3
58 SEISMIC  PROPERTIES OF V OLCA NIC ROCK S FROM  HESS  RISE 1 N .  I.  Christensen, R. H . W ilkens, S. M. Lundqu ist, and J . P . Schultz, Depa rtment of Geological Sc ience s and Graduate  Program in Geophysics, University of Washington, Seattle, Washington INTRODUCTION Hess Ris e, a major struct ural feature in the  northern Pacific, is one o f sev eral oceanic plateaus whi ch a ppar- ently  possess  anomalous seismic structures  (Sutton  et al., 1971).  Hence,  Laboratory measurements of  com- pressiona l- and s hear- wav e vel ocities in rocks from oceanic  plateau regions are of considerable interest. Sev eral qu estions come to mind : (1) Are compressional  wave  velocities of volcanic rocks from oceanic plateaus similar to basalts of equivalent age from normal oceanic crust? (2) Do vel ocity- density relations fo r plateau rocks fi t t he wel l- established tre nds for Layer 2 basalts? (3) How do Poisson's ratios, determined from  compres- sional- and shear-wav e v elocities, of oceanic plateau rocks compare w ith those of normal s ea- floor basalts? To  answ er these questions, we have selected for velocity measurements  five  v olcanic samples from di f - ferent depths (Fig. 1) from Hole  465A,  on southern Hess Rise. It is particularly significant  that  all the rocks are vesicular and have b een highly altered , whi ch  signifi- cantly affects their elasti c prop erties. SAMPLE DESCRIPTIONS, EXPERIMENTAL  PR OCE DURE, A ND  DATA Four  of the  five  samples are from the lower volcanic units  an d one is f rom the upper v olcanic breccia (F ig .  1). One  third of the breccia  (46 5A- 41 - 1)  consists of volcanic clasts 5 mm in diameter in a carbonate matrix. The clas ts range f rom semi- angul ar to roun ded, depending on  the degree of alteration to carbonate along the grain boundaries.  The remainder of the sample consists of a fi ve- g rained volcanic rock and may compose a larger clast in the breccia. The  remaining four samples are highly altered, fine- grained, vesicular volcanic rocks. They are porphyritic, with plagioclase phenocrysts in a  glassy  matrix, and they contain  abundant plagioclase microlites. The  glass  has been  altered to smectite.  Vesicles  range in  size  from  0.5 to  1 mm and are often  filled  with carbonate, as are many  small veins and fractures. Some  flow  structure is apparent  in one sample (46 5A - 4 2- 1), where the  vesicles are elongated parallel to the trachytic plagioclase microlites. No mafic minerals are present in any of the samples, and the opaque minerals are unaltered. Com pressional- wave vel ocities have been measured in  all  five  samples (Table  1),  and shear- wave velocities in three  (Table 2), using the pulse- transmiss ion t echnique Initial Reports of the Deep Sea Drilling Project Volume  62. descr ibed in deta il b y Birch (1960 ). All velocities were measur ed at room t empera ture, us ing water- saturated samples. The samples were jacketed with copper foil, and  100 - mes h screens were placed between t he cores and copper  jackets to provide space for water to drain from grain- boundary cracks as confi ning pressure was in- creased. Thus, pore pressure was kept much lower  than confining pressure. The importance of using this tech- nique  in measurin g v elocities in ocea nic rocks is dis- cussed by Christen sen and Salisbury (1975 ). Bulk den- sities (Table 1) were calculated from the weights and dimensions of the water- saturated samples. I n  add ition t o she ar- wav e veloci ties  V ),  the ratios of compressional- t o s hear- wav e v elocities  V p /V s ), Poisson's  ratios (σ ), bulk moduli  K ),  shear moduli  (µ), Lamé s constants  ( λ ), and  Young's  moduli  E)  are  given in  Table 2 at various pressures. The elastic constants were calculated from the velocities and densities, fol- lowing  the equations of Birch  (1961). DISCUSSION Figure 2  shows  compress ional- an d she ar- w v e velocities at 0.5 kbar  versus  wet- bulk density fo r the data  in Tables 1 and 2. In cluded i n this  figure  are data points  and non - linear reg ress ion curv es presented by Christensen  an d Salisbury (197 5) f or  DSDP  basalts. It is apparent  that  while the measured velocities for our sam- ples generally agree with the basalt trend, they are significantly lower  than  those of most samples studied. Of the Pacific Ocean basin samples used in the original velocity-density corr elation , onl y f our exhibited co m- pressional- wav e velocities  less  than  4.3  km/s  (Christen- sen, 1973; Christensen and Salisbury, 19 73). The  reasons for the low seismic velocities of our sam- ples appear to be the  pe rvasiv e  alteration of th e primary minerals an d the v esicularity of the rocks. Al thou gh calcite replacement of plagioclase should not seriously reduce  seismic velocities, the alteration of the  glassy mat rix to smectite s hould have a s ignificant eff ect. Poro sity - vel ocity relationships have b een examined prev iousl y fo r Atlantic Ocean basin basalts, and a good correlation  w as observed between a decrease in sei smic velocity and an increase in porosity (Christensen et al., 19 80 ). Based on wet an d dry weights of our samples, we estimate  that  th eir porosities range between 10 and 20 . It  is interesting to note  that  whereas other Pacific basin  DSDP  basalt samples g enerally exhibit relativel y higher seismic velocities, seismic velocities recently measured for basalt samples from island-arc and back- arc-basin areas (Christens en, Blai r, et al., in press; 1005

