understanding moisture ingress rates in pv...
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NREL is a national laboratory of the U.S. Department of Energy, Office of Energy Efficiency and Renewable Energy, operated by the Alliance for Sustainable Energy, LLC.
Understanding Moisture Ingress Rates in PV Modules
Barrier Technologies Workshop
Michael Kempe
September 19, 2012
2
Introduction
• Many electronic devices are sensitive to moisture (e.g. OLEDs, OPV, CIGS, CdTe).
• For some applications we would like to have a transparent flexible moisture barrier material. o Ease of application.
o Weight limits for some structures.
o Here I will explain the theory behind why such low permeation is necessary and how to prevent moisture ingress.
3
Outline
• Permeation through barrier films. 25 y requirements.
• Diffusion from the module edges.
• Edge seals
4
How Does WVTR Relate to Total Permeation?
This depicts how much water would get in if it was consumed immediately.
0.01
0.1
1
10
100
1000
10000
100000
1000000
1.00E-061.00E-051.00E-041.00E-031.00E-021.00E-011.00E+001.00E+011.00E+02
Wat
er
Laye
r Th
ickn
ess
(µ
m)
WVTR (g/m2/day)
Water Thickness Permeated in 25 y
10-6 10-5 10-4 10-3 10-2 10-1 100 101 102
Thin Film LayerThicknesses
WVTR
PET(0.10 mm)
PCTFE(0.023 mm)
PDMS(1 mm)
PEN(0.10 mm)
5
Moisture in Breathable Front-Sheets
Moisture Permation Assumptions:
(1) CEVA not a function of position X (i.e. DEVA>>DB)
(2) WVTR is proportional to DCB=C(0)-C(lB)
BBB
EVASatE
SatBEVA lCClC
WVTR
dt
dC 0
.,
,
H2O
PV Device
Barrier Film
Encapsulant
Dielectric films Metal Foil film
6
Time Constant for Water Ingress
ingressmoistureofRate
holdcanEVAwaterofAmout
WVTR
lC
SatB
EVAEVASat693.0693.0
,
,
21
H2O
PV Device
Barrier Film
Encapsulant
Dielectric films Metal Foil film
EVAEVASat
Sat
lC
tWVTR
o eCtC ,1 BBB
EVASatE
SatBEVA lCClC
WVTR
dt
dC 0
.,
,
7
Time Constant for Water Ingress
lEVA =0.46 mm, T=27 oC, CSat,EVA=0.0022 g/cm3
lPET=0.10 mm, lPEN=0.10 mm, lPCTFE=0.022 mm
PET PEN PCTFE
1/2 = 0.22 0.91 5.5 (day)
For 1/2=25 years need 0.8·10-4 g/m2/day
At 1·10-3 g/m2/day, the encapsulant will have a half
time of 1.9 y. This short time frame is insignificant
compared to a 25 y warranty.
SatB
EVAEVASat
WVTR
lC
,
,
21 693.0
8
Encapsulant Materials Structures
Si O
CH3
CH3
n
n
O
O
mn m
O O (Na, Zn)
RN
O
O
H n
OO HO OO
n m o
Ionomer
Thermoplastic Polyurethane (TPU)
Polyvinyl Butyral (PVB)
Ethylene Vinyl Acetate (EVA)
Polydimethylsiloxane (PDMS)
R
n m
R= -CH3 ,-(CH2)nCH3, others or multiple "R" groups.
Thermoplastic Polyolefin (TPO)
M. Kempe, “Overview of Scientific Issues Involved in Selection of Polymers for PV Applications”, 37th IEEE PVSC (2011).
SatB
EESat
WVTR
lC
,
,
21 693.0
9
Significantly More Adsorbent Polymers Exist
A 10X more water adsorbent polymer may reduce the barrier requirements by a factor of 10.
