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<strong>Interpretation</strong> <strong>of</strong> <strong>3D</strong> <strong>Seismic</strong> <strong>and</strong> <strong>Subsurface</strong> <strong>data</strong> <strong>from</strong> <strong>the</strong><br />

<strong>Buffalo</strong> Valley Field, Chavez county, New Mexico<br />

S<strong>and</strong>eep Pyakurel, Thomas H. Wilson, Jaime Toro, <strong>and</strong> Shahab Mohaghegh<br />

Department <strong>of</strong> Geology <strong>and</strong> Geography, 419 White Hall, West Virginia University, Morgantown, WV 26506-6300<br />

Abstract<br />

Structure <strong>and</strong> isopach maps derived <strong>from</strong> formation top picks<br />

reveal <strong>the</strong> presence <strong>of</strong> differential subsidence across <strong>the</strong><br />

<strong>Buffalo</strong> Valley field during <strong>the</strong> Pennsylvanian <strong>and</strong> Permian<br />

periods. The <strong>Buffalo</strong> Valley field is located along <strong>the</strong> Northwest<br />

Shelf <strong>of</strong> <strong>the</strong> Delaware Basin. <strong>3D</strong> seismic <strong>data</strong> reveal that <strong>the</strong><br />

field is bounded by two normal faults, both <strong>of</strong> which drops to<br />

<strong>the</strong> sou<strong>the</strong>ast. The fault bounded block rotates slightly to <strong>the</strong><br />

sou<strong>the</strong>ast during deposition <strong>of</strong> <strong>the</strong> reservoir intervals.<br />

Production <strong>from</strong> <strong>the</strong> Morrow Formation is concentrated within<br />

this fault block. The Morrow production trend in this area is<br />

roughly north-south at an angle to <strong>the</strong> nor<strong>the</strong>ast trending<br />

Northwest Shelf in this area.<br />

<strong>3D</strong> seismic <strong>data</strong> volumes consisting <strong>of</strong> P-wave <strong>and</strong> PS-wave<br />

<strong>data</strong> are interpreted <strong>and</strong> compared in this study. VSP <strong>data</strong><br />

(zero <strong>of</strong>fset an some <strong>3D</strong> VSP coverage ) are incorporated into<br />

<strong>the</strong> seismic interpretation. The tie between surface seismic<br />

<strong>and</strong>s well-log derived syn<strong>the</strong>tics is generally poor due to<br />

Fresnel zone effects in <strong>the</strong>se heterogeneous intervals.<br />

Correlation <strong>of</strong> formation top depths to arrival times in <strong>the</strong> zero<strong>of</strong>fset<br />

corridor stack are used to identify reflection events in <strong>the</strong><br />

surface seismic <strong>data</strong>. In this study we examine <strong>the</strong> relationship<br />

<strong>of</strong> reflection amplitude <strong>and</strong> o<strong>the</strong>r seismic attributes associated<br />

with reflections <strong>from</strong> <strong>the</strong> Atoka-Morrow interval to 5- year<br />

cumulative production <strong>data</strong> <strong>from</strong> <strong>the</strong> field.<br />

Background<br />

The study area is located within <strong>the</strong> <strong>Buffalo</strong> Valley field in <strong>the</strong><br />

sou<strong>the</strong>rn part <strong>of</strong> <strong>the</strong> Chavez County, New Mexico (Figure 1).<br />

The area lies on <strong>the</strong> Northwest Shelf <strong>of</strong> <strong>the</strong> Delaware Basin.<br />

Production in <strong>the</strong> <strong>Buffalo</strong> Valley field is largely <strong>from</strong> a channel<br />

s<strong>and</strong> at <strong>the</strong> base <strong>of</strong> <strong>the</strong> Morrow Formation. Reservoir depth in<br />

<strong>the</strong> field is approximately 9000 feet subsurface. The Morrow<br />