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58 SEISM IC

PROPERTIES OF VOLCANIC ROCKS FROM

H E S S RISE

1

N

I

Christensen R H Wilkens S M Lundquist and J P Schultz Department of Geological Sciences and

Graduate Program in Geophysics University of Washington Seattle Washington

INTRODUCTION

Hess Rise a major structural feature in the northern

Pacific is one of several oceanic plateaus which appar983085

ently possess anomalous seismic structures (Sutton et

al 1971)

Hence

Laboratory measurements of com983085

pressional983085 and shear983085 wave velocities in rocks from

oceanic

plateau regions are of considerable interest

Several questions come to mind (1) Are compressional

wave

velocities of volcanic rocks from oceanic plateaus

similar to basalts of equivalent age from normal oceanic

crust (2) Do velocity983085density relations for plateau

rocks fit the well983085 established trends for Layer 2 basalts

(3) How do Poissons ratios determined from

compres983085

sional983085 and shear983085wave velocities of oceanic plateau

rocks compare with those of normal sea983085 floor basalts

To

answer these questions we have selected for

velocity measurements five volcanic samples from dif983085

ferent depths (Fig 1) from Hole 465A on southern

Hess Rise It is particularly significant

that

all the rocks

are vesicular and have been highly altered which signifi983085

cantly affects their elastic properties

SAMPLE DESCRIPTIONS

EXPERIMENTAL

PROCEDURE AND DATA

Four

of the

five

samples are from the lower volcanic

units

and one is from the upper volcanic breccia (F ig

1)

One third of the breccia (465A983085 41983085 1) consists of volcanic

clasts 5 mm in diameter in a carbonate matrix The

clasts range from semi983085 angular to rounded depending

on

the degree of alteration to carbonate along the grain

boundaries

The remainder of the sample consists of a

five983085grained volcanic rock and may compose a larger

clast in the breccia

The remaining four samples are highly altered fine983085

grained vesicular volcanic rocks They are porphyritic

with plagioclase phenocrysts in a glassy matrix and they

contain

abundant plagioclase microlites The glass has

been

altered to smectite

Vesicles

range in size from

05

to

1 mm and are often filled with carbonate as are

many

small veins and fractures Some

flow

structure is

apparent

in one sample (465A983085429830851) where the

vesicles

are elongated parallel to the trachytic plagioclase

microlites No mafic minerals are present in any of the

samples and the opaque minerals are unaltered

Compressional983085 wave velocities have been measured

in

all five samples (Table

1)

