Environmental Engineering Reference
In-Depth Information
5.1 Solar Energy Harvesting (SEH) System
Several mathematical models exist in the literature [130-132] that describe the
operation of photovoltaic (PV) cells, from simple to more complex models that
account for different reverse saturation currents. In this chapter, an electrical
circuit with a single diode (single exponential) is considered as the equivalent
PV model, which consists of
n
s
number of PV cells in series, as shown in
the current-voltage (I-V) characteristic of the PV module can be described
with a single diode as the four-parameter model given by
Equation 5.1
[130],
I
o
exp
V
pv
1
+
I
pv
R
s
n
s
V
t
=
−
−
I
pv
I
L
(5.1)
where
I
L
is the light-generated current (A) and
I
o
is the dark/reverse satura-
tion current of the p-n diodes (1
10
−
9
A).
R
s
is the series resistance of the
PV module, and
V
t
is the junction terminal thermal voltage (V) depending on
the cell absolute temperature, which is defined as
×
kT
c
q
V
t
=
(5.2)
where
T
c
is the cell absolute temperature (K),
k
is the Boltzmann constant
(1.3807
10
−
19
C).
The ultimate goal is to determine whether the power harvested by the PV
module is able to power the wireless sensor node; hence, it is crucial to es-
timate the electrical power throughput of the PV module by leveraging on
the relationship between the current and voltage of the PV module expressed
by
Equation 5.1
. Referring to
Equation 5.1
, it can be deduced that the voltage
drop across the series resistance,
V
Rs
10
−
23
JK
−
1
), and
q
is the charge of the electron (1.6022
×
×
I
pv
R
s
,iscomparably much lower than
the output PV voltage
V
pv
due to the very low PV current
I
pv
on the order of
microamperes flowing through the small series resistance
R
s
of a few ohms;
=
I
pv
R
s
I
L
I
D
I
sh
V
pv
R
sh
FIGURE 5.1
Equivalent electrical circuit for a photovoltaic module.
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