tugas rumus-rumus rlt
TRANSCRIPT
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4.5.1. Estimation of gas emission into development excavationsA. Bozko method
V CH 4
=αwdlW
0γ
43200
Where:V CH
4 = methane emission, m3/minute
α = factor depending upon the excavation development for a
single excavation, α = !, for t"o headings, α = ! # $/l
%&4' "here $ = length of cut(throughl = depth of fracture $one %) m'
d = thic*ness of seam, m
w = rate of advance, m/month
W 0 = methane content of seam, m3/t
γ = densit+ of coal %1.4 ton/m3'
B. Oriechowa methodV CH
4
=25αdwV P ć k w
Where:
V CH 4 = methane emission, m3/minuteα = ! for a single road"a+,
= ! # .5l1 %&4' for t"o road"a+s "here l1 = distance
-et"een parallel road"a+s, m
d = thic*ness of seam, m
w = rate of advance, m/da+
V P = uantit+ of gas li-erated from a unit surface area of the
exposed
road"a+, m3/minute/m! %determine experimentall+'
ć = coecient de0ning the increase in gas emission determined
-+ the
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relationship ć = .!4 ln %1.5!t # 1' 2 .1t, "here t = time,
month
k w = constant given -+ the euation k w=V CH
4+V CH
4max
V CH 4
C. Barbara experimental mine methodd w
∑ ¿ γ (W 0−W k )¿
wb¿V
1CH 4
=¿
dw
∑ ¿V P¿
V 2CH 4
=b¿
dw
30k +n' 0.5
t −1
¿
∑ ¿w V P¿V
3CH 4
=n¿
nd the total gas emitted isV t CH
4
=V 1CH
4
+V 2CH
4
+V 3CH
4
Where:
dw = total thic*ness of the coal -ed exposed
b = "idth of the excavation, m
γ = densit+ of coal, ton/m3
V P = gas li-erated from a unit area of exposed surface
%m3/minute/m!'n = num-er of surfaces in a road"a+ %for full thic*ness
excavation n=!'W
0 = gas content of the coal, m3/t
W k = rest gas, m3/t
k = permea-ilit+
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n ' = seuential num-er of the da+ after the start of drivae of the
excavation.t = time of drivage of excavation, months %t = n/3'
D. Pawinski method
V CH 4
=2dw(√ mk μπ ρa )( pa
2− p0
2
p0
)t 0.5Where:
d = thic*ness of seam, m
w = rate of advance, m/s
Pa = in(situ gas pressure in the seam, 15 a
Pv = air pressure in the excavation, 15 a
m = porosit+
µ = viscosit+ of methane, 6s/m!
k = permea-ilit+
t = time elapsed after start of driving the heanding, s.E. Experimental techniques
V CH 4
= A t α
and if a heading has -een stopped, gas emission is given -+
V CH 4= A t α − A (t − Lw )
α
Where:
V CH
4 = volume of gas emitted, m3/minute
t = time elapsed, da+s
α and = constants for a given area and depend upon local
conditions
w = rate of advance, m/da+, and
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L = length of the heading.
7f o-servations are made over a period of time for gas emission from
a heading advancing at a 0xed rate, then the value of α can -e
calculated from the relationship
α =
lnV
2
V 1
lnt 2
t 1
8he value of can -e calculated from the relationship
A=V t
α
8he euations can modi0ed as follo"s:
α =
ln( V i−V 0V n−V 0 )ln( t it n )