Seismic is not too complex for geologists - If you can understand convolution, you have it made. Simply stated, when downward traveling waves pass by a.

Slides:



Advertisements
Similar presentations
Signal Estimation Technology Inc. Maher S. Maklad Optimal Resolution of Noisy Seismic Data Resolve++
Advertisements

Proving ADAPS via honest results. No well data is input
North Sea faulting How the ADAPS inversion / integration clarifies the strike-slip structure – by David Paige This study was originally proposed September,
Introducing the piggy back noise problem. This is what we saw visually on the 3D gather data. Strong and persistent cps waves riding on very low.
1.The seismic energy continuum consists of thousands of independent primary reflections, each coming from a single reflecting interface. 2. There is no.
? Mapping of gulf coast strike slip faults To the left is a set of associated strike slip and adjustment faults on the Lousiana coast. The section itself.
In the next series I present this set of cutouts and try to explain that each shows a refraction event that was lifted off. To see the events on the full.

Going for the RED is an approach used by But for Red to indicate hydrocarbons (like this example) lots of things have to be true. The project I use for.
Transform Techniques Mark Stamp Transform Techniques.
The ADAPS visual approach to interpretation When Dr. Robin Westerman talked Nexen into trying ADAPS I was presented with the display of the problem shown.
Identification of seismic phases
Reflection Coefficients For a downward travelling P wave, for the most general case: Where the first term on the RHS is the P-wave displacement component.
The evolution of the down wave. We hit the earth with some sort of an impact which results in a movement. Since the earth is elastic, it rebounds past.
Environmental and Exploration Geophysics II
Predictive Deconvolution in Practice
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson
Establishing Well to Seismic Tie
De-noising Vibroseis The contention is that the correlated Vibroseis field record (to the far left) is a mess of overlapping coherent noise and signal,
Occurs when wave encounters sharp discontinuities in the medium important in defining faults generally considered as noise in seismic sections seismic.
Another example of critical angle refraction noise.
There is a time for ultra seismic accuracy but that comes after we have located something exciting enough to look at. Since migration before stack almost.
Going for the RED is an approach used by older interpreters. But for red to indicate hydrocarbons (like this example), lots of things have to be true that.
Shale Lime Sand The argument for non-linear methods. 1 The geology 2. The reflection coefficients (spikes in non-linear lingo). 3. The down wave 4. Its.
So where does the ADAPS optimization method fit into this framework? The seismic trace equation does not fit the linear definition, since the values on.
GG450 March 20, 2008 Introduction to SEISMIC EXPLORATION.
Why determining an exact waveform is next to impossible. We start at the recording point with these facts – 1. The seismic continuum consists of overlapping.
Some background and a few basics - How my inversion works – and why it is better - How added resolution makes parallel fault picking a possibility – The.
Welcome to a before and after coherent noise removal series. There is a lot to explain about what is going on here, so I am using this otherwise wasted.
A list of inversion error causes that all attribute junkies should really understand: 1.Definition of inversion – A seismic trace is the product of the.
Depth point 1 A study of the effects of early critical angle crossings. From data I (Paige) had previously processed to check out my sonic log synthesis.
Geology 5660/6660 Applied Geophysics 18 Feb 2014 © A.R. Lowry 2014 For Wed 20 Feb: Burger (§ ) Last Time: Reflection Data Processing Step.
ADAPS optimized stack of line 401 (no inversion or integration). Please toggle with conditioned version I start with the Paige optimized stack v.s. the.
Last week’s problems a) Mass excess = 1/2πG × Area under curve 1/2πG = × in kgs 2 m -3 Area under curve = -1.8 ×10-6 x 100 m 2 s -2 So Mass.
ReferencesInfo Elog Strata Geoview Fundamentals Open Seismic Wavelet Estimation Horizon Picks Low Frequency Model Inversion Near Offset Far Offset Open.
Fiber Optic Transmission SL/HL – Option C.3. Reflection/Refraction Reflection – A wave encounters a boundary between two mediums and cannot pass through.
Downloading and Installing Autodesk Inventor Professional 2015 This is a 4 step process 1.Register with the Autodesk Student Community 2.Downloading the.
Introduction to Deconvolution
SEISMIC INTERPRETATION
Environmental and Exploration Geophysics II
Because noise removal is central to my later work, I start with a discussion on how intertwined coherent noise creates a random effect that confuses all.
ADAPS multiple removal demo. The upper halves of the slides in this series show the input gathers.The bottoms show the same data with multiples removed.
Visual interpretation is still the best. You can see reservoir possibilities that have been missed, and do it at a fraction of the normal cost. The tougher.
Welcome to a wild ride through ideas. In this show I am suggesting that the multiple fractures associated with strike slip faulting can accomplish the.
IB Physics Option F – Fibre Optics Mr. Jean. The plan: Video clip of the day Fibre Optics – C+-+Imaginghttps://ibphysics2016.wikispaces.com/Option+
How the Saudi / shale oil battle should make us stop & think. (and I don’t mean about geo-politics). The shale production reality reminds us the Saudi.
Why inversion & integration is needed to see stratigraphy.
Can we see shale fractures? Some claim to already doing it but I have my doubts. I believe I’m close, but not there yet. I’d like opinions. The section.
Reflection Coefficients For a downward travelling P wave, for the most general case: Where the first term on the RHS is the P-wave displacement component.
Frequency and Bandwidth: their relationship to Seismic Resolution
Probing the question of “how good can seismic get? I ask you to spend a good amount of time just looking at the amazing detail this section shows. When.
Info Read SEGY Wavelet estimation New Project Correlate near offset far offset Display Well Tie Elog Strata Geoview Hampson-Russell References Create New.
Environmental and Exploration Geophysics II tom.h.wilson
Environmental and Exploration Geophysics II tom.h.wilson Department of Geology and Geography West Virginia University Morgantown,
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
The inference and accuracy We learned how to estimate the probability that the percentage of some subjects in the sample would be in a given interval by.
The Frequency Domain Digital Image Processing – Chapter 8.
QUESTION OF THE DAY What is an event that you thought was going to be very scary, but actually wasn’t?
A history of misguided pre-stack processing.
Modeling of free-surface multiples - 2
How to Embed Videos into Powerpoint
Convolution and Deconvolution
The Convolution Method
Identification of seismic phases
From Raw Data to an Image
BEFORE AFTER Let’s start by examining this particular sonic log match. We have super-imposed it both on the input (before) and on the output (after). Some.
Seismic-Well Tie Flow-Chart
Think stratigraphy, This picture, all by itself, not only proves strike slip theory, but also verifies the logic used to bring out the fault detail. This.
—Based on 2018 Field School Seismic Data
Geology Quantitative Methods
Presentation transcript:

