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Презентация на тему Basic well logging analysis – sonic log

Sonic LogThe sonic log is a porosity log that measures interval transit time (Δt) of a compressional sound wave traveling through one foot of formation. Interval transit time (Δt) in microseconds per foot is the reciprocal
Basic well Logging Analysis –   Sonic Log Hsieh, Bieng-ZihFall 2009 Sonic LogThe sonic log is a porosity log that measures interval transit Sonic Log (Cont.)The sonic log device consists of one or more sound Sonic Log聲波井測為量測聲波(通常為壓縮聲波)通過 1英呎厚的地層所需的間隔傳遞時間。利用聲波井測所記錄的間隔傳遞時間、配合已知(或假設)的地層岩基以及地層流體的間隔傳遞時間,可估算出地層孔隙率 (聲波孔隙率)。 Sonic Log (Cont.)Interval transit time (Δt) is record in tracks #2 and sonic porosity Sonic Log (Cont.)The interval transit time (Δt) is dependent upon both lithology (Table-1)  matrix velocity (1) derive sonic porosity by chart 63 μsec/ft Given:Vma=26000 ft/sec (Dolomite)Δt=63 μsec/ft @ 9310 ftNote: The formation's matrix velocity must Exercise – find sonic porosity by chart(1)Depth = 9310 ftLithology [=] Dolomite (2) derive sonic porosity by formula Derive sonic porosity by Wyllie formula Where: Фsonic = sonic derived porosity Exercise – find sonic porosity by formula(1)Depth = 9310 ftLithology [=] Dolomite Sonic porosity for unconsolidated sands Sonic porosity for unconsolidated sands The Wyllie et al. (1958) formula for Sonic porosity for unconsolidated sands (Cont.)For unconsolidated sands,The compaction factor is obtained empirical corrections for hydrocarbon effect empirical corrections for hydrocarbon effectThe interval transit tie (Δt) of a formation Sonic porosity for shaly sands Sonic porosity for shaly sandsAfter the volume of shale (Vsh) is determined, Homework #3 -- sonic log Homework #3 – sonic log BHC Homework #3 – sonic log Information:Δtma = 55.5 μsec/ft (Sandstone)Δtf = 189
Слайды презентации

Слайд 2 Sonic Log
The sonic log is a porosity log

Sonic LogThe sonic log is a porosity log that measures interval

that measures interval transit time (Δt) of a compressional

sound wave traveling through one foot of formation.

Interval transit time (Δt) in microseconds per foot is the reciprocal of the velocity of a compressional sound wave in feet per second.


Слайд 3 Sonic Log (Cont.)
The sonic log device consists of

Sonic Log (Cont.)The sonic log device consists of one or more

one or more sound transmitters, and two or more

receivers.

Modern sonic logs are borehole compensated devices (BHC). These devices greatly reduce the spurious effects (假性效應) of borehole size variations (Kobesh and Blizard, 1959), as well as errors due to tilt (傾斜) of the sonic tool (Schlumberger, 1972).


Слайд 4 Sonic Log
聲波井測為量測聲波(通常為壓縮聲波)通過 1英呎厚的地層所需的間隔傳遞時間。

利用聲波井測所記錄的間隔傳遞時間、配合已知(或假設)的地層岩基以及地層流體的間隔傳遞時間,可估算出地層孔隙率 (聲波孔隙率)。

Sonic Log聲波井測為量測聲波(通常為壓縮聲波)通過 1英呎厚的地層所需的間隔傳遞時間。利用聲波井測所記錄的間隔傳遞時間、配合已知(或假設)的地層岩基以及地層流體的間隔傳遞時間,可估算出地層孔隙率 (聲波孔隙率)。

Слайд 6 Sonic Log (Cont.)
Interval transit time (Δt) is record

Sonic Log (Cont.)Interval transit time (Δt) is record in tracks #2

in tracks #2 and #3 (in your example Figure).



A sonic derived porosity curve is sometimes recorded in tracks #2 and #3, along with the Δt curve.

Track #1 normally contains a caliper log and a gamma ray log or an SP log.

Слайд 7 sonic porosity

sonic porosity

Слайд 8 Sonic Log (Cont.)
The interval transit time (Δt) is

Sonic Log (Cont.)The interval transit time (Δt) is dependent upon both

dependent upon both lithology and porosity.

Therefore, a formation's

matrix velocity (Table 1) must be known to derive sonic porosity either by chart (Fig. 27) or by formula (Wyllie et al, 1958).

