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JMD-1 Compensated Density Probe
PRODUCT PARAMETERS
- A larger source distance is used to take into account both measurement sensitivity and statistical fluctuation error.
- The method of using long and short source distance detectors to measure simultaneously can compensate for unfavorable factors such as mud cakes.
Description
Abstract
JMD-1 Compensated Density Probe is one of many nuclear logging methods. Its theoretical basis is the Compton scattering effect. It uses Cs137 as a gamma source. The energy of the emitted gamma rays is 0.661MeV. It does not react with the formation material to form electron pairs, but it will produce the Compton effect. By measuring and recording those gamma rays with higher energy, including gamma rays that have been scattered once or multiple times, the apparent density of the formation can be calculated.

Applicable Conditions
● Cased
● Bare hole fill with water or mud
● Bare Dry hole
Applications
● Exploration and quality evaluation of oil, coal, gas and other mineral deposits
● Determine lithology
● Measuring formation porosity
● Testing the cement cementing quality outside the production well casing
● Quantitative calculation of in-situ formation density
Features
● A larger source distance is used to take into account both measurement sensitivity and statistical fluctuation error.
● The method of using long and short source distance detectors to measure simultaneously can compensate for unfavorable factors such as mud cakes.
Specifications
| Scattered gamma detector | Nal crystal + photomultiplier tube |
| Natural gamma detector | Nal crystal + photomultiplier tube |
| Radioactive source | Cs137, 3700MBq |
| Quantity parameters and range | Natural gamma: 1~32768cps; Long source distance count rate: 1~32768cpS Short source distance count rate: 1~32768cps; Density: 1~3.0g/cm3; Accuracy 3% |
| Signal output | Bipolar encoding |
FAQ
① In SI, it is m·s-2, and one percent of it is the international unit abbreviation g.u.;
② Conversion between SI and CGS: 1g.u.=10-1 mGal
Gravitational field: The space around the earth with gravity is called the gravitational field.
Gravitational potential: The gravitational potential W in the gravitational field is equal to the work done by a particle of unit mass moving from infinity to that point.
① The normal gravity field of the earth: Assuming that the earth is a rotating ellipsoid (reference plane), the surface is glossy, the internal density is uniform, or it is distributed in concentric layers, the density of each layer is uniform, and the deviation of the shape of the ellipsoid from the geoid is very small, then the gravity field generated by the earth is the normal gravity field.
② The normal gravity value is only related to the latitude, the smallest at the equator and the largest at the poles, with a difference of about 50,000 g.u.; the rate of change of the normal gravity value with latitude is the largest at 45° latitude, and zero at the equator and the poles; the normal gravity value decreases with increasing altitude, and its rate of change is -3.086 g.u.. The main feature of the long-term change is the "westward drift" of the geomagnetic elements, both the dipole field and the non-dipole field drift westward, and have a global nature.
The gravitational field strength is equal to the gravitational acceleration in both numerical and dimensional terms, and the two are in the same direction. In gravity exploration, all references to gravity refer to gravitational acceleration. The gravitational field strength at a point in space is equal to the gravitational acceleration at that point.
Gravity exploration is an exploration method that is based on the density difference of rocks and ores. Since density difference will cause local changes in the normal gravity field of the earth (i.e. gravity anomaly), it is used to solve geological problems by observing and studying gravity anomalies.
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