eastranch p2 final - kansas geological survey · seismic isochron map clearly shows several...

1
SEISMIC HORIZON ANALYSIS AND RESERVOIR CHARACTERIZATION Cross plot of isopach vs. seismic isochron for the base of karst to x marker interval. The correlation is generally good. The two outliers circled in red at the top of the plot are locations where the “x” marker picks in the wells are questionable and may need to be adjusted. Seismic isochron map (in two-way travel time) of the interval from the base of karst to the “x” marker with top of San Andres subsea depth contours superimposed. SEISMIC TIED TO FORMATION TOPS Formation tops were tied to seismic horizons using synthetic seismograms. Synthetic seismograms were constructed for 11 wells in the study area with both sonic and density logs and an additional 51 wells with sonic logs only. The synthetic seismograms show that there is not a significant impedance contrast at the top of the San Andres Formation in the study area, and therefore, this stratigraphic boundary does not correspond to a seismic reflection. There is an impedance contrast at the base of the karst zone between non-porous anhydrite and porous reservoir, however. Similarly, there is a positive impedance contrast at the “x” marker, although it does not correspond to a clear seismic peak. Locations of wells in the Waddell Field study area with sonic logs (blue) and both sonic and density logs (red). 1261 1,500 ft Synthetic seismogram for well #1261 showing tie with seismic data. Labeled tops are: top Grayburg (GRBG; dark green), top San Andres (SADR; cyan), base of anhydritic section beneath the top of San Andres (B_ANHY; magenta), base of tight zone beneath top of San Andres (B_POR; light green), “x” marker (X_MKR; blue). GRBG SADR X_MKR B_POR B_ANHY Center of gravity of porosity for the interval from the base of karst to the “x” marker measured in feet subsea. Lower center of gravity (blue) corresponds to higher mean porosity. Map of mean seismic impedance for the interval from the base of karst to the “x” marker. Mean porosity contours from well logs are superimposed. Cross plot of mean porosity versus mean impedance from well logs (red) and from seismic data (blue) for the interval between the base of the tight (karst) zone and the “x” marker. POROSITY AND SEISMIC IMPEDANCE To evaluate the potential usefulness of using seismic impedance to predict porosity, we first computed well log impedance for all wells containing sonic and density logs. From this log impedance, we calculated the mean impedance for the base of karst to “x” marker interval. A cross plot of the mean log impedance versus the mean porosity for the same interval shows that the two measures are well correlated. Mean impedance was also generated from the seismic data for the interval between the base of karst and “x” marker horizons. This mean seismic impedance is also cross plotted against mean porosity at the well locations. Although there is more scatter than for the log data, the seismic data show the same trend of decreasing porosity with increasing impedance. This correlation between impedance and porosity allows us to use a map of mean seismic impedance from the base of karst to “x” marker to approximate the distribution of mean porosity in areas with poor well control. The mean impedance shows bands of north-northeast-trending highs and lows that are oblique to the main structure in the area. The high impedance areas may correspond to the locations of porous San Andres shoals. HORIZON INTERPRETATIONS USING SEISMIC IMPEDANCE VOLUME In order to improve our interpretations of the base of karst and “x” marker horizons, we have generated a model-based impedance inversion of the seismic amplitude volume in the “high volume area”. Our starting model was based on the 11 wells in the area with sonic and density logs. The base of karst and “x” marker are much better defined in the resulting impedance volume than in the original amplitude volume. A horizon corresponding to the contrast between higher impedance above and lower impedance below that corresponds to the base of karst has been interpreted across the study area. A horizon corresponding to the “x”-marker can also be interpreted on the impedance volume. The “x” marker appears to be truncated by the base of karst horizon in the southern portion of the study area and locally in other areas. In the western part of the study area, the “x” marker appears to onlap onto a deeper horizon, interpreted as the top of G4. Vertical sections D-D' (top) and E-E' (bottom), flattened on the Grayburg horizon, through the East Ranch acoustic impedance volume. Note that the “x” marker horizon is truncated by the base of karst horizon at several locations and appears to onlap the G4 horizon. We interpreted data from a 3D seismic volume in a 2.5 mi x 3.4 mi (4.1 x 5.4 km) area surrounding the “high volume area” in Waddell Field. Our goal was to map the configuration of key horizons between well control and estimate the lateral distribution and continuity of petrophysical properties. Time structure map of the base of karst horizon below the top of the San Andres Formation. Cross sections D-D' and E-E' are located. Vertical section D-D' through the seismic amplitude volume (top) and an acoustic impedance volume (bottom) generated from the seismic amplitude data using model based inversion. The top Grayburg (green) and base of tight, anhydritic karst (cyan) interpreted from well data are shown connected by straight lines. Well logs displayed are sonic (dark red) and density (dark blue). D D' D D' D D' E E' 1 mile D D' E E' Grayburg Base Tight Zone “X” Marker G4 Grayburg Base Tight Zone G4 “X” Marker ISOCHRON MAPPING A map has been generated of the isochron between the base of karst and “x” marker horizons. A cross plot of this isochron versus the isopach values generated from well tops has a generally good correlation, suggesting that the seismic isochron can be used to approximate changes in interval thickness in locations without well control. The seismic isochron map clearly shows several approximately north-south- trending thicks and thins in the reservoir interval, which appear to swing around from a north-northeast trend in the east to a north-northwest trend in the west. The isochron is locally thin in the saddle area of the southeast-trending anticline. The isochron map also shows areas where the x marker has been truncated by the karst (white areas on the map). These areas are located on the flanks, rather than the top, of the San Andres structure and have a primarily north to northeast orientation. In the southern part of the map, however, the area where the “x” marker is absent shows both a northeast trend that lines up with the saddle and a northwest trend that parallels the main trend of the anticline. When mean impedance is compared to the center of gravity of well log porosity, which specifies the depth of the porosity development in the interval between the base of karst and the “x” marker, it can be seen that the easternmost trend of low impedance (high mean porosity) corresponds closely to a low center of gravity, suggesting better developed porosity in the lower portion of the reservoir interval. In contrast, the central high impedance (low mean porosity) trend corresponds to a similar trend of higher center of gravity, suggesting that the porosity has shifted to higher levels in the interval and is of lower magnitude. The westernmost north-south trend of low impedance (high mean porosity) corresponds closely to a low center of gravity, confirming a general relationship that porosity that is developed lower in the interval is greater in magnitude.

