84
In the photon element, the I–V equation joins the I–V curves of every cell in the
photonic radiation panel. The V–R correlation at the section is governed by
V
IR K
I I I
I
= −
+
− +
S
L
o
o
log
,
(5.4)
where V mo and I mo are the voltage and current in the PV panel, respectively, and K is
a constant AkT q
/
(
) . Consequently, the link between I mo and V mo is the same as the
I–V correlation in the PV cell:
V
I R
K
I
I
I
I
mo
mo Smo
m o
Lmo
m o
o mo
omo
= −
+
−
+
log
,
(5.5)
whereby R Smo is the series resistance, I omo symbolizes the induced current into the
diode, I Lmo symbolizes the photon-produced current, and K mo is a constant. Once the
resistances of all non-series (Ns) cells are arranged in series, the constant is
Fig. 5.2 I–V feathers of a single-diode cooling state: (a) Curtain wall at the indirect and direct
photon gap state. (b) Curtain wall under energy mode. (c) Current density formation in the curtain
wall by helium (He)-aided point breaks
5 Integrated Building Design Technology
In the photon element, the I–V equation joins the I–V curves of every cell in the
photonic radiation panel. The V–R correlation at the section is governed by
V
IR K
I I I
I
= −
+
− +
S
L
o
o
log
,
(5.4)
where V mo and I mo are the voltage and current in the PV panel, respectively, and K is
a constant AkT q
/
(
) . Consequently, the link between I mo and V mo is the same as the
I–V correlation in the PV cell:
V
I R
K
I
I
I
I
mo
mo Smo
m o
Lmo
m o
o mo
omo
= −
+
−
+
log
,
(5.5)
whereby R Smo is the series resistance, I omo symbolizes the induced current into the
diode, I Lmo symbolizes the photon-produced current, and K mo is a constant. Once the
resistances of all non-series (Ns) cells are arranged in series, the constant is
Fig. 5.2 I–V feathers of a single-diode cooling state: (a) Curtain wall at the indirect and direct
photon gap state. (b) Curtain wall under energy mode. (c) Current density formation in the curtain
wall by helium (He)-aided point breaks
5 Integrated Building Design Technology