Page 109 - Introduction to Transfer Phenomena in PEM Fuel Cells
P. 109
98 Introduction to Transfer Phenomena in PEM Fuel Cells
– at the cathode:
- the gas mixture is ternary, the species involved are oxygen, nitrogen
and water vapor; the equation system to solve is written as:
c
x O 2 + x N 2 + x = 1
HO
2
N c
dx N 1 N O H O
2 =⋅ 2 + 2 x ⋅ N [3.32]
dx c D eff D eff 2
O,N 2 H O,N 2
2
2
c
dx O 1 N O 2 + N H O 1 1 N O
2 =⋅ eff 2 x ⋅ O 2 + eff − eff ⋅ N O 2 x ⋅ N 2 − eff 2
dx c D D D D O,H O
O,H O O,H O O,N 2 2 2
2
2
2
2
2
- at the diffuser inlet, the relative humidities (RH) are expressed as
follows:
p
x ce = HR ⋅ sat
c
2
HO p
p
−
x e O 2 = 0,21 1 HR ⋅ sat [3.33]
c
p
p
x e = 0,79 1 HR ⋅ sat
−
N 2 c p
3.4.3. Some parametric laws
3.4.3.1. Saturation pressure
Different formulas have been proposed for determining the saturation
pressure of water (in [Pa]). Wöhr presented, in his work, the following
empirical formula [MON 06]:
A− B
P sat () 10= C T 273 +− ⋅ 100 [3.34]
T
In this relation, the temperature is in Kelvin, and the coefficients have the
following values: A = 8.073; B = 1 656.39; C = 226.86 in K. Chun-Ying
Hsu et al. [WÖH 00] used another formula where the decimal logarithm of