |
| SH wave | Downhole hammer, piezoelectric vibrator |
| SV wave | Explosives, air gun, sparker, downhole hammer, piezoelectric vibrator |
Given:
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) ]
IS 13372 Part 2: Principle of Test Method (Seismic Testing Between Boreholes)
| Wave Type | Seismic Source Examples |
|---|---|
| P-wave | Air gun, explosives, sparker, downhole hammer, piezoelectric vibrator, magnetostrictive source |
| SH-wave | Downhole hammer, piezoelectric vibrator |
| SV-wave | Explosives, air gun, sparker, downhole hammer, piezoelectric vibrator |
[ V = \frac{L}{t} ]
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.
IS 13372 Part 2: Apparatus for Seismic Testing
| Apparatus | Details |
|---|---|
| Seismic Source | Select based on wave type: |
| - P wave | Air gun, explosives, sparker, downhole hammering device, piezoelectric vibrator, magnetostrictive source |
| - SH wave | Downhole hammering device, piezoelectric vibrator |
| - SV wave | Explosives, air gun, sparker, downhole hammering device, piezoelectric vibrator |
| Seismic Receiver | Types: |
| - Geophone | Voltage ∝ particle velocity; freq. range 10 Hz–2 kHz; natural freq. < 0.5 × predominant wave freq. |
| - Piezoelectric accelerometer | Voltage ∝ particle acceleration; freq. range 10 Hz–60 kHz; natural freq. ≥ 2 × predominant wave freq. |
| - Hydrophone | Voltage ∝ water pressure; freq. range 10 Hz–60 kHz; only for water-filled boreholes |
| Receiver Array | Triaxial array: 1 vertical + 2 horizontal receivers at right angles for wave identification |
| Mounting Equipment | For source/receiver installation and borehole surveying (spacing, depth, deviation) |
| Data Acquisition System | Includes: |
| - Amplifier | Gain 70–130 dB; flat freq. response 4 Hz–2 kHz |
| - Signal enhancement | For noisy environments or wide spacing |
| - 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 common |
| Wave Type | Sources |
|---|---|
| P wave | Air gun, explosives, sparker, downhole hammer, piezoelectric vibrator, magnetostrictive source |
| SH wave | Downhole hammer, piezoelectric vibrator |
| SV wave | Explosives, air gun, sparker, downhole hammer, |
IS 13372 Part 2 - Seismic Test Procedure Key Points
| Wave Type | Sources |
|---|---|
| P wave | air gun, explosives, sparker, downhole hammer, piezoelectric vibrator, magnetostrictive source |
| SH wave | downhole hammer, piezoelectric vibrator |
| SV wave | explosives, air gun, sparker, downhole hammer, piezoelectric vibrator |
Receivers:
Data Acquisition System:
Reports must include:
[ V = \frac{D}{t} ]
graph LR
A[Seismic Source] --> B[B
IS 13372 Part 2: Calculation and Interpretation Summary
| Parameter | Formula / 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 Velocity | Typical P-wave velocity ~ 3.5 km/s (Table 2.5) |
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.
IS 13372 Part 2: Reporting of Results (Clause 7)
The report for seismic testing between boreholes must include:
[ E_d = \rho V_p^2 (1 + \nu)(1 - 2\nu) / (1 - \nu) ]
Where:
| Wave Type | Sources |
|---|---|
| P-wave | Air gun, explosives, sparker, downhole hammer, piezoelectric vibrator, magnetostrictive source |
| SH-wave | Downhole hammer, piezoelectric vibrator |
| SV-wave | Explosives, air gun, sparker, downhole hammer, piezoelectric vibrator |
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.
Frequently Asked
Recommended Seismic Sources for Crosshole Testing (IS 13372 Part 2, Clause 4.1 & Table 1):
| Wave Type | Recommended Sources |
|---|---|
| P-wave | Air gun, explosives, sparker, downhole hammering device, piezoelectric vibrator, magnetostrictive source |
| SH-wave | Downhole hammering device, piezoelectric vibrator |
| SV-wave | Explosives, air gun, sparker, downhole hammering device, piezoelectric vibrator |
Loading diagram...
This ensures effective generation of required seismic waves for crosshole velocity measurements.
Measurement of P and S Wave Velocities Between Boreholes (IS 13372 Part 2)
Travel Time Measurement (Clause 6.1):
Velocity Calculation (Clause 6.2):
[
V = \frac{D}{t}
]
where:
Borehole Setup (Clause 5.1 & 5.4):
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This method ensures accurate estimation of seismic wave velocities between boreholes for subsurface characterization.
Equipment Required for Accurate Seismic Data Acquisition (IS 13372 Part 2)
Seismic Source
Seismic Receivers
Mounting & Surveying Equipment
Data Acquisition System
| Wave Type | Typical Sources |
|---|---|
| P wave | Air gun, explosives, sparker, downhole hammer, piezo vibrator, magnetostrictive source |
| SH wave | Downhole hammer, piezo vibrator |
| SV wave | Explosives, air gun, sparker, downhole hammer, piezo vibrator |
Loading diagram...
Note: Boreholes should be surveyed precisely; receivers must maintain firm
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:
[ \nu = \frac{(V_p/V_s)^2 - 2}{2[(V_p/V_s)^2 - 1]} ]
[ G_d = \rho V_s^2 = \frac{E_d}{2(1 + \nu)} ]
[ K_d = \rho \left(V_p^2 - \frac{4}{3} V_s^2 \right) = \frac{E_d}{3(1 - 2\nu)} ]
[ 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) ]
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This method provides a reliable estimate of rock mass dynamic elastic properties for geotechnical
Best Practices for Borehole Drilling and Receiver Placement (IS 13372 Part 2)
Borehole Location & Drilling (Clause 5.1):
Receiver Placement (Clause 5.2):
Measurement Interval (Clause 5.4):
| Aspect | Best Practice |
|---|---|
| Hole casing | Prefer uncased; if cased, use low-velocity PVC, well-grouted |
| Hole spacing | Determined by project; avoid too large spacing |
| Hole survey accuracy | Precisely survey position, depth, deviation |
| Receiver contact | Firm contact with hole wall; suspension in water |
| Receiver array | Triaxial (1 vertical + 2 horizontal) |
| Measurement interval | 0.5 to 5.0 m |
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