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Page 1: eastranch p2 final - Kansas Geological Survey · seismic isochron map clearly shows several approximately north-south-trending thicks and thins in the reservoir interval, which appear

SE

ISM

IC H

OR

IZO

NA

NA

LY

SIS

AN

D R

ES

ER

VO

IR C

HA

RA

CT

ER

IZA

TIO

N

Cro

ss

plo

t of is

op

ac

h v

s. s

eis

mic

iso

ch

ron

for th

e b

as

eo

f ka

rst to

x m

ark

er in

terv

al. T

he

co

rrela

tion

is g

en

era

llyg

oo

d. T

he

two

ou

tliers

circ

led

in re

d a

t the

top

of th

ep

lot a

re lo

ca

tion

s w

he

re th

e“x

”m

ark

er p

ick

s in

the

we

lls a

re q

ue

stio

na

ble

an

d m

ay

ne

ed

to b

e a

dju

ste

d.

Se

ism

ic is

oc

hro

n m

ap

(in tw

o-w

ay

trav

el tim

e) o

f the

inte

rva

l from

the

ba

se

of k

ars

t to th

e“x

”m

ark

er w

ith to

p o

f Sa

nA

nd

res

su

bs

ea

de

pth

co

nto

urs

su

pe

rimp

os

ed

.

SE

ISM

IC T

IED

TO

FO

RM

AT

ION

TO

PS

Fo

rma

tion

top

s w

ere

tied

to s

eis

mic

ho

rizons u

sin

g s

ynth

etic

se

ism

og

ram

s. S

ynth

etic

seis

mo

gra

ms w

ere

constru

cte

d fo

r11

we

lls in

the s

tudy a

rea w

ith b

oth

son

ic a

nd

density

logs

an

d a

n a

dd

itiona

l 51 w

ells

with

sonic

logs o

nly.

Th

e s

yn

the

tic s

eis

mogra

ms s

ho

w th

at th

ere

is n

ot a

sig

nific

an

t imp

ed

ance c

ontra

st a

t the to

p o

f the S

an

Andre

sF

orm

atio

n in

the s

tudy a

rea, a

nd th

ere

fore

, this

stra

tigra

phic

bo

un

da

ry d

oes n

ot c

orre

spond to

a s

eis

mic

refle

ctio

n.T

here

is a

n im

pe

da

nce c

ontra

st a

t the

base o

f the k

ars

t zon

eb

etw

ee

n n

on

-poro

us a

nh

ydrite

and p

oro

us re

serv

oir,

ho

we

ve

r. Sim

ilarly, th

ere

is a

po

sitiv

e im

pedan

ce c

on

trast a

tth

e“x

”m

ark

er, a

lthough

it does n

ot c

orre

spon

d to

a c

lear

se

ism

ic p

ea

k.