and shear983085 wave velocities in

three (Table 2) using the pulse983085 transmission technique

Initial Reports of the Deep Sea Drilling Project

Volume

62

described in detail by Birch (1960) All velocities were

measured at room temperature using water983085 saturated

samples The samples were jacketed with copper foil

and 100983085mesh screens were placed between the cores and

copper

jackets to provide space for water to drain from

grain983085 boundary cracks as confining pressure was in983085

creased Thus pore pressure was kept much lower

than

confining pressure The importance of using this tech983085

nique

in measuring velocities in oceanic rocks is dis983085

cussed by Christensen and Salisbury (1975) Bulk den983085

sities (Table 1) were calculated from the weights and

dimensions of the water983085 saturated samples

In

addition to shear983085wave velocities

V

s

)

the ratios

of compressional983085 to shear983085wave velocities V

p

V

s

)

Poissons

ratios (σ ) bulk moduli

K)

shear moduli

(micro )

Lameacute s constants (λ ) and Youngs moduli

E)

are given

in

Table 2 at various pressures The elastic constants

were calculated from the velocities and densities fol983085

lowing the equations of Birch

(1961)

DISCUSSION

Figure 2 shows compressional983085 and shear983085wave

velocities at 05 kbar versus wet983085 bulk density for the

data in Tables 1 and 2 Included in this figure are data

points

and non983085 linear regression curves presented by

Christensen

and Salisbury (1975) for

D SD P

basalts It is

apparent

that

while the measured velocities for our sam983085

ples generally agree with the basalt trend they are

significantly lower

than

those of most samples studied

Of the Pacific Ocean basin samples used in the original

velocity983085density correlation only four exhibited com983085

pressional983085wave velocities less

than

43

kms (Christen983085

sen 1973 Christensen and Salisbury 1973)

The reasons for the low seismic velocities of our sam983085

ples appear to be the pervasive alteration of the primary

minerals and the vesicularity of the rocks Although

calcite replacement of plagioclase should not seriously

reduce

seismic velocities the alteration of the glassy

matrix to smectite should have a significant effect

Porosity983085 velocity relationships have been examined

previously for Atlantic Ocean basin basalts and a good

correlation

was observed between a decrease in seismic

velocity and an increase in porosity (Christensen et al

1980) Based on wet and dry weights of our samples we

estimate

that

their porosities range between 10 and

20

I t

is interesting to note

that

whereas other Pacific

basin D SD P basalt samples generally exhibit relatively

higher seismic velocities seismic velocities recently

measured for basalt samples from island983085 arc and back983085

arc983085 basin areas (Christensen Blair et al in press

1005

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N I CHRISTENSEN R H WILKENS S M LUNDQUIST J P SCHULTZ

Lithology

Limestone

Sampled

Section

Breccia

Bo t tom

of Breccia

Medium Grained

Vesicular

Fine Gra ined

Highly Vesicular

Coarse Grained

Fine Gra ined

Amygdaloida l

983085 4 2 0

^ 4 3 0

4 1 0

983085465A 98308541 9830851

465A 98308542 9830851

983085440 E

o

983085 4 5 0

983085465A 98308544 9830853

983085465A 98308545 9830851

983085 4 6 0

983085465A 98308546 9830852

983085 4 7 0

Figure 1 Sample locations and basement lithology of Hole 465A

Table 1 Compressional983085wave velocities

F

p

)

Sample

interval

in cm)

465A 41983085 1 9098308595

465A 42983085 1 134983085139

465A 449830853

138983085143

465A 5983085 1 7698308581

465A 46983085 2

5598308560

Porosity

)

14 80

14 95

10 54

896

10 35

Wet983085 Bulk

Density

gcm)

2770

2090

2306

2 310

2273

Velocity

km s)

at Varying Pressures

kbar)