Слайд 9 (Table-1) matrix velocity

(Table-1) matrix velocity

Δtma   
Vma Δtma (μsec/ft)
(ft/sec) (μsec/ft) commonly used
Sandstone 18,000 to 19,500 55.5 to 51.0 55.5 to 51.0
Limestone 21,000 to 23,000 47.6 to 43.5 47.6
Dolomite 23,000 to 26,000 43.5 to 38.5 43.5
Anhydrite 20,000 50.0 50.0
Salt 15,000 66.7 67.0
Casing
(Iron) 17,500 57.0 57.0

Слайд 10 (1) derive sonic porosity by chart

(1) derive sonic porosity by chart

Слайд 11 63 μsec/ft

63 μsec/ft

Слайд 12 Given:
Vma=26000 ft/sec (Dolomite)
Δt=63 μsec/ft @ 9310 ft
Note:
The

Given:Vma=26000 ft/sec (Dolomite)Δt=63 μsec/ft @ 9310 ftNote: The formation's matrix velocity

formation's matrix velocity must be known
Derive sonic porosity by

chart

Слайд 13 Exercise – find sonic porosity by chart
(1)
Depth =

Exercise – find sonic porosity by chart(1)Depth = 9310 ftLithology [=]

9310 ft
Lithology [=] Dolomite (Vma=26000 ft/sec)
Sonic porosity =

?

(2)
Depth = 9320 ft
Lithology [=] Limestone (Vma=21000 ft/sec)
Sonic porosity = ?

Слайд 14 (2) derive sonic porosity by formula

(2) derive sonic porosity by formula

Слайд 15 Derive sonic porosity by Wyllie formula




Where:
Фsonic

Derive sonic porosity by Wyllie formula Where: Фsonic = sonic derived

= sonic derived porosity
Δtma = interval transit time

of the matrix
Δtlog = interval transit time of formation
Δtf = interval transit time of the fluid in the well bore
(fresh mud = 189;salt mud = 185)

Слайд 16 Exercise – find sonic porosity by formula
(1)
Depth =

Exercise – find sonic porosity by formula(1)Depth = 9310 ftLithology [=]

9310 ft
Lithology [=] Dolomite
Mud [=] fresh mud
Sonic porosity

= ?

(2)
Depth = 9320 ft
Lithology [=] Limestone
Mud [=] fresh mud
Sonic porosity = ?



Слайд 17 Sonic porosity for unconsolidated sands

Sonic porosity for unconsolidated sands

Слайд 18 Sonic porosity for unconsolidated sands
The Wyllie et

Sonic porosity for unconsolidated sands The Wyllie et al. (1958) formula

al. (1958) formula for calculating sonic porosity can be

used to determine porosity in consolidated sandstones and carbonates.

Where a sonic log is used to determine porosity in unconsolidated sands, an empirical compaction factor or Cp should be added to the Wyllie et al. (1958) equation:



Where Cp = compaction factor

Слайд 19 Sonic porosity for unconsolidated sands (Cont.)
For unconsolidated sands,




The

Sonic porosity for unconsolidated sands (Cont.)For unconsolidated sands,The compaction factor is

compaction factor is obtained from:



Where Cp = compaction factor

Δtsh = interval transit time for adjacent shale
C = a constant which is normally 1.0 (Hilchie,1978)



Слайд 20 empirical corrections for hydrocarbon effect

empirical corrections for hydrocarbon effect

Слайд 21 empirical corrections for hydrocarbon effect
The interval transit tie

empirical corrections for hydrocarbon effectThe interval transit tie (Δt) of a

(Δt) of a formation is increased due to the

presence of hydrocarbons (i.e. hydrocarbon effect).

If the effect of hydrocarbons is not corrected, the sonic derived porosity will be too high.

Hilchie (1978) suggests the following empirical corrections for hydrocarbon effect:
Ф = Фsonic × 0.7 (gas)
Ф = Фsonic × 0.9 (oil)


Слайд 22 Sonic porosity for shaly sands

Sonic porosity for shaly sands

Слайд 23 Sonic porosity for shaly sands
After the volume of

Sonic porosity for shaly sandsAfter the volume of shale (Vsh) is

shale (Vsh) is determined, it can be used to

correct the porosity log for shale effect. The formula for correcting the sonic log for volume of shale is (Dresser Atlas, 1979):



Where Δtsh = interval transit time for adjacent shale

Слайд 24 Homework #3 -- sonic log

Homework #3 -- sonic log

Слайд 25 Homework #3 – sonic log
BHC

Homework #3 – sonic log BHC

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