Lo

ca

tion

s o

f we

lls in

the

Wa

dd

ell F

ield

stu

dy

are

a w

ith s

on

iclo

gs

(blu

e) a

nd

bo

th s

on

ic a

nd

de

ns

ity lo

gs

(red

).

12

61

1,5

00

ft

Sy

nth

etic

se

ism

og

ram

for w

ell #

12

61

sh

ow

ing

tie w

ith s

eis

mic

da

ta. L

ab

ele

d to

ps

are

: top

Gra

yb

urg

(GR

BG

; da

rk g

ree

n), to

pS

an

An

dre

s (S

AD

R; c

ya

n), b

as

e o

f an

hy

dritic

se

ctio

n b

en

ea

thth

e to

p o

f Sa

nA

nd

res

(B_

AN

HY

; ma

ge

nta

), ba

se

of tig

ht z

on

eb

en

ea

th to

p o

f Sa

nA

nd

res

(B_

PO

R; lig

ht g

ree

n),

“x

”m

ark

er

(X_

MK

R; b

lue

).

GR

BG

SA

DR

X_M

KR

B_P

OR

B_A

NH

Y

Ce

nte

r of g

rav

ity o

f po

ros

ity fo

r the

inte

rva

l from

the

ba

se

of k

ars

t to th

e“x

”m

ark

er m

ea

su

red

in fe

et

su

bs

ea

. Lo

we

r ce

nte

r of g

rav

ity (b

lue

) co

rres

po

nd

s to

hig

he

r me

an

po

ros

ity.

Ma

p o

f me

an

se

ism

ic im

pe

da

nc

e fo

r the

inte

rva

l from

the

ba

se

of k

ars

t to th

e“x

”m

ark

er. M

ea

n p

oro

sity

co

nto

urs

from

we

ll log

s a

re s

up

erim

po

se

d.

Cro

ss

plo

t of m

ea

n p

oro

sity

ve

rsu

s m

ea

n im

pe

da

nc

efro

m w

ell lo

gs

(red

) an

d fro

m s

eis

mic

da

ta (b

lue

) for th

ein

terv

al b

etw

ee

n th

e b

as

e o

f the

tigh

t (ka

rst) z

on

e a

nd

the

“x

”m

ark

er.

PO

RO

SIT

YA

ND

SE

ISM

IC IM

PE

DA

NC

E

To

evalu

ate

the p

ote

ntia

l usefu

lness o

f usin

g s

eis

mic

impedance to

pre

dic

t poro

sity, w

e firs

t com

pute

d w

ell lo

g im

pedance fo

rall w

ells

conta

inin

g s

onic

and d

ensity

logs. F

rom

this

log im

pedance, w

e c

alc

ula

ted th

e m

ean im

pedance fo

r the b

ase o

f kars

tto

“x”

mark

er in

terv

al.

Acro

ss p

lot o

f the m

ean lo

g im

pedance v

ers

us th

e m

ean p

oro

sity

for th

e s

am

e in

terv

al s

how

s th

at th

etw

o m

easure

s a

re w

ell c

orre

late

d.

Me

an im

pedance

was a

lso g

enera

ted fro

m th

e s

eis

mic

data

for th

e in

terv

al b

etw

een th

e b

ase o

f kars

t and

“x”

mark

er

ho

rizons.T

his

mean s

eis

mic

impedan

ce is

als

o c

ross p

lotte

d a

gain

st m

ean p

oro

sity

at th

e w

ell lo

catio

ns.A

lthough th

ere

ism

ore

scatte

r tha

n fo

r the

log d

ata

, the

seis

mic

data

show

the s

am

e tre

nd o

f decre

asin

g p

oro

sity

with

incre

asin

g im

pedance.

Th

is c

orre

latio

n b

etw

een im

pedance a

nd p

oro

sity

allo

ws u

s to

use a

map o

f mean s

eis

mic

impe

dance fro

m th

e b

ase o

f kars

tto

“x”

mark

er to

appro

xim

ate

the d

istrib

utio

n o

f mean p

oro

sity

in a

reas w

ith p

oor w

ell c

ontro

l.

