Summary. Time only. Distance only. Simultaneous Methods. Distance and Time. Slip-Sweeps Dynamic Slip-Sweeps Unconstrained simultaneous sources

Similar documents
Using long sweep in land vibroseis acquisition

The case for longer sweeps in vibrator acquisition Malcolm Lansley, Sercel, John Gibson, Forest Lin, Alexandre Egreteau and Julien Meunier, CGGVeritas

Noise Reduction in VibroSeis Source Kaëlig Castor*, Thomas Bianchi, Olivier Winter, Thierry Klein, CGG

There is growing interest in the oil and gas industry to

Th-P08-11 Deblending of Single Source Vibroseis Land Data in Egypt with V1 Noise Attenuation Algorithm

Simultaneous multi-source acquisition using m-sequences

T17 Reliable Decon Operators for Noisy Land Data

Summary. Seismic vibrators are the preferred sources for land seismic ( ) (1) Unfortunately, due to the mechanical and

Stereo satellite elevation mapping for stakeless 3D seismic surveying. Demonstration Project BP Libya

Summary. Page SEG SEG Denver 2014 Annual Meeting

Improvement of signal to noise ratio by Group Array Stack of single sensor data

The transformation of seabed seismic

Radial Gain and its Advantages in Seismic Data Acquisition

Tu N Higher Vibrator Hydraulic Force for Improved High Frequency Generation

Attenuation of high energy marine towed-streamer noise Nick Moldoveanu, WesternGeco

Surface-consistent phase corrections by stack-power maximization Peter Cary* and Nirupama Nagarajappa, Arcis Seismic Solutions, TGS

Developments in vibrator control

OPTIMIZING HIGH FREQUENCY VIBROSEIS DATA. Abstract

X039 Observations of Surface Vibrator Repeatability in a Desert Environment

Downloaded 11/02/15 to Redistribution subject to SEG license or copyright; see Terms of Use at

South Africa CO2 Seismic Program

Total 3D seismic onshore - a disruptive transition! London, Nov 2011.

Th B3 05 Advances in Seismic Interference Noise Attenuation

Seismic Reflection Method

AVO compliant spectral balancing

Simultaneous Sources: a technology whose time has come Craig J. Beasley, WesternGeco.

Introduction. Field Test Description

Th ELI1 07 How to Teach a Neural Network to Identify Seismic Interference

B028 Improved Marine 4D Repeatability Using an Automated Vessel, Source and Receiver Positioning System

Can Real-time Wireless Recording Systems be Robust, Reliable and Scalable? Mick Lambert President & C.O.O. Wireless Seismic Inc.

Variable-depth streamer acquisition: broadband data for imaging and inversion

Introduction. Figure 2: Source-Receiver location map (to the right) and geometry template (to the left).

25823 Mind the Gap Broadband Seismic Helps To Fill the Low Frequency Deficiency

Design of an Optimal High Pass Filter in Frequency Wave Number (F-K) Space for Suppressing Dispersive Ground Roll Noise from Onshore Seismic Data

REVISITING THE VIBROSEIS WAVELET

Technology of Adaptive Vibroseis for Wide Spectrum Prospecting

Repeatability Measure for Broadband 4D Seismic

Satinder Chopra 1 and Kurt J. Marfurt 2. Search and Discovery Article #41489 (2014) Posted November 17, General Statement

Spread spectrum techniques for seismic data acquisition

SECTION 2 BROADBAND RF CHARACTERISTICS. 2.1 Frequency bands

Multicomponent seismic polarization analysis

Evaluation of 3C sensor coupling using ambient noise measurements Summary

Deblending workflow. Summary

Th ELI1 08 Efficient Land Seismic Acquisition Sampling Using Rotational Data

Downloaded 09/04/18 to Redistribution subject to SEG license or copyright; see Terms of Use at

FINAL REPORT EL# RS. C. A. Hurich & MUN Seismic Team Earth Sciences Dept. Memorial University Sept. 2009

2012 SEG SEG Las Vegas 2012 Annual Meeting Page 1

Using Frequency Diversity to Improve Measurement Speed Roger Dygert MI Technologies, 1125 Satellite Blvd., Suite 100 Suwanee, GA 30024

Sharing Considerations Between Small Cells and Geostationary Satellite Networks in the Fixed-Satellite Service in the GHz Frequency Band

Multiple Access System

ADC Based Measurements: a Common Basis for the Uncertainty Estimation. Ciro Spataro

19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, 2-7 SEPTEMBER 2007 VIRTUAL AUDIO REPRODUCED IN A HEADREST

PC Digital Data Acquisition

Advancements in near-surface seismic reflection acquisition

MEMS-based 3C accelerometers for land seismic acquisition: Is it time?

