9
PROCEEDINGS OF JOINT CONVENTION JAKARTA 2003 The 32 nd IAGI and The 28 th HAGI Annual Convention and Exhibition STUDY ESTIMATE DISTRIBUTION VARIABILITY OF TOTAL MOISTURE IN SEAM COAL USE METHOD OF GPR Eddy Ibrahim, Lilik Hendrajaya, Gunawan Handayani, Umar Fauzi, Syaiful Islam INTRODUCTION This article depict development of technique of GPR for the measurement of total moisture content at coal either through temporal and spasial. Measurement technique the developed is technique of reflection profiling acquisition by determining orientation both of antenna unshielded to yield the polarization of propagation perpendicular to bedding plane of seam coal and place direct both of antenna above outcrop coal ( figure 1) at same of rank of coal which is definition with path length 6.05 m ( figure 2) while at outcrop coal with different of rank of coal by lateral with path length is 3.12 m ( figure 3) used by geometry height of antennas is 0,1 λ ( figure 3 a). Usage of this technique with frequency of antenna 100 MHZ where the analysis of using attribute interval have succeeded determined of total moisture content in seam coal at sameness rank of coal where by lateral zone 1 having compared to higher total moisture content of zone 2 due to result of analysis of proximate ( laboratory test) by channel sampling ( figure 4, 5 ). To result of clear process that quantitatively due to amplitude value of zone 2 the magnitude intensity storey level of compared to higher of zone 1 where the value show highly lower total moisture content of seam coal by lateral ( figure 6 ). While from attribute interval to entire trace focussed at seam coal for time window ( 4.2 ns - 22.5 ns) can more show total moisture content lateral variability of seam coal and according to after validated with result testing of laboratory ( analyse of proximate) (figure 7 and 7a). While to clarify boundary of lateral difference of the physical used by phase spectrum analysis where value phase angular of average vertically to entire trace focussed at seam coal for time window ( 4.2 ns - 22.5 ns) hence earning seen clear of boundary area of lateral between coal of high total moisture content with coal of total moisture content low where lower right side the phase angular value of expressing high amplitude value while the boundary area of expressed by the happening of phase inversion ( figure 8 and 8a) For the determined of seam coal which by lateral differ rank of coal also succeed to be conducted by using frequency of antenna 200 MHZ where because of this traverse line do not be conducted by analysis of proximate ( test of laboratory) hence boundary information of rank of coal obtained from PTBA and data drill closest ( figure 9 ). As for process result earn seen that ( figure 10) visually still difficult differentiate between coal of antharacite ( left side) from trace 1 - 50 and coal of dry coal ( right side) from trace 51 - 104. Because amplitude intensity and pattern either through lateral and vertical cannot quantified directly, more than anything else phase angle able to be used for determined of seam coal boundary by lateral. To overcome this problem of usage attribute interval in the reality can differentiate expressly due to measurement of peak of amplitude value at coal of anthracite ( trace 1 - 50) is 726,53602 DN happened at trace 11 while at coal of dry coal ( trace 51 - 104) peak of value of is 380,74705 DN at trace 56 and 598,15242 DN at trace 90 (figure 11). Thus can be concluded by that because of peak of value yielded amplitude is result of from level average assess per trace and per sample hence can clarify that total moisture content for the coal of lower anthracite far than coal of Dry coal. While to determine boundary area by lateral between both rank of coal earn determined by using phase angle value where frontier both of rank of coal at trace to 52 with phase angle value - 1.4012 radian of trace to 53 with phase angle value 1,15244 radian ( figure 12).

moisture use gpr.pdf

Embed Size (px)

Citation preview

PROCEEDINGS OF JOINT CONVENTION JAKARTA 2003The 32nd IAGI and The 28th HAGI Annual Convention and Exhibition

STUDY ESTIMATE DISTRIBUTION VARIABILITY OF TOTALMOISTURE IN SEAM COAL USE METHOD OF GPR

Eddy Ibrahim, Lilik Hendrajaya, Gunawan Handayani, Umar Fauzi, Syaiful Islam

INTRODUCTION

This article depict development of technique ofGPR for the measurement of total moisturecontent at coal either through temporal andspasial. Measurement technique the developed istechnique of reflection profiling acquisition bydetermining orientation both of antennaunshielded to yield the polarization ofpropagation perpendicular to bedding plane ofseam coal and place direct both of antennaabove outcrop coal ( figure 1) at same of rank ofcoal which is definition with path length 6.05 m( figure 2) while at outcrop coal with differentof rank of coal by lateral with path length is 3.12m ( figure 3) used by geometry height ofantennas is 0,1 λ ( figure 3 a).

