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Gold
Product Description
Next Generation Downhole Seismic: Why the Borehole 3C Geophone Leads the Market
The global demand for high resolution subsurface imaging is growing faster than ever. Carbon capture projects require decades of monitoring. Geothermal energy expansion needs precise fracture mapping. Critical mineral exploration demands discovery at greater depths. At the center of these trends stands a proven tool: the Borehole 3C Geophone. This instrument, available in electromagnetic (GDJ DJ), piston type (GDJ JG), and non adjacent (GDJ JF) series, represents the current state of the art in downhole seismic sensing. Let us explore why it dominates and how it will evolve.
Trend One: Smaller Diameter for Deeper and Tighter Holes
Exploration drill holes are getting narrower to reduce drilling costs. The industry standard has moved from HQ to NQ and even BQ sizes. Our GDJ JF non adjacent borehole geophone has an outer diameter of only 45 millimeters. This fits through NQ rods (approximately 60 mm inner diameter) and even some BQ sizes. The electromagnetic and piston models at 55 and 50 millimeters also remain competitive. Future versions may shrink further, but today this is the smallest practical three component borehole geophone on the market.
Trend Two: Lighter Equipment for Remote Operations
Field crews in jungles, deserts, and arctic regions cannot carry heavy tools. Weight reduction is a major innovation driver. The GDJ JF non adjacent model with 60 meter cable weighs only 6 kilograms. That is lighter than a typical suitcase. The GDJ DJ at 10 kilograms and GDJ JG at 12 kilograms are still significantly lighter than older generation tools that often exceeded 25 kilograms. Lower weight means lower shipping costs, safer handling, and faster mobilization.
Trend Three: High Temperature Tolerance for Geothermal and Deep Wells
As wells go deeper, temperatures rise. Many conventional geophones fail above 40 degrees Celsius. Our Borehole 3C Geophone operates up to 55 degrees Celsius. This covers most sedimentary basins and geothermal fields. For higher temperatures, future designs may push to 70 or 80 degrees Celsius. But for current projects, 55C is sufficient for the majority of borehole seismic surveys.
Trend Four: Flexible Frequency for Multi Scale Imaging
The ability to select any frequency from 4Hz to 100Hz allows one tool to serve both deep regional studies and shallow high resolution profiles. A mining company exploring for a deep ore body can order the geophone with a 4Hz sensor. The same company can later use a 100Hz sensor for detailed near borehole imaging. This flexibility reduces equipment inventory. Future trends may push frequencies lower than 4Hz or higher than 100Hz, but the current range already covers 95 percent of applications.
Trend Five: Multiple Coupling Mechanisms for Any Borehole Condition
No single coupling method works everywhere. That is why we offer three distinct series. Electromagnetic coupling (GDJ DJ) works in steel cased holes and provides repeatable clamping. Piston coupling (GDJ JG) works in open hard rock holes and gives strong wall contact. Non adjacent coupling (GDJ JF) works in soft formations, PVC casing, and deviated wells. This tri design approach matches the diversity of real world boreholes. Future tools may add active clamping or robotic centering, but the current three way split already solves most problems.
Repeating the Core Technical Selling Points for Future Buyers
Engineers planning next year‘s surveys need to remember these specifications: three component (full vector wavefield), 4 to 100Hz frequency (adjustable to target depth), 45 to 55 mm diameter (fits narrow holes), 300 to 500 mm height (short enough for deviated wells), 6 to 17 kg weight (light enough for manual handling), 55 degree Celsius maximum (adequate for most deep boreholes), and three coupling choices (one for every borehole type).
Parameter Table as a Reference for Technology Planners
| Model | GDJ DJ | GDJ JG | GDJ JF |
|---|---|---|---|
| Series Type | Electromagnetic Borehole Geophone | Piston Type Borehole Geophone | Non Adjacent Borehole Geophone |
| Frequency (Hz) | 4 to 100 Optional | 4 to 100 Optional | 4 to 100 Optional |
| Working Mini Diameter (mm) | 70 to 120 | 50 to 110 | None Required |
| Working Temperature (C) | 25 to 55 | 25 to 55 | 25 to 55 |
| Tool Diameter (mm) | 55 | 50 | 45 |
| Tool Height (mm) | 465 | 500 | 300 |
| Weight 60m Cable (kg) | 10 | 12 | 6 |
| Weight 120m Cable (kg) | 14 | 17 | 10 |
What the Next Five Years Will Bring
We anticipate three improvements. First, even smaller diameters approaching 38 millimeters. Second, higher temperature versions rated to 70 degrees Celsius. Third, wireless telemetry for real time data transmission. But until those arrive, the current Borehole 3C Geophone series remains the best choice for cost effective, reliable downhole seismic acquisition. Its specifications meet or exceed current industry requirements.
