sp k1,k(Tw)w
k ) 1, 2 (12)
Conse rvation of Ene rgy of the Channe l Gas。 The following term s ar e tak en into account : convective heat exchan ge with th e chann el wall an d th e entha lpy flowing into or from th e elementar y contr ol volum e thr ough th e filter wall。 For th e inlet chann el, th e gas leaves th e contr ol volum e at temperatur e T1:
exp - Rk
vw
Ene rgy Ba lance in the Wall。 The energy balance equat ion for th e wall should tak e into account th e contr ibut ion of convective heat tran sfer from th e chan - nel flow an d from th e flow thr ough th e wall, th e heat
2 2 released by exoth erm ic soot combustion, an d th e con-
Cp,g[D F1v1 T1|z+∆z - D F1v1 T1|z + 4D∆zFwvw T1|z] )
h14D∆z(Tw - T1) (7)
ductive heat tran sfer along th e chann el wall:
∂ (F wC
T +F w C
T ) ) h (T
- T ) +
On th e oth er han d, for th e outlet chann el, th e gas ent ers
∂t p
p,p w
s s p,s w
1 1 w
th e contr ol volum e at temperatur e Tw:
h2(T2 - Tw) + FwvwCp,g(T1 - Tw) + H react + Hcond
(13)
2 2
Cp,g[D F2v2 T2|z+∆z - D F2v2 T2|z - 4D∆zFwvw Tw|z] )
h24D∆z(Tw - T2) (8)
Mass Ba lance for the Deposit Laye r。 Ass um ing
From th e equat ion for th e consum ption rat e of th e deposit (eq 12), th e heat released by th e overall reaction exp ressed per un it time is comput ed:
that both reactions (1) an d (2) ar e first order in th e oxidant s (O2 an d NO2, respe ctively) an d that diffu sion is negligible compar ed to convection, th e oxidant s bal-
2
H react ) -
k)1
∆Hk
Mk
1
Fwvwy
Rk
1 - exp-
sp k1(Tw)w
vw
ance equat ion in th e exhau st gas is
∂
∂x(Fgvyk) ) -sjkj,kFgykRk j ) 1, 2 an d k ) 1, 2 (9)
where th e subscript j ident ifies regions 1 (deposit) an d 2 (porous wall) an d th e subscript k identifies th e gaseous
k ) 1, 2 (14)
∆Hk indicat es a combined reaction entha lpy res ulting from th e complete an d incomplete oxidat ion of car bon in th e two cases of soot-O2 an d soot-NO2 reactions, which is linked to R according to th e relat ions
reactant s of th e reactions (1) an d (2) (O2 an d NO2, respe ctively)。 Becau se th ere is no reaction in th e porous
∆H1 ) 2(R1 - 0。5)∆HCO
+ 2(1 - R1)∆HCO (15)
wall, k2 ) 0。 The coefficie nt k1 for th e deposit is assum ed to be an Arrh enius-type function of temperatur e, an d th e following rat e exp ression is used for th ese reactions:
∆H2 ) (1 - R2)∆HCO
+ (R2 - 0。5)∆HCO - R2∆H NO
(16)
k1,k
) k T e-Ek/RT (10)
The contr ibut ion of heat conduction is
As far as th e reaction with O2 is concern ed, th e values of th e kinetic rat e param eters can be tak en from previous expe rience (Table 5)。25 Any minor ina ccura cies
Hcond ) -λp
∂ w 柴油机碳烟氧化英文文献和中文翻译(11):http://www.youerw.com/fanyi/lunwen_99285.html