Latest field trial confirms potential of new seismic method based on continuous source and receiver wavefields

ISSN Volume 28 Issue 6 June A New Spring for Geoscience. Special Topic

Th N Broadband Processing of Variable-depth Streamer Data

GPR ANTENNA ARRAY FOR THE INSPECTION OF RAILWAY BALLAST

Tu SRS3 07 Ultra-low Frequency Phase Assessment for Broadband Data

This tutorial describes the principles of 24-bit recording systems and clarifies some common mis-conceptions regarding these systems.

Chapter 7. Multiple Division Techniques

Desinging of 3D Seismic Survey And Data Processing of Abu Amood Oil Field Southern of Iraq

G003 Data Preprocessing and Starting Model Preparation for 3D Inversion of Marine CSEM Surveys

Downloaded 01/03/14 to Redistribution subject to SEG license or copyright; see Terms of Use at

41ST ANNUAL MARINE / OFFSHORE INDUSTRY OUTLOOK CONFERENCE GEOSCIENCE UPDATE: MR. ALAN M. BREED EVP SALES & MARKETING

SEN366 (SEN374) (Introduction to) Computer Networks

SPNA 2.3. SEG/Houston 2005 Annual Meeting 2177

Data and Computer Communications. Tenth Edition by William Stallings

3-D tomographic Q inversion for compensating frequency dependent attenuation and dispersion. Kefeng Xin* and Barry Hung, CGGVeritas

Seismic interference noise attenuation based on sparse inversion Zhigang Zhang* and Ping Wang (CGG)

CDMA - QUESTIONS & ANSWERS

CH 4. Air Interface of the IS-95A CDMA System

Accuracy Estimation of Microwave Holography from Planar Near-Field Measurements

Interferometric Approach to Complete Refraction Statics Solution

WS01 B02 The Impact of Broadband Wavelets on Thin Bed Reservoir Characterisation

Successful mobile-radio tester now with US TDMA and AMPS standards

Wireless Progresses! Mick Lambert President & C.O.O. Wireless Seismic Inc.

Cross Spectral Density Analysis for Various Codes Suitable for Spread Spectrum under AWGN conditions with Error Detecting Code

Why not narrowband? Philip Fontana* and Mikhail Makhorin, Polarcus; Thomas Cheriyan and Lee Saxton, GX Technology

Long Range Acoustic Classification

Looking deeper through Pre Amplifier gain A study

Progress in DAS Seismic Methods

CH 5. Air Interface of the IS-95A CDMA System

TECHNICAL CONDITIONS FOR RADIO EQUIPMENT OF INMARSAT SHIP EARTH STATIONS, etc

MEMS-based accelerometers: expectations and practical achievements

A COMPACT, AGILE, LOW-PHASE-NOISE FREQUENCY SOURCE WITH AM, FM AND PULSE MODULATION CAPABILITIES

Wireless Networks (PHY): Design for Diversity

Breaking Through RF Clutter

HD Radio FM Transmission. System Specifications

Performance Analysis of DSSS and FHSS Techniques over AWGN Channel

Adaptive Beamforming for Multi-path Mitigation in GPS

Agilent AN 1275 Automatic Frequency Settling Time Measurement Speeds Time-to-Market for RF Designs

A New Noise Parameter Measurement Method Results in More than 100x Speed Improvement and Enhanced Measurement Accuracy

Four-Channel Sample-and-Hold Amplifier AD684

######################################################################

Enabling autonomous driving

Borehole Seismic Processing Summary Checkshot Vertical Seismic Profile

Isolator-Free 840-nm Broadband SLEDs for High-Resolution OCT

THE EFFECT of multipath fading in wireless systems can

Transcription:

Over 40,000 VPs per day with real-time quality control: Opportunities and Challenges Peter I. Pecholcs, Stephen K. Lafon, Hafiz Al-Shammery and Panos G. Kelamis (Saudi Aramco) Olivier Winter, Jean-Baptiste Kerboul and Thierry Klein (CGGVeritas) Summary In order to evaluate high density source and receiver land seismic acquisition designs, two sets of simultaneous highproductivity field tests were performed in a relatively flat terrain area with good signal-to-noise ratio. These included distance separated simultaneous sweeping (DSSS) (Bouska, 2009), slip-sweep (Rozemond, 1996), distance separated simultaneous slip-sweep (dynamic slip-sweep) and independent simultaneous sources (ISS) (Howe et. al., 2008) with unique sweeps and real-time QC we were not sweeping blind. The second dynamic slip-sweep field test used a 29Km active fixed super-spread (12 receiver lines separated by 300m) with 20 point vibrator fleets on a 25m x 25m source grid. Ten point vibrators were oriented orthogonal to the receiver spread in the North and ten in the South direction with a lateral separation distance of 14.5Km. This method achieved 30,346 vibration points (VPs) in a 24 hour period. The same fixed active receiver spread was reduced to continuously record the unconstrained simultaneous sources (micro-seismic mode) in 18 quadrants (3x6). Each quadrant was 1.8Km x 1.8Km with 4,320 VPs on a 25m x 25m source grid (77,760 total VPs). The unconstrained stakeless productivity test was first acquired with 18 unique 12s pseudorandom sweeps (Sallas et. al., 2008) and repeated with 18 unique linear upsweeps (14.5s average sweep length). These tests achieved optimum productivity rates of 45,501 and 44,793 VPs per 24 hours, respectively, with real-time QC. Even higher rates could have been achieved with stakeless guidance training of the vibrator drivers. In these field test cases, without any training, high productivity rates were achieved with 72 drivers organized in three 8-hour shifts. Four vibrator pushers were used per shift. Three helped with fleet management and one for TDMA real-time communication between the vibrators and the recorder. Figure 1. Twenty four vibrators used in the 2010 field tests. Introduction In recent years, many oil and gas companies have used new high-channel count recording systems equipped with new vibrator control systems to acquire densely sampled symmetric seismic surveys. From these seismic surveys, decimation studies have shown that a balanced increase in receiver and source density improves the resolution of seismic images at all target depths (Bianchi et. al, 2009). Although we have seen a steady improvement in seismic image quality, we are far from acquiring a true uncommitted 3D stack array acquisition design. The main challenge is how to QC and process mega-channel, continuously recorded seismic data in the field and how to reconfigure in-house processing centers (Denis and Sauzedde, 2009). One method used to compensate for recording channel limitations is to position the vibroseis fleets outside the receiver spread. This increases the crossline offset, at the cost of reoccupying VPs. Combining this method with high-productivity source methods, will allow us to acquire densely sampled wide-azimuth seismic survey designs. The most common simultaneous source high-productivity methods are constrained by distance only, time only, or a combination of both time and distance (Table 1). The important question we need to ask is What is the most productive vibroseis acquisition method that preserves data quality? (Bagaini, 2010). DSSS is the lowest risk method, because each vibroseis record can be treated independently without noise interference given sufficient distance separation. The upper limit in terms of productivity is the unconstrained simultaneous source method. As the distance between independent unconstrained vibroseis fleets is reduced, the increased level of cross-talk interference must be removed in seismic processing without removing prestack signal. Simultaneous Methods DSSS Slip-Sweeps Dynamic Slip-Sweeps Unconstrained simultaneous sources Distance only Time only Distance and Time Table 1. High-productivity distance and time classification. The productivity of each of these methods can be simply improved by increasing the number of vibrator fleets and recording channels. This provides the option to either increase the distance and/or time separation between simultaneous sources. Traditionally, the high-productivity vibroseis acquisition (HPVA) slip-sweep method is designed with point vibrator fleets and organized as a single or multiple salvos. In this case, when the fleets are closely positioned to one another, the slip-time can be increased to mitigate harmonic noise interference or the noise attenuated with special processing