Th

e m

ean im

ped

ance s

how

s b

ands o

f north

-north

east-tre

ndin

g h

ighs a

nd lo

ws th

at a

re o

bliq

ue to

the m

ain

stru

ctu

re in

the

are

a.T

he h

igh im

pedan

ce a

reas m

ay c

orre

spond to

the lo

catio

ns o

f poro

us S

an

Andre

s s

hoals

.

HO

RIZ

ON

INT

ER

PR

ETA

TIO

NS

US

ING

SE

ISM

IC IM

PE

DA

NC

E V

OL

UM

E

In o

rder to

imp

rove o

ur in

terp

reta

tion

s o

f the

ba

se

of k

ars

t and

“x”

mark

er h

oriz

on

s, w

e h

ave g

en

era

ted

a m

od

el-b

ase

d im

pedan

ce in

vers

ion o

f the s

eis

mic

am

plitu

de v

olu

me in

the

“hig

h v

olu

me a

rea

”. Our s

tartin

gm

ode

l wa

s b

ase

d o

n th

e 1

1 w

ells

in th

e a

rea

with

so

nic

and d

ensity

logs.

The b

ase o

f ka

rst a

nd

“x”

ma

rker a

re m

uch

bette

r defin

ed in

the re

su

lting im

pedance v

olu

me th

an

in th

e o

rigin

al a

mplitu

de v

olu

me.

Aho

rizon

co

rresp

on

din

g to

the

co

ntra

st b

etw

ee

n h

igh

er im

pedance

above

and lo

wer im

pedance

belo

w th

at c

orre

spon

ds to

the b

ase o

f kars

t has b

een in

terp

rete

d a

cro

ss th

e s

tudy a

rea.

Aho

rizon

co

rresp

on

din

g to

the

“x”-m

ark

er c

an

als

o b

e in

terp

rete

d o

n th

e im

pedan

ce v

olu

me.

Th

e“x

”m

ark

er a

ppears

to b

e tru

ncate

d b

y th

e b

ase o

f kars

t ho

rizon in

the s

outh

ern

portio

n o

f the s

tudy a

rea a

nd lo

cally

ino

ther a

rea

s. In

the

we

ste

rn p

art o

f the

stu

dy a

rea

, the

“x”

ma

rker a

ppears

to o

nla

p o

nto

a d

eepe

r horiz

on, in

terp

rete

d a

s th

e to

p o

f G4.

Ve

rtica

l se

ctio

ns

D-D

' (top

) an

d E

-E' (b

otto

m), fla

tten

ed

on

the

Gra

yb

urg

ho

rizo

n,

thro

ug

h th

e E

as

t Ra

nc

h a

co

us

tic im

pe

da

nc

e v

olu

me

. No

te th

at th

e“x

”m

ark

er h

oriz

on

is tru

nc

ate

d b

y th

e b

as

e o

f ka

rst h

oriz

on

at s

ev

era

l loc

atio

ns

an

d a

pp

ea

rs to

on

lap

the

G4

ho

rizo

n.

We

inte

rpre

ted

da

ta fro

m a

3D

se

ism

icvo

lum

e in

a 2

.5 m

i x 3

.4 m

i (4.1

x 5

.4km

) are

a s

urro

un

din

g th

e“h

igh

vo

lum

eare

a”

in W

ad

de

ll Fie

ld. O

ur g

oa

l wa

s to

map

the c

on

figu

ratio

n o

f ke

y h

oriz

on

sbe

twe

en w

ell c

on

trol a

nd

estim

ate

the

late

ral d

istrib

utio

n a

nd c

ontin

uity

of

pe

trophysic

al p

rope

rties.

Tim

e s

truc

ture

ma

p o

f the

ba

se

of k

ars

t ho

rizo

n b

elo

w th

e to

p o

f the

Sa

nA

nd

res

Fo

rma

tion

. Cro

ss

se

ctio

ns

D-D

' an

d E

-E' a

re lo

ca

ted

.