Formation consists mostly <strong>of</strong> interbedded s<strong>and</strong>, shale <strong>and</strong> thin<br />

limestone deposits. The reservoir quality s<strong>and</strong>stone lies in <strong>the</strong><br />

lower part <strong>of</strong> <strong>the</strong> Morrow formation <strong>and</strong> is interpreted to be an<br />

inter-distributary channel fill deposit. The base <strong>of</strong> <strong>the</strong> Morrow<br />

coincides with <strong>the</strong> Mississippian unconformity. Channels at <strong>the</strong><br />

base <strong>of</strong> <strong>the</strong> Morrow scour into <strong>the</strong> Mississippian Barnett shale,<br />

which overlies <strong>the</strong> Chester Formation. The top <strong>of</strong> <strong>the</strong> Morrow is<br />

overlain by Atoka Formation which is comprised mostly <strong>of</strong> s<strong>and</strong><br />

shale <strong>and</strong> carbonate.<br />

Figure 1: Location map.<br />

<strong>Seismic</strong> <strong>data</strong> <strong>from</strong> <strong>the</strong><br />

<strong>Buffalo</strong> Valley area were<br />

provided by WesternGeco<br />

Syn<strong>the</strong>tic Tie<br />

The tie between reflection events <strong>and</strong><br />

formation tops was established at <strong>the</strong><br />

Read <strong>and</strong> Stevens, Inc., Lula #3 well (API<br />

No. 30-005-60481). Data available for <strong>the</strong><br />

Lula #3 include a near <strong>of</strong>fset VSP <strong>and</strong><br />

near <strong>of</strong>fset corridor stack (Figure 3).<br />

Arrival times <strong>of</strong> reflection events in <strong>the</strong><br />

surface seismic <strong>data</strong> were approximately<br />

44 milliseconds early relative to those in<br />

<strong>the</strong> VSP corridor stack. Wea<strong>the</strong>ring<br />

corrections <strong>and</strong> surface consistent static<br />

corrections are <strong>the</strong> likely cause <strong>of</strong> this<br />

difference.<br />

0.600<br />

0.700<br />

0.800<br />

0.900<br />

1.000<br />

1.100<br />

Trobough 1-A<br />

Lula3<br />

Bogle State Com 1<br />

6035 ft 4625 ft<br />

- Line 1034 + Corridor & Synth -<br />

SP: 1.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0<br />

A<br />

Wolf<br />

Cis<br />

Can<br />

St<br />

At<br />

1C<br />

2C<br />

Miss<br />

WDev<br />

0.600<br />

0.700<br />

0.800<br />

0.900<br />

1.000<br />

1.100<br />

Figure 3: Surface<br />

<strong>Seismic</strong>, VSP Corridor<br />

Stack & syn<strong>the</strong>tics<br />

Fresnel zone effects likely prevent a<br />

good match <strong>of</strong> syn<strong>the</strong>tic to corridor stack<br />

<strong>and</strong> VSP corridor stack to surface<br />

seismic. Some <strong>of</strong> this heterogeneity can<br />

be observed in <strong>the</strong> <strong>3D</strong> VSP <strong>data</strong> around<br />

<strong>the</strong> Lula #3 well (Right). The Fresnel<br />

zone radius at lower Pennsylvanian<br />

Morrow depths is approximately 1500<br />

feet using an RMS velocity <strong>of</strong> 16400 feet<br />

per second derived <strong>from</strong> <strong>the</strong> well velocity<br />

survey, <strong>and</strong> dominant frequency <strong>of</strong><br />

approximately 62.5 Hz. Given <strong>the</strong> <strong>3D</strong><br />

0.800<br />

0.900<br />

1.000<br />

1.100<br />

1.200<br />

SP:<br />

Lula3<br />

- Corridor Stack & Upgoing VSP -<br />

75.0 100.0 125.0 1.0 25.0 50.0 150.0 154.0<br />

Wolf<br />

Cis<br />

Can<br />

St<br />

At<br />

1C<br />

2C<br />

Miss<br />

WDev<br />

Figure 2: Zero Offset<br />

VSP & Corridor Stack<br />

Surface seismic <strong>data</strong> in <strong>the</strong> vicinity<br />

<strong>of</strong> <strong>the</strong> Lula #3 well (Figure 3) along<br />

with <strong>the</strong> near <strong>of</strong>fset corridor stack <strong>and</strong><br />

b<strong>and</strong>pass filtered syn<strong>the</strong>tic seismic<br />

traces compiled <strong>from</strong> <strong>the</strong> Lula #3<br />

sonic illustrate <strong>the</strong> seismic tie used to<br />

interpret reflection events. The east<br />

west inline 1034 is split at <strong>the</strong> Lula #3<br />

well. The corridor stack along with a<br />

series <strong>of</strong> b<strong>and</strong>pass filtered syn<strong>the</strong>tics<br />

