Environmental Engineering Reference
In-Depth Information
For the up-scaling test, 30 kg of charcoal was fed into the bottom of gasi
er and
ignited in order to preheat the gasi
er, and 300 kg of dense-RDF was introduced
into the downdraft gasi
er per batch. To start the gasi
cation process, the air
fl
ow
rate of 75 Nm 3 /h was supplied into the gasi
cation process, the
samples of producer gas were taken for analysis. To optimize the operating con-
dition, the experiment was repeated with the air
er. During the gasi
flow rate of 85 and 101 Nm 3 /h.
To study the feasibility of long-term test run for 200 accumulated operating
hour, 60
fl
100 kg of charcoal was fed into the bottom of gasi
er and ignited in order
-
to preheat the gasi
er; whereas wood chip was also supplied together with dense-
RDF at the different weight ratio of dense-RDF to wood chip of 50:50, 75:25, and
100:0. After all feedstock were put into the gasi
er, the ignition process was
conducted and then air was supplied into the gasi
er at the optimum condition to
promote the gasi
cation process. During the steady state experiment, the producer
gas was taken at the exit of gasi
er for the investigation of producer gas compo-
sition and heating value. The system performance for power production was also
evaluated at the same time. The gasi
cation process was terminated when it was
observed that no producer gas generated. The whole experiment was repeated again
until the operation test run reached 200 h. In the accumulated 200 h test run, the
dual fuel engine-generator test using diesel and producer gas was performed.
2.2.4 Analysis
The composition of producer gas in terms of CO, H 2 ,CO 2 ,CH 4 , and N 2 was
analyzed by gas chromatography (GC) according to the ASTM standard. The
producer gas velocity is measured by the gas
flow meter, and the producer gas yield
at standard condition can be calculated by Eq. 1 , while the heating value of pro-
ducer gas was calculated by Eq. 2 .
fl
Q Producer gas ¼ Q 1 T 2
T 1
ð
1
Þ
;
flow rate of producer gas at the exit condition (m 3 /h), T 1 is
the temperature of producer gas at the gasi
where Q 1 is the volume
fl
er exit (
°
C), and T 2 is the temperature at
standard condition (25
°
C).
LHV Producer gas ¼ R ð X i
LHV i Þ
ð
2
Þ
where LHV producer gas is the producer gas lower heating value (MJ/Nm 3 ), X i
rep-
resents each composition of producer gas yield (Nm 3 /h), and LHV i
is the lower
heating value of each producer gas composition (MJ/Nm 3 ).
The ef
ciency of the gasi
cation process was expressed in term of cold gas
ef
ciency de
ned as the ratio of energy input into the gasi
er to the energy output
from the gasi
er, as given in Eq. 3 .
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