
124 Industrial Air Quality and Ventilation
© 2010 Taylor & Francis Group, LLC
Taking into account Equation 3.256, we obtain the second boundary condition:
=
P
x
k
v
m
βψρ
12
1
2
, (3.258)
which can be written as follows (keeping Equation 3.239 and 3.249 in mind) after
some transformations:
∂
=
⋅+
=
x
l
n
n
l
n
l
xl
l
2
2
2
1
cossin
π
ππ
l
n
n
l
n
l
l
1
1
1
sincos
π
(3.259)
Thus, we have to solve the following inhomogeneous differential partial equa-
tion with second-order partial derivatives [68] with the initial conditions (Equations
3.251 and 3.254) and the boundary conditions (Equations 3.255 and 3.259)
∂
=
∂
−−⋅
2
2
2
2
1
t
v
x
v
ll
nn