algorithms. The same harmonic noise can be avoided in super-spread configuration. If the same receiver spread is reduced by one-half in the cross-line direction, the extra channels can be used to form a super-spread. This allows the fleets to be separated in distance and time and limit the harmonic noise interference to the far offsets. Further improvements in productivity can be gained by using the CGGVeritas fleet management system, where for each fleet specific GPS coordinates and time slots are allocated (Postel, et. al., 2008). In October, 2009 and February, 2010 Saudi Aramco, Argas, and CGGVeritas were given the unique opportunity to test these high-productivity methods with an existing 9,000 channel production seismic crew with 24 point vibrators (Figure 1). This paper reviews these recent dynamic slipsweep and unconstrained simultaneous source methods using unique pseudorandom and linear sweeps. The high-productivity field test methods increased (Figure 9). With this steady increase in VPs per hour, achieving greater than 40,000 VPs per 24 hours, may have been possible, if additional test time had been available. Unconstrained simultaneous source methods The unconstrained simultaneous source field tests acquired in February, 2010, used a reduced active receiver spread with point vibrators isolated in 3 x 6 quadrants, where each quadrant was 1.8Km by 1.8Km with 4,320 VPs on a 25m x 25m source grid (Figure 4 bottom). The unconstrained simultaneous source field test was acquired with 18 unique pseudo-random and linear upsweeps, along with real-time QC. Both sweep designs were designed to reduce the crosstalk noise by 20dB or greater. These field tests were acquired with real-time QC. We were no longer sweeping blind. Both the seismic data and vibrator attributes could be quality controlled in real time. Dynamic slip-sweep method The first dynamic slip-sweep field test used 6 fleets (two vibrators per fleet), 12s linear upsweep, 6s slip-time and the minimum simultaneous separation distance was set to 6.5 Km. Thirteen swaths were recorded into a fixed spread of 24 receiver lines (Figure 2). The combination of sliptime and distance minimized the interference of harmonic noise (Figure 3 top) and proved to have no impact on the final processing results. The production and dynamic slipsweep results were equivalent (Figure 3 - bottom). During this field test we achieved a maximum productivity of 6,000 VPs per day as compared to conventional flip-flop productivity of 3,000 VPs with three fleets. Figure 3. Dynamic slip sweep (upper). Note the lack of harmonic noise contamination. The production (left) and dynamic slip-sweep stack (right) are equivalent. Figure 2. The first dynamic slip-sweep survey design. The second dynamic slip-sweep field test (February, 2010) was repeated in a new location with 20 vibrator trucks (4 spares) on a 25m x 25m source grid. Two salvos with 10 point vibrators per salvo were horizontally separated by 14.5Km along a 29Km super-spread (Figure 4 top). We used a 6s linear upsweep, 3s slip-time and the minimum simultaneous distance was set to 3Km. We achieved 30,346 VPs per 24 hour period after two swaths of acquisition time. As the vibroseis drivers became more familiar with the stakeless guidance monitor, the number of VPs per hour Figure 4. Dynamic slip-sweep super-spread with vibroseis salvos shown in red (top) and unconstrained simultaneous source (bottom) field test designs. Unique linear sweeps The selection of 18 unique linear sweeps was based on the analysis of the maximum amplitude from the crosscorrelation matrix of linear sweeps ranging from 6 to 23s.

Cross-correlating any sweep along the diagonal with an adjacent linear sweep with only a one second difference in sweep rate reduces the cross-talk noise by 20dB or more (Figure 5). For this reason, we chose a simple approach and organized the 18 linear sweeps as shown in Table 2. degradation) of radio contact between only one vibrator or more within a fleet can stop or slow down production. In this case, observers would have to consider moving the recorder truck to improve radio communication or implement the use of radio repeaters. Figure 6. Unconstrained simultaneous sweeps using pseudorandom (left), unique linear (middle) and the same linear sweep (right). Note the different levels of cross-talk. Figure 5. Linear sweep cross-correlation matrix from 6s to 23s. Note with only 1 s difference, the cross-talk is reduced by approximately 20dB. Optimized linear sweep lengths per quadrant in seconds 6 23 9 20 12 17 15 14 18 11 21 8 7 22 10 19 13 16 16 13 19 10 22 7 Figure 7. Real-time QC of simultaneous sweeps for pseudorandom (left), unique linear (middle) and the same linear sweeps (right). 8 21 11 18 14 15 17 12 20 9 23 6 Table 2. After acquiring 50% of the total time to complete the acquisition in quadrant one (1,1), each vibrator changed sweeps from blue to green. The average sweep length for all quadrants was 14.5s. Unique pseudorandom sweeps Eighteen unique pseudorandom sweeps were defined and applied to point vibrators in each quadrant (3x6 quadrants). As described by Sallas et. al. (2009), the objective of using the pseudorandom sweeps was to reduce the cross-talk noise by greater than 20dB and increase the low frequency energy. Unconstrained simultaneous source real-time QC In the past, to speed up acquisition, the recording system sent the start command through the radio to the vibrators and the vibrators sent the ready-to-shake command to the recorder. Now, in continuous recording mode, the vibrators will sweep independently of radio communication. Radio communication is where a great percentage of acquisition time is lost. In flip-flop, slip-sweep (HPVA) and highfidelity vibroseis seismic (HFVS) modes, a loss (or Figure 8. This real-time QC illustrates the vibrator position in each quadrant. The red dots indicate vibrators above predefined distortion threshold. Using the V1 methodology (Postel et. al., 2008) and unconstrained simultaneous source acquisition modes (enhanced with V1 real-time QC modes) the radio communication is no longer needed for source control. We are no longer dependent on distance or terrain conditions. The QC can be monitored either in the recorder truck or in a V1 equipped vehicle. Production is no longer interrupted when a vibrator is out of specification or when radio communication is lost. The vibrators will continue sweeping. During production, the Tablet PC, within each vibrator, stores all the QC attributes such as vibrator phase, distortion, amplitude, position, sweep parameters, and GPS time. These attributes and more can be retrieved by modem at a later time, or relayed by the other vibrators, or repeaters to the recorder. We are aware of the state of each

