analysis techniques for cell failure

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SOME FAILURE MODES AND ANALYSIS TECHNIQUES FOR TERRESTRIAL SOLAR CELL MODULES * Alex Shumka and Kenneth H. Stem Jet Propulsion Laboratory, California Institute of Technology Pasadena, California ABSTRACT This paper describes the types of failure modes observed in failedfdefective silicon solar cell modules of various types and procured from different manufacturers . This paper also de- scribes analytical techniques that are particular- ly useful diagnostic tools for performing failure analysis. I. INTRODUCTION Within the past few years an increasing em- phasis on photovoltaics as a potential power source for terrestrial application has stimulated rapid advancements in solar cell technology, par- ticularly in the development of silicon solar cell module technology. The practical application of these technologies for large scale power sources will be strongly dependent on such considerations as cost, energy conversion efficiency and long term reliability. Information on long term re- liability is presently limited to field and lab- oratory tests on a relatively small number of various types of modules. Reliability data is yet to be obtained on a large number of modules that are currently in the developmental and/or con- ceptual stage. However, the test data that is currently available is extremely valuable for pre- liminary reliability estimation for existing modules and for indicating problem areas which can then be circumvented through engineering design of future modules. One objective of this paper is to address the re- liability problem by presenting analysis data on failedjdefective silicon solar cell modules of various types and procured from different manufac- turers. The type of failure modes more frequently observed are: internal short and open circuits, output power degradation, and isolation resistance degradation. The cause of failure will be dis- cussed in detail and in many cases will be related to the particular type of technology used in the manufacture of these modules. Wherever applicable, appropriate corrective actions will be recommended. Another objective of this paper is to describe some nar failure analysis techniques that had to be developed because solar cell modules possess unique structurai features. Some of these tech- niques allow for a non-destructive analysis. 11. FAILURE WDES During the past tbo years, failures in solar cell modules have been detected during initial electrical testing, environmental testing and dur- ing field applications. The various types of failuresthat have been observed during the JPL failure analysis of these modules include: open- circuit solar cell interconnects; cracked solar cells; delamination a£ the protective encapsulant ; dielectric breakdown; corrosion and vorkmanship . Many open-circuit solar cell interconnect failures were caused by interconnect fatigue due to in- adequate stress relief. Some of the interconnects were melted open-circuit and the surrounding areas were discolored and charred as a result of arcing across the work hardened and fractured inter- connect. This condition occurred in high voltage field applications and similar failures were created in a JPL laboratory test that simulated the field conditions. Cracked solar cells, in many instances, resulted in open-circuits and/or power degradation of the modules. In addition, many of these solar cells showed evidence of being overheated to the extent that the modules were discolored, burned, charred and the solder had melted and reflowed on the rear side of the solar cell. These solar cells may have been overheated as a result of reverse biasing caused by cell shadowing, cell fracturing or by cell power degra- dation. In some instances, cell fracturing was probably caused by mishandling, environmental stresses or the fractures may not have been de- tected during initial visual inspection. Delamin- ation of the protective encapsulant in many in- stances was caused by physical movement of the solar cell interconnects due to inadequate stress relief and by physical movement of the solar cells due to overheating. In some instances, delamin- ation of the protective encapsulant was caused by environmental effects. Dielectric breakdown, in one instance, was caused by a sharp bent strand of a wire mesh interconnect that had penetrated the insulation material to the metal substrate or frame. In another instance, dielectric breakdown was caused by a cut or break in an insulated cable * This paper presents the results of one phase of research conducted at the Jet Propulsion Laboratory, California Institute of Technology for the Department of Energy, by agreement with the National Aeronautics and Space Administration. Proceedings of the 13th IEEE Photovoltaic Specialists Conference Washington, D.C., June 4-8, 1978, pp. 824-834

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SOME FAILURE MODES AND ANALYSIS TECHNIQUES FOR TERRESTRIAL SOLAR CELL MODULES *

Alex Shumka and Kenneth H. S t e m

Jet Propulsion Laboratory, Cal i fornia I n s t i t u t e of Technology

Pasadena, Cal i fornia

ABSTRACT

This paper describes the types of f a i l u r e modes observed in fa i ledfdefec t ive s i l i con so la r c e l l modules of various types and procured from d i f fe ren t manufacturers . This paper a l so de- sc r ibes ana ly t ica l techniques tha t a r e par t icular- l y useful diagnostic too ls f o r performing f a i l u r e analysis.

I. INTRODUCTION

Within t he pas t few years an increasing em- phasis on photovoltaics a s a po ten t ia l power source f o r t e r r e s t r i a l appl icat ion has stimulated rapid advancements i n so la r c e l l technology, par- t i c u l a r l y in the development of s i l i con so l a r c e l l module technology. The p rac t i ca l appl icat ion of these technologies f o r l a rge sca le power sources w i l l be strongly dependent on such considerations as cos t , energy conversion eff ic iency and long term r e l i a b i l i t y . Information on long term re- l i a b i l i t y is presently limited t o f i e l d and lab- oratory t e s t s on a r e l a t i ve ly s m a l l number of various types of modules. Re l i ab i l i t y data i s yet t o be obtained on a l a rge number of modules t ha t a r e current ly in the developmental and/or con- ceptual stage. However, t he t e s t data t h a t is current ly avai lable i s extremely valuable fo r pre- liminary reliability estimation fo r ex is t ing modules and fo r indicat ing problem areas which can then be circumvented through engineering design of fu ture modules.