02

333

329

396

400

379

04

340

334

398

4 0 3

383

06

344

337

399

405

387

08

347

340

399

408

389

10

350

3 4 3

399

410

3 91

Table 2 Elastic constants and

shear983085wave

velocities F

s

)

Sample Pressure

interval in cm) kbar) km s) V

p

V

s

Mbar)

Mbar)

E

Mbar)

λ

Mbar)

465A^49830853 138983085143

465A98308545983085 1 7698308581

465A983085 469830852 5598308560

040

060

080

100

020

040

060

080

100

020

040

060

080

100

201

202

202

203

203

206

208

209

209

210

186

189

191

194

196

197

197

198

197

197

194

194

194

195

195

204

203

203

201

199

033

033

033

033

033

032

032

032

032

032

034

034

034

033

024

024

024

024

024

024

024

024

025

025

022

023

023

023

009

009

009

010

010

010

010

010

010

010

008

008

008

009

025

025

025

025

025

026

026

027

027

027

021

022

022

023

018

018

018

018

018

017

018

018

018

018

017

017

017

017

017

7 0

6 0

5 0

140

3 0

2 0

DSDP Basalts

0 5 kbar

y

2 0 2 2 24 2 6

Density g cm3)

28

3 0

Figure 2 Compressional and shear983085wave

velocities

at 05 kbar versus

wet983085bulk density Solid triangles represent data from this study

other data are from Christensen and Salisbury (1975)

Christensen Wilkens

in

press) are often

in

the same

range

as

those

of

the Hess Rise samples reported here

Fur the rmore

the values

of

Poissons ratio reported

in

Table 2 are generally higher than the average

for

DSDP

basalts (Christensen and Salisbury 1975) but agree

well

with values reported from the island983085arc and back983085 arc983085

basin sites

I t is

unfortunate that there are no published seismic983085

refraction profiles

of the

Hess Rise This precludes

estimation

of the

depth

to

which these low983085velocity

rocks persist beyond the 70 meters directly sampled

by

drilling Future interpretation

of

seismic data

in

this

region must take into account the fact that velocity con983085

trasts

at

the sediment basement interface may

be sig983085

1006

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SEISMIC PROPERTIES

nificantly lower than those normally encountered in

ocean basins

KNOWLEDGMENTS

Financial support

for

this study was provided

by

Office

of

Naval

Research Contract N-0014-75-C-0502 The manuscript was reviewed

by

R I

Carlson

and S C

Blair

REFEREN ES

Birch F 1960

The

velocity

of

compressional waves

in

rocks

to 10

kilobars 1 J Geophys

Res

651083-1102

1961

The

velocity

of

compressional waves

in

rocks

to 10

kilobars

2

J

Geophys

Res 662199-2224

Christensen

N I

1973 Compressional

and

shear wave velocities

in

basaltic rocks Deep Sea Drilling Project Leg 16

In

van Andel

Tj H Heath

G

R

et

al

Init

Repts DSDP 16 Washington

US

Govt Printing Office) 647-649

Christensen

N I

Blair

S C

Prior

R C et al in

press Seismic

velocities at elevated pressures of igneous rocks from the Mariana

Trough

and

fore-arc region Deep

Sea

Drilling Project Leg 60 In

Hussong D Uyeda S et al Init Repts DSDP 60 Wash-

ington US Govt Printing Office)

Christensen

N I

Blair

S C

Wilkens

R

H

et al 1980 Com-

pressional wave velocities densities and porosities of basalts from

Holes 417A 417D and 418A Deep Sea Drilling Project Legs 51

through 53 In Donnelly

T

Francheteau

J

Bryan

W

Robin-

son R Flower M Salisbury M

et al Init Repts DSDP

51

52 53 Pt 1

Washington

(US

Govt Printing Office)

