bei chapter 3 - stanford university

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BEI Chapter 3

Monday, December 3, 12

Travel-time depth1500 m/s2000 m/s

2500 m/s3000 m/s

1000m

2000m

3000m4000m

z

Monday, December 3, 12

Travel-time depth1500 m/s2000 m/s

2500 m/s3000 m/s

Two-way travel-time1.331.00

0.80.670.8

z1000m

2000m

3000m4000m

Monday, December 3, 12

Travel-time depth1500 m/s

2000 m/s2500 m/s3000 m/s

1s

2s3s

Two-way travel-time1.331.00

0.80.670.8

4s⌧ =

2z

v

Monday, December 3, 12

Horizontal moving waves Offset

time

Monday, December 3, 12

Horizontal moving waves Offset

Head-wave

Groundroll, guided waves, direct arrivals

Monday, December 3, 12

LMO

Monday, December 3, 12

LMO

Critical angle

Monday, December 3, 12

Linear moveout

Monday, December 3, 12

LMO

Monday, December 3, 12

LMO

Head waves

Monday, December 3, 12

LMO

Monday, December 3, 12

LMO

Critical angle

Monday, December 3, 12

LMO

Critical angle

Monday, December 3, 12

Head wavesCritical angle

Monday, December 3, 12

LMO

Monday, December 3, 12

Mute

Monday, December 3, 12

Mute

Monday, December 3, 12

Muting

Input MutedMonday, December 3, 12

Dipping waves

z

x

ray

front

v

✓✓

Monday, December 3, 12

Dipping waves

z

x

ray

front

v

✓✓

z0

Monday, December 3, 12

Dipping waves

z

x

ray

front

vz = z0 � x tan ✓

✓✓

z0

Monday, December 3, 12

Dipping waves

z

x

ray

front

vz = z0 � x tan ✓

z0 =

vt

cos ✓

✓✓

z0

Monday, December 3, 12

Dipping waves

z

x

ray

front

vz = z0 � x tan ✓

✓✓

z0 z cos ✓ = vt� x sin ✓

t(x, z) =

z

v

cos ✓ +

x

v

sin ✓

Monday, December 3, 12

Dipping waves

z

x

ray

front

✓✓

z0

f

⇣t� x

v

sin ✓ � z

v

cos ✓

Monday, December 3, 12

Horizontal velocity: Constant velocity

v2

v1

Monday, December 3, 12

Horizontal velocity: Wavefront in media

v2

v1

Monday, December 3, 12

Horizontal velocity: Wavefront in media

v2

v1

Monday, December 3, 12

Horizontal velocity: Interface

v2

v1

Monday, December 3, 12

Horizontal velocity: Reflection and transmission

v2

v1

Monday, December 3, 12

Horizontal velocity: Reflection and transmission

v2

v1

Monday, December 3, 12

Horizontal velocity: Reflection & transmission wavefronts

v2

v1

Monday, December 3, 12

Horizontal velocity: Reflection & transmission wavefronts

v2

v1

Monday, December 3, 12

Horizontal velocity: Reflection & transmission wavefronts

v2

v1

Monday, December 3, 12

Horizontal velocity: Reflection & transmission wavefronts

v2

v1

Monday, December 3, 12

Horizontal velocity: Reflection & transmission wavefronts

v2

v1

Monday, December 3, 12

Stepout doesn’t change in v(z) media

v2

v1

@t0

@x

Monday, December 3, 12

Phase velocity

@t0

@x

=sin ✓

v

@t0@z

=

cos ✓

v

Horizontal phase velocity

Vertical phase velocity

Snell wave

Monday, December 3, 12

Phase velocity

@t0@z

=

cos ✓

v

p=Snell parameter, observable with surface measurements

Vertical phase velocity

Snell wave

@t0

@x

=sin ✓

v

= p

Monday, December 3, 12

A little math for later@t0

@x

=

sin ✓

v

= p

@t0

@z

=

cos ✓

v

=

s1

v(z)

2� p

2

t0(x, z) =

sin ✓

v

x +

Z z

0

cos ✓

v

dz

t0(x, z) = p x +

Z z

0

s1

v(z)

2� p

2dz

Monday, December 3, 12

Velocity

v2

v1 Velocity can be described in turns

of v(z) or v’(p,t)

Monday, December 3, 12

Velocity

v2

v1 Velocity can be described in turns

of v(z) or v’(p,t)

v̂ =

rx

t

dx

dt

Monday, December 3, 12

RMS Velocity

v2

v1

x(p, t) =

Z t

0v

0(p, t) sin ✓(p, t) dt = p

Z t

0v

0(p, t)2 dt

v̂ =

rx

t

dx

dt

vRMS =

s1

t

Z t

0v0(p, t)2 dt

Monday, December 3, 12

RMS Velocity

v2

v1

x(p, t) =Z t

0v0(p, t) sin✓(p, t) dt

Monday, December 3, 12

RMS Velocity

v2

v1

x(p, t) =Z t

0v0(p, t) sin✓(p, t) dt

sin✓p=v

Monday, December 3, 12

RMS Velocity

v2

v1

x(p, t) =Z t

0v0(p, t) sin✓(p, t) dtsin✓

p v

Monday, December 3, 12

RMS Velocity

v2

v1

x(p, t) =Z t

0dtp v0(p, t)2

dx

dtp=

v = dx

dtx

t

Monday, December 3, 12

RMS Velocity

v2

v1

x(p, t) =Z t

0dtp v0(p, t)2

pv = x

t1

Monday, December 3, 12

RMS Velocity

v2

v1

x(p, t) =Z t

0dtp v0(p, t)2

pv = x

t1

vRMS =

s1

t

Z t

0v0(p, t)2dt

Monday, December 3, 12

RMS Velocity

v2

v1

x(p, t) =Z t

0dtp v0(p, t)2

pv = x

t1

Monday, December 3, 12

True vs estimated wavefront

Monday, December 3, 12

NMO Correction

Monday, December 3, 12

Vrms discrete form

vRMS =

s1

t

Z t

0v0(p, t)2 dt

V (it) = vRMS(it) =

vuut 1

it ⇤�⌧

itX

0

v(it)2�⌧

Monday, December 3, 12

Interval from RMSV 2(1) = v2(1)

2V 2(2) = v2(1) + v2(2)

3V 2(3) = v2(1)v2(2) + v2(3)

Monday, December 3, 12

Interval from RMS

3V 2(3) = 2V 2(2) + v2(3)

v2(3) = 3V 2(3)� 2V 2(2)

V 2(1) = v2(1)

2V 2(2) = v2(1) + v2(2)

3V 2(3) = v2(1) + v2(2) + v2(3)

Monday, December 3, 12

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