EXPLORATION GEOPHYSICS
EARTH MODEL
NORMAL-INCIDENCE REFLECTION AND TRANSMISSION COEFFICIENTS DENSITY r1 VELOCITY V 1 DENSITY r 2 VELOCITY V2 WHERE: r1 = DENSITY OF LAYER 1 V1 = VELOCITY OF LAYER 1 r 2 = DENSITY OF LAYER 2 V2 = VELOCITY OF LAYER 2
SEISMIC ACQUISITION
GEOPHONE STRUCTURE
GEOPHONE TYPES & FREQUENCY
SOURCE TRUCKS
3D-SEISMIC COVERAGE
CDP & FOLD STACK
MARINE SEISMIC CABLE LAYOUT
MULTIPLE RAYPATH
FACTORS AFFECTING AMPLITUDE
ATTENUATION TECHNIQES
SEISMIC DATA PROCESSING
PROCESSING FLOWCHART
OBJECTIVE OF PROCESSING REAL EARTH EARTH PROPERTIES PULSE SEISMIC TRACE PROCESSING MODEL EARTH
EFFECT OF STACKING ON NOISE SIGNAL PLUS RANDOM AT SIX-DETECTOR ARRAY NOISE SIGNAL SIGNAL + NOISE SIGNAL + NOISE EACH RECEIVER SUMMED OUTPUT
PURPOSE: TO COMBINE TWO DATA SETS FOR A MORE COMPLETE INTERPERATION SEISMIC-WELL TIES PURPOSE: TO COMBINE TWO DATA SETS FOR A MORE COMPLETE INTERPERATION SEISMIC DATA TWO WAY TIME SEISMIC VELOCITY SEISMIC IMPEDENCE SEISMIC SEQUENCES SEISMIC FACIES STRUCTURE WELL DATA LINEAR DEPTH VELOCITY DENSITY GEOLOGIC AGE LITHOLOGY FAULT ORIENTATION
ACOUSTIC STRUCTURE OF EARTH LAYERED EARTH SONIC DENSITY RC
CONVOLUTION
DETAILED SYNTHETIC SEISMOGRAM
DETAILED SYNTHETIC SEISMOGRAM
POST-STACK PROCESSING RESIDUAL STATICS DISPLAY ENHANCEMENT MIGRATION ATTRIBUTE ANALYSIS INVERSION TIME-DEPTH CONVERSION
SUMMARY OF SEISMIC PROCESSING DATA ARE GATHERED AND CMP-ORDERED GATHERS ARE FORMED VELOCITY ANALYSIS IS PERFORMED ON SELECTED GATHERS THE GATHERS ARE MOVEOUT CORRECTED, STACKED, AND PLOTTED STACKING MAY BE FOLLOWED BY ADDITIONAL PROCESSING
VELOCITY ANALYSIS NORMAL MOVEOUT (NMO) X = TX - T0 TX T0 IMAGE POINT WHERE T0 = ZERO OFFSET TIME
NMO-ISOTROPIC LAYER X A C Z B WHERE THEREFORE D IMAGE POINT
ASSUMED RAYPATH FOR VNMO CALCULATION MULTI-LAYER CASE ASSUMED RAYPATH FOR VNMO CALCULATION X TX,1 Z V1 T0,1 T0,2 TX,2 ACTUAL RAYPATH FOR LAYER 1: FOR LAYER 2: VNMO = NORMAL MOVEMEOUT VELOCITY
FOR EACH TRACE T AND X VALUES ARE DETERMINED HOW IS VNMO DETERMINED? FOR EACH TRACE T AND X VALUES ARE DETERMINED
VELOCITY ANALYSIS Y=b+mX T2 - X2 PLOT X2 OFFSET2 t2 HYPERPOLA PLOTS AS A STRAIGHT LINE ON T2 - X2 GRAPH Y=b+mX WHERE
VMNO CORRECTION KNOWING THE VNMO, T AND OFFSET, THE TIME CORRECTION NECESSARY TO SHIFT EACH TRACE CAN BE CALCULATED
INTERVAL VELOCITY DETERMINATION FROM SEISMIC FROM VELOCITY ANALYSIS, WE KNOW VNMO1,T0,1 VNMO2, T0,2 SUBTITUTING THESE VALUES INTO THE DIX EQUATION
MIGRATION EFFECTS FLAT HORIZONS REMAIN UNCHANGED IF THERE ARE NO VELOCITY ANOMALIES ABOVE DIPPING HORIZONS BECOME STEEPER, SHALOWER, AND MOVE LATERALLY UPDIP SYNCLINES BECOME BROADER, WITH ANY BOW TIES ELIMINATED ANTICLINES BECOME NARRWER DIFRACTIONS COLLPSE TO POINTS
RAY PATH MIGRATION t x WHERE = TRUE DIP OF REFLECTOR REFLECTION REFLECTOR x t WHERE = TRUE DIP OF REFLECTOR = APPERENT DIP OF REFLECTOR V= VELOCITY
WHY MIGRATE? TIME DEPTH DEPTH MODEL ARRIVAL TIMES IF BEDS ARE DIPPING, APPERENT POSITION OF EVENTS ON A STACKED SECTION DIFFERS FROM THEIR TRUE POSITION DEPTH MODEL ARRIVAL TIMES 7 KFT/SEC TIME DEPTH 9 KFT/SEC 11 KFT/SEC
ASSUMPTION UNDERLYING MIGRATION ALL EVENTS ARE PRIMARIES- NO NOISE, NO MULTIPLES, NO SHEAR WAVES ALL EVENTS COME FROM THE PLANE VERTICALLY BENEATH THE SEISMIC LINE- NO SIDEWIPE VELOCITY ARE KNOWN EVERY WHERE
MIGRATION MOVES DIPPING HORIZONS
FOCUSING EFFECT OF A SHARP SYNCLINE
DEFOCUSING EFFECT OF AN ANTICLINE
FOCUSING EFFECT OF A SYNCLINE
3-D MIGRATION ELIMINATES ASSUMPTION OF 2--D MIGRATION THAT ALL DATA COMES FROM WITHIN PLANE OF SECTION REQUIRES 3-D DATA COLLECTION TO INSURE CLOSELY SPACED TRACES IN BOTH X, Y DIRECTIONS MOVES ENERGY IN BOTH INLINE AND CROSSLINE DIRECTIONS INLINES AND CROSSLINES TIE AFTER 3-D MIGRATION MAP MIGRATION IS AN ALTERNAIVE FOR COARSE GRID OF 2-D LINES
TIME VS. DEPTH SECTIONS
CDP GATHER AFTER DEMULTIPLEXING
CDP GATHER AFTER AMPLITUDE CORRECTION
CDP GATHER AFTER DECONVOLUTION
VELOCITY ANALYSIS
CDP GATHER AFTER NMO CORRECTION
CDP GATHER AFTER MUTING STRETCHED ZONES
CDP STACKED SECTION
CDP STACKED SECTION WITH TVF FILTER