0 0.2 0.4 0.6 0.8 1
0
0.2
0.4
0.6
0.8
1
1.2
0.0%
0.0%
0.1%
1.0%
10.0%
0.0027 0.0029 0.0031 0.0033 0.0035 0.0037
Temperature (⁰C)
Solu
bil
ity (
g/c
m3)
1/Temperature (1/K)
PVB #1
PVB #2
TPU #2
TPU #1
Ionomer #1
EVA
Ionomer #2
PDMS
TPO #2
Poly-α-Olefin #1
Poly-α-Olefin #2
10%
1%
0.1%
0.01%
0.001%
97.2 71.7 49.4 29.9 12.6 -2.89
10
EVA Allows Significant Moisture Ingress From Edges
0.0000
0.0005
0.0010
0.0015
0.0020
0.0025
0 5 10 15 20
Distance X from edge (cm)
Dis
solv
ed
Wate
r (g
/cm
3) 1.109360481
2.109129888
3.110725775
4.114604761
5.114374168
6.114143575
7.113912982
8.113682389
9.113451796
10.1132212
12.11276002
12.4166406
EVA Glass
Glass
H2O
X=0 X=20
H2O
Jan
Feb
Mar
Apr
May
Jun
Jul
Aug
Sep
Oct
Nov
Dec
Increasing
Months
Jan
Feb
Mar
Apr
May
Jun
Jul
Aug
Sep
Oct
Nov
Dec
Finite element analysis using meteorological data from Miami Florida 2001
11
Alternative Encapsulants Slow Down Moisture Ingress
0 0.2 0.4 0.6 0.8 1
0
0.2
0.4
0.6
0.8
1
1.2
1.0E-10
1.0E-09
1.0E-08
1.0E-07
1.0E-06
1.0E-05
1.0E-04
0.0027 0.0029 0.0031 0.0033 0.0035 0.0037
Temperature (⁰C)
Dif
fusi
vit
y (
cm2/s
)
1/Temperature (1/K)
PDMS #1
Poly-α-Olefin #1
Poly-α-Olefin #2
EVA
TPO #2
TPU #1
TPU #2
PVB
PVB #2
Ionomer #2
Ionomer #1
97.2 71.7 49.4 29.9 12.6 -2.89
10-4
10-5
10-6
10-7
10-8
10-9
10-10
Lower diffusivity can reduce ingress rates from the side by two orders of magnitude.
12
Determining Moisture Ingress Distance From Edges
M.D. Kempe, A. A. Dameron, M.O. Reese, to be submitted to Progress in Photovoltaics (2012)
PDMS EVA TPO Ionomer #1 PDMS EVA TPO Ionomer #1Munich, Germany 19.5 23.3 28.3 29.2 30.3 38.2 47.7 49.2Denver, Colorado 25.8 30.1 35.3 36.2 40.2 48.4 56.7 57.9Miami, Florida 33.8 35.6 37.9 38.3 44.4 48.9 54.3 55.2Albuquerque, New Mexico 30.6 34.6 39.4 40.1 46.4 54.0 61.3 62.4Bangkok, Thialand 38.0 39.7 42.0 42.4 48.9 53.4 58.9 59.8Phoenix, Arizona 40.6 40.6 48.7 44.3 56.6 63.8 71.1 72.1Riyadh, Saudi Arabia 42.3 45.8 50.1 50.8 58.0 65.0 72.2 73.3
Rack Mounted Insulated Back
Diffusivity Weighted Average Module Temperature
Effective Temperature (⁰C)
1
10
100
1,000
0.0027 0.0029 0.0031 0.0033 0.0035
Wid
th o
f ed
ge
se
al
(cm
)
1/K
25 year 5% Breakthrough Width
PDMS
Poly-α-olefin
EVA
TPO
TPU #1
TPU #2
PVB #1
PVB #2
Ionomer #2
Ionomer #185⁰C 60⁰C 20⁰C
Distance from edge which after 25 years will be at 5% of the equilibrium concentration.
EaPDMS=27 kJ/mol EaEVA=38 kJ/mol EaTPO=53 kJ/mol
EaIonomer#1=56 kJ/mol
13
Test Sample Designed to Mimic Module Edge
Seal Encapsulant
Glass
Glass
H2O
w
50 mmGlass (3.18 mm)Polymer Film (~0.5 mm)Ca (100 nm)Glass (3.18 mm)
H2O
Ca + 2 H20 → Ca(OH)2 + H2
Module Edge Test Sample
n
Polyisobutylene
Desiccant (e.g. CaO or molecular sieves,
Preferably type 3A Molecular Steve that does not absorb O2 and N2)
Edge Seals +
14
Oxidation of Ca Indicates Moisture Ingress
Ca + 2 H20 → Ca(OH)2 + H2
Mirror-Like → Transparent
H2O
H2O
50 mm
Unexposed 1500 h, 85⁰C, 85% RH
15
Moisture Ingress Rate Governed by Diffusion
15
H2O
H2O
Moisture ingress measured at 45ºC and 85ºC, with RH held at 85%, and at lower levels using saturated salt solutions of LiCl, MgCl, or NaNO3.