Usage of this technique with frequency ofantenna 100 MHZ where the analysis of usingattribute interval have succeeded determined oftotal moisture content in seam coal at samenessrank of coal where by lateral zone 1 havingcompared to higher total moisture content ofzone 2 due to result of analysis of proximate (laboratory test) by channel sampling ( figure 4, 5). To result of clear process that quantitativelydue to amplitude value of zone 2 the magnitudeintensity storey level of compared to higher ofzone 1 where the value show highly lower totalmoisture content of seam coal by lateral ( figure6 ). While from attribute interval to entire tracefocussed at seam coal for time window ( 4.2 ns- 22.5 ns) can more show total moisture contentlateral variability of seam coal and according toafter validated with result testing of laboratory (analyse of proximate) (figure 7 and 7a). While toclarify boundary of lateral difference of thephysical used by phase spectrum analysis wherevalue phase angular of average vertically toentire trace focussed at seam coal for timewindow ( 4.2 ns - 22.5 ns) hence earning seenclear of boundary area of lateral between coal of

high total moisture content with coal of totalmoisture content low where lower right side thephase angular value of expressing highamplitude value while the boundary area ofexpressed by the happening of phase inversion (figure 8 and 8a)

For the determined of seam coal which bylateral differ rank of coal also succeed to beconducted by using frequency of antenna 200MHZ where because of this traverse line do notbe conducted by analysis of proximate ( test oflaboratory) hence boundary information of rankof coal obtained from PTBA and data drillclosest ( figure 9 ). As for process result earnseen that ( figure 10) visually still difficultdifferentiate between coal of antharacite ( leftside) from trace 1 - 50 and coal of dry coal (right side) from trace 51 - 104. Becauseamplitude intensity and pattern either throughlateral and vertical cannot quantified directly,more than anything else phase angle able to beused for determined of seam coal boundary bylateral. To overcome this problem of usageattribute interval in the reality can differentiateexpressly due to measurement of peak ofamplitude value at coal of anthracite ( trace 1 -50) is 726,53602 DN happened at trace 11 whileat coal of dry coal ( trace 51 - 104) peak of valueof is 380,74705 DN at trace 56 and 598,15242DN at trace 90 (figure 11). Thus can beconcluded by that because of peak of valueyielded amplitude is result of from level averageassess per trace and per sample hence can clarifythat total moisture content for the coal of loweranthracite far than coal of Dry coal. While todetermine boundary area by lateral between bothrank of coal earn determined by using phaseangle value where frontier both of rank of coal attrace to 52 with phase angle value - 1.4012radian of trace to 53 with phase angle value1,15244 radian ( figure 12).

PROCEEDINGS OF JOINT CONVENTION JAKARTA 2003The 32nd IAGI and The 28th HAGI Annual Convention and Exhibition

REFERENCE

Annan A.P., Waller W.M., Strangway D.W.,Rossiter J.R.,Redman J.P. and Watts R.D. 1975.The electromagnetic Response of a low-loss, 2-layer dielectric earth for horizontal electricdipole excitation, Geophysics 40, 286-298.

Annan A.P., 2001. Ground Penetrating RadarWorkshop Notes, Sensors & Software, Ontario,Canada.

Balnis C.A, 1982. Antenna Theory Analysis andDesign. Harper & Row, Philadelphia.

David C.N. 1999. The directional dependence ofthe ground penetrating radar response on theaccumulation zones of temperate Alpine glacier,First Break 17, 249-259.

Tjia M.O., 1997. Teori Elektrodinamika Klasik,Departemen Fisika, FMIPA, Institut TeknologiBandung.

Engheta N. and Papas C.H. 1982. Radiationpatterns of interfacial dipole antenna. RadioScience 17, 1557-1566.

Gestel J.V. and Stoffa P.L., 1999. Multi-configuration ground penetrating radar data. 69th

SEG meeting, Houston, USA, ExpandedAbstracts, 540-543.

J. van der Kruk., 2001 Three-DimensionalImaging of Multi-component groundpenetrating radar data, Ph.D diss. T U DelftUniversity.

Jol. H.M., 1995. Ground penetrating radarantennae frequencies and transmitter powerscompared for penetration depth, resolution andreflection continuity, Geophysical Prospecting43, 693-709.

Lehman F., Boerner D.E., Holliger K. and GreenA.G. 2000. Multicomponent georadar data :some important implications for data acquisitionand processing. Geophysics 65, 1542-1552.

Miwa T., Sato M, and Niitsuma H. 1999.Subsurface fracture measurement withpolarimetric borehole radar. IEEE TransactionGeoscience and Remote Sensing 37, 828-837.