1467-

1472

Christensen N I and Salisbury M

H

1973 Velocities elastic

moduli

and

weathering-age relationships

for

Pacific layer

2 ba-

salts Earth

Planet

Sci

Lett

19461-465

1975 Structure

and

constitution

of

the lower oceanic crust

Rev Geophys Space

Phys

1357-86

Christensen N I W ilkens R H Blair S C et al in press Seismic

velocities densities

and

elastic co nstants

of

volcanic breccias

and

basalt from Deep

Sea

Drilling Project

Leg 59

In Kroenke L

Scott R et al Init Repts DSDP 59 Washington US Govt

Printing Office)

Sutton G H Maynard G H and Hussong D M 1971 Wide-

spread occurrence of a high-velocity basalt layer in the Pacific

crust found with repetitive sources

and

sonobuoys In Heacock

J

G Ed) The Structure and Physical roperties of the Earth s

Crust Geophys Monogr Ser 14 Washington (Am Geophys

Union) pp 193-209

1007

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httpslidepdfcomreaderfulldsdp6258 23

N I CHRISTENSEN R H WILKENS S M LUNDQUIST J P SCHULTZ

Lithology

Limestone

Sampled

Section

Breccia

Bo t tom

of Breccia

Medium Grained

Vesicular

Fine Gra ined

Highly Vesicular

Coarse Grained

Fine Gra ined

Amygdaloida l

983085 4 2 0

^ 4 3 0

4 1 0

983085465A 98308541 9830851

465A 98308542 9830851

983085440 E

o

983085 4 5 0

983085465A 98308544 9830853

983085465A 98308545 9830851

983085 4 6 0

983085465A 98308546 9830852

983085 4 7 0

Figure 1 Sample locations and basement lithology of Hole 465A

Table 1 Compressional983085wave velocities

F

p

)

Sample

interval

in cm)

465A 41983085 1 9098308595

465A 42983085 1 134983085139

465A 449830853

138983085143

465A 5983085 1 7698308581

465A 46983085 2

5598308560

Porosity

)

14 80

14 95

10 54

896

10 35

Wet983085 Bulk

Density

gcm)

2770

2090

2306

2 310

2273

Velocity

km s)

at Varying Pressures

kbar)

02

333

329

396

400

379

04

340

334

398

4 0 3

383

06

344

337

399

405

387

08

347

340

399

408

389

10

350

3 4 3

399

410

3 91

Table 2 Elastic constants and

shear983085wave

velocities F

s

)

Sample Pressure

interval in cm) kbar) km s) V

p

V

s

Mbar)

Mbar)

E

Mbar)

λ

Mbar)

465A^49830853 138983085143

465A98308545983085 1 7698308581

465A983085 469830852 5598308560

040

060

080

100

020

040

060

080

100

020

040

060

080

100

201

202

202

203

203

206

208

209

209

210

186

189

191

194

196

197

197

198

197

197

194

194

194

195

195

204

203

203

201

199

033

033

033

033

033

032

032

032

032

032

034

034

034

033

024

024

024

024

024

024

024

024

025

025

022

023

023

023

009

009

009

010

010

010

010

010

010

010

008

008

008

009

025

025

025

025

025

026

026

027

027

027

021

022

022

023

018

018

018

018

018

017

018

018

018

018

017

017

017

017

017

7 0

6 0

5 0

140

3 0

2 0

DSDP Basalts

0 5 kbar

y

2 0 2 2 24 2 6

Density g cm3)

28

3 0

Figure 2 Compressional and shear983085wave

velocities

at 05 kbar versus

wet983085bulk density Solid triangles represent data from this study

other data are from Christensen and Salisbury (1975)