have been inserted into <strong>the</strong> gap at<br />

<strong>the</strong> well location for comparison to<br />

surrounding seismic <strong>data</strong>. Formation<br />

top correlations to reflection events<br />

are illustrated. The section is quite<br />

heterogeneous at local scales, <strong>and</strong><br />

Lula3<br />

Line:<br />

Trace:<br />

1.000<br />

1.100<br />

2069.0<br />

10340.0<br />

St<br />

At<br />

1C<br />

2C<br />

Miss<br />

Figure 3: <strong>3D</strong> VSP<br />

VSP response, it is not surprising to see disagreement in <strong>the</strong><br />

details <strong>of</strong> <strong>the</strong> seismic response observed between <strong>the</strong> various<br />

<strong>data</strong> sets <strong>and</strong> <strong>the</strong> syn<strong>the</strong>tic seismogram. Based on <strong>the</strong> above<br />

comparisons we place <strong>the</strong> base <strong>of</strong> <strong>the</strong> Morrow (top <strong>of</strong> <strong>the</strong><br />

Chester) at 1.074 sec in <strong>the</strong> surface seismic. The reflection <strong>from</strong><br />

<strong>the</strong> top <strong>of</strong> <strong>the</strong> Atoka arrives at approximately 1.041 sec.<br />

1.000<br />

1.100<br />

0.800<br />

0.900<br />

1.000<br />

1.100<br />

1.200<br />

Figure 5: Type log for study<br />

area (Well 30005060321)<br />

Top <strong>of</strong> <strong>the</strong><br />

Atoka<br />

Top <strong>of</strong> <strong>the</strong><br />

Morrow<br />

Morrow Basal<br />

Channel<br />

Top <strong>of</strong> <strong>the</strong><br />

Barnet Shale<br />

Top <strong>of</strong> <strong>the</strong><br />

Chester<br />

<strong>Seismic</strong> time structure<br />

Time structure on <strong>the</strong> Chester <strong>and</strong><br />

Atoka reflection events (figures 6 <strong>and</strong><br />

7, respectively) reveals that <strong>the</strong> field is<br />

bounded along its western <strong>and</strong> eastern<br />

margins by two faults across which <strong>the</strong><br />

strata drop to <strong>the</strong> east. <strong>Seismic</strong> pr<strong>of</strong>iles<br />

<strong>from</strong> <strong>the</strong> <strong>3D</strong> survey (Figure 8) reveal<br />

that <strong>the</strong>se faults are nearly vertical.<br />

The isochore map for <strong>the</strong><br />

Atoka to Chester reflection<br />

events (Figure 9) suggests<br />

some movement along<br />

<strong>the</strong>se faults occurred during<br />

deposition <strong>of</strong> this lower<br />

Pennsylvanian interval.<br />

Log Response<br />

Formation top picks for most <strong>of</strong> <strong>the</strong><br />

wells were based on <strong>the</strong> gamma<br />

ray <strong>and</strong> density log response. The<br />

top <strong>of</strong> <strong>the</strong> Morrow (Figure 5) was<br />

generally difficult to pick but is<br />

<strong>of</strong>ten associated with a drop in<br />

density associated with <strong>the</strong><br />

predominantly clastic Morrow<br />

deposits. The basal Morrow<br />

channel is a low γ ray, high<br />

porosity zone that overlies <strong>the</strong> high<br />

Top <strong>of</strong> <strong>the</strong> Morrow<br />

γ ray Barnett shale (Figure 5)<br />

Basal Morrow<br />

Channel<br />

Figure 6: Time structure<br />

on top <strong>of</strong> <strong>the</strong> Chester Fm.<br />

Figure 7: Structure contour<br />

map: top <strong>of</strong> <strong>the</strong> Atoka Fm.<br />

Figure 8: <strong>Seismic</strong> pr<strong>of</strong>ile<br />

passing through <strong>the</strong> Lula #3<br />

well.<br />

Can – top <strong>of</strong> <strong>the</strong> Canyon<br />

Formation;<br />

St – top <strong>of</strong> <strong>the</strong> Strawn<br />

Formation;<br />

At – top <strong>of</strong> <strong>the</strong> Atoka<br />

Formation;<br />

1C – top <strong>of</strong> <strong>the</strong> Mississippian<br />

Chester Formation.<br />

Figure 9: Atoka to Chester<br />

Isochore Map.