Noon D.A., 1996. Stepped-frequency radardesign and signal processing enhances groundpenetrating radar performance, Ph.D. diss,University of Queensland.

Roberts R.L., 1994. Analysis and theoreticalmodeling of GPR polarization data, Ph.D.diss,Ohio State Univ.

Roberts R.L. and Daniels J.J. 1996. Analysis ofGPR Polarization phenomena. Journal ofEnvironmental and Enginering Geophysics 1,139 – 157.

Sheriff, R.E., 1984. Encyclopedia Dictionary ofExploration Geophysics, Soc. Explor. Geophys.,Tulsa, OK., 2nd ed., 323 pp.

Soon Jee Seol, Jung-Ho Kim, Yoonho Song andSeung-Hwan Chung, 2001. Finding the strikedirection of fractures using GPR,GeophysicalProspecting 49, 300 – 308.

Topp, G.C., Davis, J.L., Annan, A.P., 1980.Electromagnetic determination of soil watercontent : measurements in coaxial transmissionlines, Water Resour. Res 16, 574 – 582.

Van Overmeeren, R.A., Sariowan, S.V. andGehrels, J.C, 1997. Ground penetrating radar fordetermining volumetric water content; results ofcomparative measurements at two test sites,Journal of Hydrology 197, 316-338.

PROCEEDINGS OF JOINT CONVENTION JAKARTA 2003The 32nd IAGI and The 28th HAGI Annual Convention and Exhibition

Figure 1. Mode of acquisition of reflection profiling for frequency antenna 100 MHz direct above outcrop coal

coal

I

Figure 2 . : Outcrop coal physical model measured. This coal seam by lateral at the rank of coal is sameness. That is bituminuous coal( seam B2)

Figure 3. : Outcrop coal physical model with path This seam coal by lateral is difference of

Antracite

Line boundacoal) (from P

Indicatorboundary

nterburden

length of 3.12 M rank of coal

Dry coal

ry (rank ofTBA)

PROCEEDINGS OF JOINT CONVENTION JAKARTA 2003The 32nd IAGI and The 28th HAGI Annual Convention and Exhibition

.

Figure 4. : Schematic of acquisition of channel sampling

Figure 3a. : Mode of acquisition of reflection profiling at path length 3.12 M Frequency of antenna 200 MHz with height 0,1 λ above outcrop

coal.

PROCEEDINGS OF JOINT CONVENTION JAKARTA 2003The 32nd IAGI and The 28th HAGI Annual Convention and Exhibition

High

Low

Zona 1 Zona 2

Figure 5.: Profile result of analysis of proximate from channel sampling ‘ direction of horizontal expressed position take channel sampling and direction of vertical is thick of coal seam and scale bar expressing obstetrical gradation of total moisture in coal seam

Figure 6.: Profile result of process at physical model outcrop coal with path length 6.05 M

PROCEEDINGS OF JOINT CONVENTION JAKARTA 2003The 32nd IAGI and The 28th HAGI Annual Convention and Exhibition

Figure 7 :

Figure 7a : .

. Graph of average amplitude value by vertical to entire trace at outcrop coal model with path length 6.05 M

Graph of peak of amplitude values per trace at outcrop coal model with path length is 6.05 m

PROCEEDINGS OF JOINT CONVENTION JAKARTA 2003The 32nd IAGI and The 28th HAGI Annual Convention and Exhibition

Figure 8.: Graph of average phase angle values by vertical to entire trace at outcrop coal model with path length is 6.05 M

Figure 8a : Graph of peak of phase angle values per trace at outcrop coal model with path length is 6.05 m

PROCEEDINGS OF JOINT CONVENTION JAKARTA 2003The 32nd IAGI and The 28th HAGI Annual Convention and Exhibition

Figure 10 : Profile result of process use frequency of antenna 200 MHz At outcrop coal model with path length is 3.12 M

Figure 9 : Data information of lithology at mine Air Laya Where Outcrop coal model with path length 3.12m The model is lay in seam C.

Seam coalmeasured

Antracite Dry coal

PROCEEDINGS OF JOINT CONVENTION JAKARTA 2003The 32nd IAGI and The 28th HAGI Annual Convention and Exhibition

Figure . 11 : Average of amplitude values by vertical to entire trace ( trace 1 – 104) at seam coal zone with path length is 3.12 m by using frequency of antenna is 200 MHz

Figure . 12 : Average of phase angle values by vertical to entire trace ( trace 1 – 104) at seam coal zone with path length is 3.12 M by using frequency of antenna 200 MHz