CSIR-NET 2014
116. Δg(x,y) are the gravity anomalies recorded on a horizontal plane underlain by a distribution of mass M which a density d surrounded by a material of constant density d0. G is the Newton's gravitational constant. If
A=∫ Δg(x,y)ds , then M=
s
A) A/4πG
B) A/4πG
C) A/4πG *(d/d0)
D) A/2πG *(d/d-d0)
Answer: D
s
A) A/4πG
B) A/4πG
C) A/4πG *(d/d0)
D) A/2πG *(d/d-d0)
Answer: D
Explanation:
In gravity total
excess mass is
The
volume is the volume ‘under’ the anomaly, which needs to be
considered in 3D. In practice, the anomaly is divided into little
columns whose volumes are added (shown in above figure).
considered in 3D. In practice, the anomaly is divided into little
columns whose volumes are added (shown in above figure).
Each
column should have an area small enough that there is little
variations of g across it, so that it’s value equals it’s area times it’s
height.
variations of g across it, so that it’s value equals it’s area times it’s
height.
→ To
calculate it’s total mass perhaps the mass of an ore the
densities of the both body and it’s surroundings are needed.
Assuming the body and its surrounding each have a uniform
density.
densities of the both body and it’s surroundings are needed.
Assuming the body and its surrounding each have a uniform
density.
Mbody
= Mexcess[ρbody
/ ρbody
- ρsurroundings]
Mbody
= A /2πG ( d / d –
d0)
d
= ρbody =
density of the body
d0
= ρsurroundings
= density of the
surrounding rock
G
= universal gravitational constant
(6.67408
* 10-11 m3
/ kg s2
)
A
= volume of the anomaly.
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