Christensen Wilkens

in

press) are often

in

the same

range

as

those

of

the Hess Rise samples reported here

Fur the rmore

the values

of

Poissons ratio reported

in

Table 2 are generally higher than the average

for

DSDP

basalts (Christensen and Salisbury 1975) but agree

well

with values reported from the island983085arc and back983085 arc983085

basin sites

I t is

unfortunate that there are no published seismic983085

refraction profiles

of the

Hess Rise This precludes

estimation

of the

depth

to

which these low983085velocity

rocks persist beyond the 70 meters directly sampled

by

drilling Future interpretation

of

seismic data

in

this

region must take into account the fact that velocity con983085

trasts

at

the sediment basement interface may

be sig983085

1006

7262019 dsdp62_58

httpslidepdfcomreaderfulldsdp6258 33

SEISMIC PROPERTIES

nificantly lower than those normally encountered in

ocean basins

KNOWLEDGMENTS

Financial support

for

this study was provided

by

Office

of

Naval

Research Contract N-0014-75-C-0502 The manuscript was reviewed

by

R I

Carlson

and S C

Blair

REFEREN ES

Birch F 1960

The

velocity

of

compressional waves

in

rocks

to 10

kilobars 1 J Geophys

Res

651083-1102

1961

The

velocity

of

compressional waves

in

rocks

to 10

kilobars

2

J

Geophys

Res 662199-2224

Christensen

N I

1973 Compressional

and

shear wave velocities

in

basaltic rocks Deep Sea Drilling Project Leg 16

In

van Andel

Tj H Heath

G

R

et

al

Init

Repts DSDP 16 Washington

US

Govt Printing Office) 647-649

Christensen

N I

Blair

S C

Prior

R C et al in

press Seismic

velocities at elevated pressures of igneous rocks from the Mariana

Trough

and

fore-arc region Deep

Sea

Drilling Project Leg 60 In

Hussong D Uyeda S et al Init Repts DSDP 60 Wash-

ington US Govt Printing Office)

Christensen

N I

Blair

S C

Wilkens

R

H

et al 1980 Com-

pressional wave velocities densities and porosities of basalts from

Holes 417A 417D and 418A Deep Sea Drilling Project Legs 51

through 53 In Donnelly

T

Francheteau

J

Bryan

W

Robin-

son R Flower M Salisbury M

et al Init Repts DSDP

51

52 53 Pt 1

Washington

(US

Govt Printing Office)

1467-

1472

Christensen N I and Salisbury M

H

1973 Velocities elastic

moduli

and

weathering-age relationships

for

Pacific layer

2 ba-

salts Earth

Planet

Sci

Lett

19461-465

1975 Structure

and

constitution

of

the lower oceanic crust

Rev Geophys Space

Phys

1357-86

Christensen N I W ilkens R H Blair S C et al in press Seismic

velocities densities

and

elastic co nstants

of

volcanic breccias

and

basalt from Deep

Sea

Drilling Project

Leg 59

In Kroenke L

Scott R et al Init Repts DSDP 59 Washington US Govt

Printing Office)

Sutton G H Maynard G H and Hussong D M 1971 Wide-

spread occurrence of a high-velocity basalt layer in the Pacific

crust found with repetitive sources

and

sonobuoys In Heacock

J

G Ed) The Structure and Physical roperties of the Earth s

Crust Geophys Monogr Ser 14 Washington (Am Geophys

Union) pp 193-209

1007

Page 3: dsdp62_58

7262019 dsdp62_58

httpslidepdfcomreaderfulldsdp6258 33

SEISMIC PROPERTIES

nificantly lower than those normally encountered in

ocean basins

KNOWLEDGMENTS

Financial support

for

this study was provided

by

Office

of

Naval

Research Contract N-0014-75-C-0502 The manuscript was reviewed

by

R I

Carlson

and S C

Blair

REFEREN ES

Birch F 1960

The

velocity

of

compressional waves

in

rocks

to 10

kilobars 1 J Geophys

Res

651083-1102

1961

The

velocity

of

compressional waves

in

rocks

to 10

kilobars

2

J

Geophys

Res 662199-2224

Christensen

N I

1973 Compressional

and

shear wave velocities

in

basaltic rocks Deep Sea Drilling Project Leg 16

In

van Andel

Tj H Heath

G

R

et

al

Init

Repts DSDP 16 Washington

US

Govt Printing Office) 647-649

Christensen

N I

Blair

S C

Prior

R C et al in

press Seismic

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