vibrator based upon these QC attributes. These are used to optimize fleet management. Figure 9. Dynamic slip-sweep productivity per hour. How the pseudo real-time QC works The pseudo real-time QC software, can be setup in a light truck in the middle of the vibrator fleets, on a high elevation point, and run by a vibrator pusher. Through repeaters, it can also be monitored in the base camp or other locations. This automatic QC in the vibrator and recorder allows both the vibroseis driver and observer to quickly take decisions about reshooting a VP. This ensures acquisition compliance within pre-plan specifications at high-productivity rates. If an adequate internet connection were available, the software could be run safely (with access through login and password). This interface is currently under development. Conclusions Figure 10. Unconstrained pseudorandom (left) and unique linear simultaneous sweep productivity per hour (right). Peak productivity per hour was 2,064 for unconstrained simultaneous sources. Based on these limited tests, we determined that the use of both distance and time constraints, poses the lowest risk acquisition high-productivity method with our current production seismic crews. Given the opportunity to achieve production levels greater than 40,000 VPs/day, this implies we can finally acquire well sampled wide-azimuth seismic surveys. Currently, we believe the fixed time slot method with both distance and time, can achieve very highproductivity rates with our current production seismic crews. As noted earlier, the unconstrained simultaneous sources technique offers the highest production rates. Seismic processing algorithms will need to be developed and proven to preserve prestack signals. In all the field test cases, it was clear that the vibroseis drivers require proper training with stakeless guidance systems, as shown by the standard deviation for move-up times on a 25m source grid (Figure 9). Figure 11. The median, mean and standard-deviation values for the move-up times for unconstrained simultaneous source field tests using a 25m source grid. Why are we faster today? The answer is very simple - point vibrators or fleets of vibrators are sweeping independently with stakeless guidance systems and real time QC. For example, if the vibrator fleet is out of position (tolerance) the driver will know instantly before sweeping by a synthesized voice from the Tablet PC. The driver will be warned to sweep again without any QC radio communication (Figure 10). Figure 12. Stakeless guidance monitor (Tablet PC) Acknowledgements The authors thank the Saudi Arabian Ministry of Petroleum and Mineral Resources, and the Saudi Arabian Oil Company (Saudi Aramco) for their support and permission to publish this paper. We also like to thank Yi Luo and Shoudong Huo of Saudi Aramco.

References Bouska, J., 2009, Distance separated simultaneous sweeping: Efficient 3D Vibroseis acquisition in Oman: 79 th Annual International Meeting, SEG, Expanded Abstracts, 1-5. Bianchi, T., Monk D. and Meunier J., 2009, Fold or Force?: 71 st EAGE Conference and Exhibition. Denis, M. and Sauzedde P., 2009, Dukhan 3D: An ultra high density, Full wide azimuth Seismic survey for the future: IPTC, Doha. Howe D., Foster M., Allen T., Taylor B., and Jack I., 2008, Independent simultaneous sweeping a method to increase the productivity of land seismic crews: 78 th Annual International Meeting, SEG, Expanded Abstracts, 2826-2830. Postel, J.J., Meunier, J., Bianchi, T., and Taylor, R., 2008, V1: Implementation and application of single-vibrator acquisition: The Leading Edge, 27, no. 5, 604-608. Rozemond, J.H., 1996, Slip-sweep acquisition: 66 th Annual International Meeting, SEG, Expanded Abstracts, 64-67. Sallas, J.J., Gibson, J.B., Lin F., Winter, O., Montgomery, B., and Nagaraiappa P., 2008, Broadband Vibroseis using simultaneous pseudorandom sweeps: 78 th Annual International Meeting, SEG, Expanded Abstracts, 100-104.