Final Future Focused Recommendation
Invest now in the Borehole 3C Geophone that matches your typical borehole conditions. If you work mainly in cased wells, buy the GDJ DJ electromagnetic series. If you work in open hard rock holes, buy the GDJ JG piston type. If you work in variable or difficult conditions, buy the GDJ JF non adjacent series. All three will serve you well into the next decade.
Product Description
| Low-Frequency (vertical, horizontal and three-component ) Geophones | |||
| Parameter\type name | CDJ—Z2A/P2A/S2A | CDJ-Z2B/P2B/S2B | CDJ-Z2C/P2C/S2S |
| Natural Frequency (Hz) | 2±10% | ||
| Sensitivity G | 1.2±10% | 3.5±10%% | 2±10% |
| (v/cm.s-1) | |||
| Coil Resistance Rc(Ω) | 1600±5% | 13000±5% | 6040±5% |
| Internal Resistance | 1540±5% | 12800±5% | 5800±5% |
| (Ω) | |||
| Damping Coefficient Bt | 0.7±10% | ||
| Harmonic Distortion D | ≤ 0.2 | ||
| Insulating Resistance | ≥ 20 | ||
| Ri (MΩ) | |||
| Coil’S Maximum Displacement P-P(mm) | 3 | ||
| Suspension Mass( g ) | 60 | ||
| Working Temperature | —25 ~ +55 | ||
| (℃) | |||
| Geophone Element Weight (K g ) | 0.25 | ||
| Low-Frequency (vertical, horizontal and three-component ) Geophones | |||
| Parameter\type name | CDJ—Z2.5A/P2.5A/S2.5A | CDJ-Z2.5B/P2.5B/S2.5C | CDJ-Z2.5C/P2.5C/S2.5S |
| Natural Frequency (Hz) | 2.5±10% | ||
| Sensitivity G | 1.2±10% | 3.5±10% | 2±10% |
| (v/cm.s-1) | |||
| Coil Resistance Rc(Ω) | 1600±5% | 13000±5% | 6040±5% |
| Internal Resistance | 1540±5% | 12800±5% | 5650±5% |
| (Ω) | |||
| Damping Coefficient Bt | 0.7±10% | ||
| Harmonic Distortion D | ≤ 0.2 | ||
| Insulating Resistance | ≥ 20 | ||
| Ri (MΩ) | |||
| Coil’S Maximum Displacement P-P(mm) | 3 | ||
| Suspension Mass( g ) | 60 | ||
| Working Temperature | —25 ~ +55 | ||
| (℃) | |||
| Geophone Element Weight (K g ) | 0.25 | ||
| Low-Frequency (vertical, horizontal and three-component ) Geophones | |||
| Parameter\type name | CDJ—Z3A/P3A/S3A | CDJ-Z3B/P3B/S3B | CDJ-Z3C/P3C/S3S |
| Natural Frequency (Hz) | 3±10% | ||
| Sensitivity G | 1.2±10% | 3.5±10% | 3±10% |
| (v/cm.s-1) | |||
| Coil Resistance Rc(Ω) | 1600±5% | 13000±5% | 6040±5% |
| Internal Resistance | 1540±5% | 12800±5% | 5650±5% |
| (Ω) | |||
| Damping Coefficient Bt | 0.7±10% | ||
| Harmonic Distortion D | ≤ 0.2 | ||
| Insulating Resistance | ≥ 20 | ||
| Ri (MΩ) | |||
| Coil’S Maximum Displacement P-P(mm) | 3 | ||
| Suspension Mass( g ) | 60 | ||
| Working Temperature | —25 ~ +55 | ||
| (℃) | |||
| Geophone Element Weight (K g ) | 0.25 | ||