45 85
(⁰C) (⁰C)
NaNO₃ 67% 59%
MgCl 31% 25%
LiCl 11% 10%
RH (%)
16
Edge Seal Modeling
%100
%RHeSS kT
Ea
om
s
kT
Ea
oeff
D
eDD
Mobile phase water absorption is split between the
polymer matrix and the mineral components.
Assume linearity with relative humidity.
Mobile phase water diffusivity is an effective diffusivity.
This accounts for a rapid equilibration between adsorbed
and dissolved water.
A non-reversible
reaction with water
that immobilizes the
water. OHR
2
0
0.002
0.004
0.006
0.008
0.01
0.012
0.014
0.016
0.018
0 20 40 60 80 100
K (
cm/h
1/2
)
% RH
85⁰C
45⁰C
PIB #2
Values for the 5 constants were found from absorption measurements and a fit to the data.
17
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0 2 4 6 8 10
Ingr
ess
De
pth
(cm
)
Time (Years)
Denver Colorado, PIB #2
Insulated Back, Glass/Polymer
Close Roof, Glass/Glass
Open Rack, glass/glass
Open Rack, Glass/Polymer
Square Root Relation Works to Longer Times
Denver Colorado
Used TMY3 Data and Temperature estimate methods from to King et al.
tKX
18
Results for Different Climates
Glass/Polymer Modules.
A sensitivity analysis gave about ±15% on K and Width, and ±30% on 25 yr equivalent time.
0.33
47
0.16
5
0.047 (cm/h1/2) (cm) (h)
0.00087 0.45 1,100
0.00103 0.47 1,300
0.00096 0.50 1,400
0.00107 0.51 1,500
0.00102 0.50 1,400
0.00124 0.53 1,600
0.00128 0.60 2,000
0.00153 0.63 2,300
0.00199 0.90 4,700
0.00225 0.95 5,200
0.00228 1.02 6,000
0.00258 1.07 6,700
Miami, FlordiaOpen Rack
Insulated Back
Open RackBangkok, Thailand
Insulated Back
Riyadh, Saudi ArabiaOpen Rack
Insulated Back
Open RackPhoenix, Arizona
Insulated Back
Denver, ColoradoOpen Rack
Open Rack
Insulated Back
Munich, GermanyInsulated Back
Do (cm2/s)=
Modeled K Modeled 25 y
required width
Modeled 25 y
equivalent time
at 85⁰C/85% RH
EaD (kJ/mol)=
So (g/cm3)=
EaS (kJ/mol)=
Reactive Ca absorption (g/cm3)=
19
What edge seal parameters are important?
M. D. Kempe, A. A. Dameron, T. J. Moricone, M.O. Reese, “Evaluation and Modeling of Edge-Seal Materials for Photovoltaic Appilcations, 35th IEEE PVSC, Honolulu, HI (2010).
1. Adhesion is the most important parameter. a) Must be maintained after environmental exposure.
b) Residual stress in glass will affect adhesion.
c) Material may expand as it absorbs water.
d) Good surface preparation is necessary.
2. Breakthrough time is the next most important. a) The 12 mm edge delete perimeter should be wide enough to keep
moisture out.
3. Module mounting configuration is not important. a) Hotter installations tend to dry out the module partially countering the
effects of increased diffusivity.
4. The steady state transmission is less important. a) The amount of permeate is very low.
b) Ideally one will not reach steady state.
20
Conclusions
• An ingress half time of 25 years is needed. For typical barriers and encapsulants, a WVTR of less than 0.8·10-4 g/m2/day or better is needed.
• High solubility encapsulants may decrease the barrier needs to as low as 1·10-3 g/m2/day or better.
• With impermeable front and backsheets, very low diffusivity polymers can limit moisture ingress to a few cm from the edges.
• A PIB based edge seal width of 1 cm should be able to prevent moisture ingress.
21
Acknowledgements
Sarah Kurtz John Wohlgemuth
David Miller Joshua Martin
Arrelaine Dameron Matthew Reese Tom Morricone
Dhananjay Panchagade
This work was supported by the U.S. Department of Energy under Contract No. DE-AC36-08-GO28308 with the National Renewable Energy Laboratory.