Structure on <strong>the</strong> top <strong>of</strong> <strong>the</strong> Chester<br />

<strong>and</strong> Atoka formations is shown in<br />

Figures 10 <strong>and</strong> 11. In general <strong>the</strong><br />

structure follows <strong>the</strong> nor<strong>the</strong>ast trend<br />

<strong>of</strong> <strong>the</strong> Northwestern Shelf; however,<br />

north trending structural indentations<br />

interrupt <strong>the</strong> regional trend within <strong>the</strong><br />

field. Comparison <strong>of</strong> <strong>the</strong> time <strong>and</strong><br />

structure maps suggests that <strong>the</strong><br />

north trending faults observed in <strong>the</strong><br />

<strong>3D</strong> seismic <strong>data</strong> are probably<br />

associated with <strong>the</strong> structural<br />

indentation portrayed in <strong>the</strong> well<br />

derived structure maps.<br />

Figure 11: Structure on <strong>the</strong><br />

top <strong>of</strong> <strong>the</strong> Atoka Formation<br />

Structure & Isopach Maps<br />

Figure 10: Structure on <strong>the</strong><br />

top <strong>of</strong> <strong>the</strong> Atoka Formation<br />

Figure 12: Isopach map: top <strong>of</strong><br />

<strong>the</strong> Atoka to top <strong>of</strong> <strong>the</strong> Chester<br />

The isochore map <strong>of</strong> <strong>the</strong> Atoka to Chester top (Atoka through<br />

Morrow) reflection times (Figure 9) shows thickening along <strong>the</strong><br />

westernmost fault as well as across <strong>the</strong> sou<strong>the</strong>rn extent <strong>of</strong> <strong>the</strong> fault<br />

block in <strong>the</strong> survey area. The sou<strong>the</strong>rn part <strong>of</strong> <strong>the</strong> block appears to<br />

have rotated south-southwest during deposition, <strong>and</strong> at <strong>the</strong> same<br />

time <strong>the</strong>re appears to have been local subsidence across <strong>the</strong><br />

western fault that diminished to <strong>the</strong> north along its length. Reduced<br />

travel time differences observed in <strong>the</strong> Atoka-Morrow isochore to<br />

<strong>the</strong> north, along <strong>the</strong> trend <strong>of</strong> <strong>the</strong> western fault, show some similarity<br />

to <strong>the</strong> decreased thickness <strong>of</strong> <strong>the</strong> interval observed in <strong>the</strong> isopach<br />

map (Figure 12).<br />

The Atoko-Morrow isopach map (Figure 12) reveals that in <strong>the</strong><br />

nor<strong>the</strong>rn part <strong>of</strong> <strong>the</strong> <strong>3D</strong> survey area <strong>the</strong> Atoka-Morrow interval is<br />

over 100 feet thick, <strong>and</strong> increases to over 200 feet thick in <strong>the</strong><br />

south. The well derived maps provide a much coarser view <strong>of</strong> <strong>the</strong><br />

subsurface, with well spacing <strong>of</strong> about 2000 feet on average.<br />

However a pronounced trend <strong>of</strong> thickened Atoka-Morrow is clearly<br />

revealed along <strong>the</strong> trend <strong>of</strong> <strong>the</strong> seismic interpreted fault block.<br />

Future efforts will include conversion <strong>from</strong> timer to depth based on<br />

available sonic <strong>and</strong> well control <strong>from</strong> <strong>the</strong> field<br />

Production Data<br />

Five year cumulative production <strong>data</strong> <strong>from</strong> <strong>the</strong> <strong>Buffalo</strong> Valley field<br />

are shown in figures 13 <strong>and</strong> 14. Production <strong>data</strong> <strong>from</strong> two wells<br />

(highlighted in yellow) in <strong>the</strong> southwest corner <strong>of</strong> <strong>the</strong> area were<br />

omitted since production <strong>from</strong> <strong>the</strong>se wells was much higher (60471<br />