Ve

rtica

l se

ctio

n D

-D' th

rou

gh

the

se

ism

ic a

mp

litud

e v

olu

me

(top

) an

d a

na

co

us

tic im

pe

da

nc

e v

olu

me

(bo

ttom

) ge

ne

rate

d fro

m th

e s

eis

mic

am

plitu

de

da

ta u

sin

g m

od

el b

as

ed

inv

ers

ion

. Th

e to

p G

ray

bu

rg (g

ree

n) a

nd

ba

se

of tig

ht,

an

hy

dritic

ka

rst (c

ya

n) in

terp

rete

d fro

m w

ell d

ata

are

sh

ow

n c

on

ne

cte

d b

ys

traig

ht lin

es

. We

ll log

s d

isp

lay

ed

are

so

nic

(da

rk re

d) a

nd

de

ns

ity (d

ark

blu

e).

DD

'

DD

'

D

D'

E

E'

1 m

ile

DD

'

EE

'

Gra

yb

urg

Ba

se

Tig

ht Z

on

e

“X

”M

ark

er

G4

Gra

yb

urg

Ba

se

Tig

ht Z

on

e

G4

“X

”M

ark

er

ISO

CH

RO

N M

AP

PIN

G

Am

ap h

as b

een g

enera

ted o

f the is

ochro

n b

etw

een th

e b

ase o

f kars

tand

“x”

mark

er h

oriz

ons.A

cro

ss p

lot o

f this

isochro

n v

ers

us th

e is

opach

valu

es g

enera

ted fro

m w

ell to

ps h

as a

genera

lly g

ood c

orre

latio

n,

suggestin

g th

at th

e s

eis

mic

isochro

n c

an b

e u

sed to

appro

xim

ate

changes in

inte

rval th

ickness in

loca

tions w

ithout w

ell c

ontro

l.T

he

seis

mic

isochro

n m

ap c

learly

show

s s

evera

l appro

xim

ate

ly n

orth

-south

-tre

ndin

g th

icks a

nd th

ins in

the re

se

rvoir in

terv

al, w

hic

h a

ppear to

sw

ing

aro

und fro

m a

north

-north

east tre

nd

in th

e e

ast to

a n

orth

-north

west

trend in

the w

est.

The

isochro

n is

locally

thin

in th

e s

addle

are

a o

f the

south

east-tre

ndin

g a

ntic

line.T

he is

ochro

n m

ap a

lso s

how

s a

rea

s w

here

the x

mark

er h

as b

ee

n tru

ncate

d b

y th

e k

ars

t (white

are

as o

n th

e m

ap).

These a

reas a

re lo

ca

ted o

n th

e fla

nks, ra

ther th

an th

e to

p, o

f the

San

Andre

s s

tructu

re a

nd h

ave a

prim

arily

north

to n

orth

east o

rienta

tion. In

the s

outh

ern

part o

f the m

ap, h

ow

ever, th

e a

rea w

here

the

“x”

mark

er is

absent s

how

s b

oth

a n

orth

east tre

nd th

at lin

es u

p w

ith th

e s

addle

and a

north

west tre

nd th

at p

ara

llels

the m

ain

trend o

f the a

ntic

line.

When m

ean im

pedance is

com

pare

d to

the c

ente

r of g

ravity

of w

ell lo

gpo

rosity, w

hic

h s

pecifie

s th

e d

epth

of th

e p

oro

sity

develo

pm

ent in

the

inte

rval b

etw

een th

e b

ase o

f kars

t and th

e“x

”m

ark

er, it c

an

be s

een th

at

the e

aste

rnm

ost tre

nd o

f low

impedance (h

igh m

ean p

oro

sity

)co

rresponds c

losely

to a

low

cente

r of g

ravity, s

uggestin

g b

ette

rde

velo

ped p

oro

sity

in th

e lo

we

r portio

n o

f the re

serv

oir in

terv

al. In

co

ntra

st, th

e c

entra

l hig

h im

pe

dance (lo

w m

ean p

oro

sity

) trend

co

rresponds to

a s

imila

r trend o

f hig

her c

ente

r of g

ravity, s

uggestin

g th

at

the p

oro

sity

has s

hifte

d to

hig

her le

vels

in th

e in

terv

al a

nd is

of lo

wer

magnitu

de.T

he w

este

rnm

ost n

orth

-south

trend o

f low

impe

dance (h

igh

mean p

oro

sity

) corre

sponds c

losely

to a

low

cente

r of g

ravity, c

onfirm

ing

a g

enera

l rela

tionship

that p

oro

sity

that is

develo

ped lo

wer in

the in

terv

al

is g

reate

r in m

agnitu

de.