Seismic is not too complex for geologists - If you can understand convolution, you have it made. Simply stated, when downward traveling waves pass by a set of reflecting interfaces, the reflected energy at any point is the sum of the products of each of the interfaces times the corresponding wave amplitude. Deconvolution is the reverse - i.e. the process of solving for these interface values using an estimate of the shape of that wavelet. Inversion is just another word for that process. I think most professional geologists can handle that. Since there is a heavy tie between reflection coefficients and well logging, understanding the importance of inversion should come naturally. Of course there are arguments about how to approximate the wave shape, and what to do with the computed coefficients. Those I am involved in are on whether to compute using statistical optimization (in the time domain), or whether to move into the artificial frequency and phase domains (which depend on statistical modeling). But that does not affect the understanding of what deconvolution and inversion are, and those arguments do not have to involve higher mathematics, so I urge all to pay attention. The results of processing decisions made from these calculations affect the whole industry, from exploration to reservoir modeling. The problem with leaving the processing decisions to the mathematical theorists is that they have gone too far with their attribute calculations, seemingly losing sight of reflection facts that do not require advanced math to understand. The first of these facts is that the seismic energy continuum consists of thousands of independent primary reflections, each coming from a single reflecting interface. These individual primary reflections do not mix in the subsurface. Earth filtering creates trailing lobes, the dominant frequency of those lobes decreasing with time. Because of the.huge difference in to and fro travel time between traces, this filtering creates big differences in primary reflection wave shape. The second (but associated) fact is that this travel difference shifts the relationship between primaries. To illustrate the importance of this, suppose the second lobe of the top primary is lined up with the first lobe of the bottom. The fact that the two primaries have opposite polarity means that a lime might look like a gas sand. Of course all variations in between will occur. I ask you to stop and consider that these two items are reflection facts, not opinion, and that they must be considered in any effort to improve resolution. Together they probably explain why some success has been obtained using angle stacks, and also that together they tend to make AVO claims questionable. On the next slide you will see the menu for my collection of non-linear seismic thoughts. There I go on to discuss more topics I consider important.

Introduction – take a minute to see where I am coming from and why this might be worth your time. Then look at some great well log matches to see the merits of non-linear optimization. Or some seismic basics all interpreters should be aware of. And now look at some sources of seismic noise And a quick look at refractions spawned by critical angle crossing. Now to the results of noise removal on a deep South Louisiana project. Or back up to look at the system in action on this last one. Sit back and watch the timed slides. Or here to the results from seemingly hopeless Permian basin data. Or here to still another example of down wave truncation. Or here to where I first identified strike slip faulting on a North Sea project. Or here to a Gulf Coast strike slip fault example. Or here where I discuss direct reservoir detection. Or here for a different discussion of intertwined signal and noise. Or here for a different twist on why ignored noise saved prospects for newcomers. Or here for a more complete noise primer. Or here for a comprehensive look at my inversion. Or here for another look at well log matches. Or here for a fairly sarcastic look at near/middle/far stack options and a wrap-up. This is the router in Paige ’ s set of non-linear seismic thoughts. If you were there, browsing through would be super fast and simple. To get there, see next slide.

I have spent a good bit of time collecting PowerPoints into a folder, which I have sent to my FTP site. If you are interested, You have to do the following to access the work. 1. Enter " adaps.exavault.com " in your browser and go there. The username is adaps and the password is adaps Select the folder PN and "download all". It sends a zipped file. Create a new folder on your PC named PN, unzip and load the two files (shows and base.ppsx) into PN. 3 access "base.ppsx" and you will get the router which will lead you to all the others. This eliminates the load time problem. Thanks in advance Dave Paige