<strong>and</strong> 25725 Bbl ) than that in surrounding wells making it difficult to<br />

portray <strong>the</strong> production pattern on a linear contour scale when <strong>the</strong>se<br />

two wells were included. The average 5 year cumulative production<br />

obtained <strong>from</strong> 57 wells in <strong>the</strong> field is 4842.07 Bbl<br />

Figure 13: Oil production (units<br />

in barrels <strong>of</strong> oil)<br />

<strong>Seismic</strong> Attributes<br />

Figure 15: Average instantaneous<br />

frequency observed in a 0.014 sec<br />

window centered on <strong>the</strong> Morrow<br />

Figure 14: Gross s<strong>and</strong><br />

thickness within <strong>the</strong><br />

Morrow Interval<br />

Figure 16: Average instantaneous<br />

envelope observed in a 0.014 sec<br />

window centered on <strong>the</strong> Morrow.<br />

Preliminary attribute assessment suggests some relationship<br />

between spatial variations <strong>of</strong> instantaneous frequency (Figure 15) <strong>and</strong><br />

envelope (Figure 16) to production distribution. The average value <strong>of</strong><br />

<strong>the</strong> attribute was extracted <strong>from</strong> a 14 ms window centered roughly in<br />

<strong>the</strong> Morrow reflection event. A distinct channel-like pattern is not<br />

observed in <strong>the</strong> attribute maps. The productive Morrow s<strong>and</strong>s are<br />

generally less than 30 feet thick <strong>and</strong> are below <strong>the</strong> resolution limit <strong>of</strong><br />

<strong>the</strong> <strong>3D</strong> seismic <strong>data</strong>; however, areas <strong>of</strong> low instantaneous frequency<br />

coincide roughly with highs in <strong>the</strong> 5-year cumulative production within<br />

<strong>the</strong> survey area.<br />

P to S converted wave <strong>data</strong><br />

The <strong>3D</strong> seismic <strong>data</strong> set also includes a converted P to S wave<br />

volume. Side-by-side examples <strong>of</strong> <strong>the</strong> P-wave <strong>and</strong> PS-wave <strong>data</strong><br />

are shown below (figures 17 <strong>and</strong> 18 respectively). A pronounced<br />

zone <strong>of</strong> reduced amplitude is observed in <strong>the</strong> PS-wave <strong>data</strong><br />

volume that is not observed in <strong>the</strong> P-wave section. This zone <strong>of</strong><br />

low amplitude <strong>and</strong> reflection coherence may be associated with a<br />

narrow fracture zone (potentially gas filled).<br />

Figure 18: Display<br />

<strong>of</strong> P to S-wave<br />

<strong>data</strong> along pr<strong>of</strong>ile<br />

shown in Figure<br />

17.<br />

Figure 17: P-Wave<br />

seismic pr<strong>of</strong>ile<br />

through <strong>the</strong> Lula #3<br />

VSP well.<br />

Conclusion<br />

A tie between syn<strong>the</strong>tic <strong>and</strong> surface seismic proved difficult to<br />

establish. Comparison <strong>of</strong> well log derived syn<strong>the</strong>tics to <strong>the</strong> VSP<br />

near-<strong>of</strong>fset corridor stack was essential to identifying two-way<br />

travel times to formation tops <strong>and</strong> corresponding reflection events<br />

observed in <strong>the</strong> <strong>3D</strong> surface seismic. The response <strong>of</strong> <strong>the</strong> Atoka-<br />

Morrow intervals observed in <strong>the</strong> <strong>3D</strong> VSP confirms observations<br />

<strong>of</strong> <strong>the</strong> well log response in <strong>the</strong> field that <strong>the</strong> Atoka-Morrow interval<br />

is heterogeneous at interwell <strong>and</strong> seismic (Fresnel Zone) scales.<br />

The log response <strong>of</strong> <strong>the</strong> Morrow, is difficult to correlate <strong>from</strong> well<br />

to well whereas <strong>the</strong> top <strong>of</strong> <strong>the</strong> Chester Formation proved to be a<br />

more useful marker horizon.<br />

The <strong>3D</strong> seismic <strong>data</strong> <strong>from</strong> <strong>the</strong> field reveal that <strong>the</strong> play is<br />

bounded by nearly vertical faults that step down to <strong>the</strong> east. The<br />

faults are oriented roughly north-south at an angle to <strong>the</strong> NE<br />

trending shelf in this area. The eastern fault terminates to <strong>the</strong><br />

north while <strong>of</strong>fsets along <strong>the</strong> western fault decrease to <strong>the</strong> south.<br />

There appears to have been some movement along <strong>the</strong> faults<br />

during deposition <strong>of</strong> <strong>the</strong> Atoka-Morrow interval. Observable fault<br />

<strong>of</strong>fsets are located near <strong>the</strong> center <strong>of</strong> <strong>the</strong> field on <strong>the</strong> western fault<br />

<strong>and</strong> near <strong>the</strong> sou<strong>the</strong>rn end <strong>of</strong> <strong>the</strong> field along <strong>the</strong> eastern fault.<br />

Production <strong>from</strong> <strong>the</strong> Pennsylvanian Morrow Formation along<br />

<strong>the</strong> Northwest Shelf <strong>of</strong> <strong>the</strong> Permian Basin is generally confined to<br />

channel s<strong>and</strong>s at <strong>the</strong> base <strong>of</strong> <strong>the</strong> Morrow. These s<strong>and</strong>s are<br />

generally identifiable by low γ ray <strong>and</strong> high neutron porosity log<br />

response. Log derived structure <strong>and</strong> isopach maps reveal <strong>the</strong><br />

influence <strong>of</strong> <strong>the</strong> faults observed in <strong>the</strong> seismic. Structure maps<br />

clearly reveal that <strong>the</strong> field sits on an interruption in <strong>the</strong> regional<br />

trend <strong>of</strong> <strong>the</strong> Northwest Shelf. The Atoka-Morrow isopach reveals<br />

thickening <strong>of</strong> <strong>the</strong> Atoka-Morrow interval along <strong>the</strong> trend <strong>of</strong> <strong>the</strong><br />

fault block. Atoka-Morrow thickening increases <strong>from</strong> north to<br />

south suggesting that <strong>the</strong> fault block may have rotated to <strong>the</strong><br />

south during deposition <strong>of</strong> <strong>the</strong> Atoka-Morrow interval, consistent<br />

with observations made in <strong>the</strong> <strong>3D</strong> seismic <strong>data</strong> volume.<br />

Analysis <strong>of</strong> <strong>the</strong> P to S converted wave <strong>data</strong> suggests it will help<br />

identify additional faults or fracture zones within <strong>the</strong> field. Nearly<br />

vertical low amplitude zones appear in <strong>the</strong> P to S-wave <strong>data</strong> that<br />

could not o<strong>the</strong>rwise be easily identified in <strong>the</strong> P-wave volume.<br />

The analysis <strong>of</strong> seismic attributes <strong>and</strong> <strong>the</strong>ir correlation to<br />

production is in its early stages. Possible relationships between<br />

spatial variability in seismic attribute response <strong>and</strong> production<br />

<strong>from</strong> <strong>the</strong> Morrow channel will be examined in more<br />

comprehensive detail as <strong>the</strong> study continues.<br />

References<br />

Oil <strong>and</strong> gas fields <strong>of</strong> sou<strong>the</strong>astern New Mexico, Roswell Geological<br />

Society, 1999 & 1977 Supplements.<br />

Acknowledgements<br />

This research was funded through DOE/NETL contract DE-FC26-<br />

03NT41629. Our thanks to WesternGeco for providing <strong>the</strong> <strong>3D</strong><br />

seismic <strong>data</strong> <strong>from</strong> <strong>the</strong> area. The comments <strong>of</strong> Dave Oldham were<br />

greatly appreciated. Much <strong>of</strong> <strong>the</strong> well <strong>data</strong> were obtained <strong>from</strong> <strong>the</strong><br />

New Mexico Energy, Minerals, <strong>and</strong> Natural Resources Department<br />

Oil Conservation Division at http://ocdimage.emnrd.state.nm.us/.<br />

Production <strong>data</strong> used in <strong>the</strong> study were obtained <strong>from</strong> <strong>the</strong> New<br />

Mexico Tech “Go-Tech” site at http://octane.nmt.edu/<strong>data</strong>/ ongard/.

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