One object ive of t h i s paper is t o address t he re- l i a b i l i t y problem by presenting analysis data on fa i led jdefec t ive s i l i con solar c e l l modules of various types and procured from d i f f e r en t manufac- tu re rs . The type of f a i l u r e modes more frequently observed are: in te rna l short and open c i r c u i t s , output power degradation, and i so la t ion res i s tance degradation. The cause of f a i l u r e w i l l be dis- cussed i n d e t a i l and in many cases w i l l be re lated t o t he par t icu la r type of technology used i n t he manufacture of these modules. Wherever applicable, appropriate correct ive act ions w i l l be recommended. Another object ive of t h i s paper i s t o describe some n a r f a i l u r e ana lys i s techniques t h a t had t o be developed because so la r c e l l modules possess

unique s t ruc tu ra i features . Some of these tech- niques allow fo r a non-destructive analysis .

11. FAILURE WDES

During t he past tbo years, f a i l u r e s i n solar c e l l modules have been detected during i n i t i a l e l e c t r i c a l t e s t i ng , environmental t e s t i ng and dur- ing f i e l d appl icat ions. The various types of f a i l u r e s tha t have been observed during t h e JPL f a i l u r e ana lys i s of these modules include: open- c i r c u i t so la r c e l l interconnects; cracked so l a r c e l l s ; delamination a£ t he pro tec t ive encapsulant ; d i e l e c t r i c breakdown; corrosion and vorkmanship . Many open-circuit so la r c e l l interconnect f a i l u r e s were caused by interconnect f a t i gue due t o in- adequate stress r e l i e f . Some of t he interconnects were melted open-circuit and t he surrounding a r ea s were discolored and charred a s a r e s u l t of arcing across t he work hardened and fractured in te r - connect. This condition occurred i n high vol tage f i e l d appl icat ions and s imilar f a i l u r e s were created i n a JPL laboratory t e s t t h a t simulated t he f i e l d conditions. Cracked so l a r c e l l s , i n many instances, resul ted i n open-circuits and/or power degradation of t he modules. I n addi t ion, many of these so la r c e l l s showed evidence of being overheated t o t he extent t ha t t he modules were discolored, burned, charred and t he solder had melted and reflowed on t h e r ea r s i d e of t h e so l a r c e l l . These so la r c e l l s may have been overheated a s a r e su l t of reverse biasing caused by c e l l shadowing, c e l l f rac tur ing o r by c e l l power degra- dation. I n some instances, c e l l f rac tur ing was probably caused by mishandling, environmental s t r e s se s or the f rac tures may not have been de- tected during initial v i sua l inspection. Delamin- a t ion of t he protect ive encapsulant i n many in- stances was caused by physical movement of t he solar c e l l interconnects due t o inadequate s t r e s s r e l i e f and by physical movement of t h e so l a r c e l l s due t o overheating. I n some instances, delamin- a t ion of t he protect ive encapsulant was caused by environmental e f fec t s . Die lec t r ic breakdown, i n one instance, was caused by a sharp bent strand of a wire mesh interconnect tha t had penetrated the insulat ion mater ial t o t he metal subs t ra te o r frame. I n another instance, d i e l e c t r i c breakdown was caused by a cut o r break in an insulated cable

* This paper presents t he r e s u l t s of one phase of research conducted a t t he J e t Propulsion Laboratory, California I n s t i t u t e of Technology fo r t he Department of Energy, by agreement with the National Aeronautics and Space Administration.

Proceedings of the 13th IEEE Photovoltaic Specialists ConferenceWashington, D.C., June 4-8, 1978, pp. 824-834

t h a t r e s u l t e d i n breakdown t o t h e m e t a l s u b s t r a t e or connector box. Corrosion of s t randed wire cab les t o a module increased t h e dc r e s i s t a n c e of t h e c a b l e s u f f i c i e n t l y t o degrade t h e peak power po in t of t h e module. There was another i n s t a n c e where t h e co r ros ion of t h e wire mesh in terconnect between a s o l a r c e l l and t h e module's end term- i n a t i o n r e s u l t e d i n an open-ci rcui t . Typical work- manship d e f e c t s included a c u t i n s u l a t e d w i r e t h a t r e s u l t e d i n a dec rease i n i n s u l a t i o n r e s i s t a n c e between t h e s o l a r c e l l s and t h e metal s u b s t r a t e , excess so lde r a t t h e edge of a s o l a r c e l l t h a t decreased t h e ce l l t s shunt r e s i s t a n c e s u f f i c i e n t l y t o degrade t h e peak power p o i n t of t h e module, improperly t igh tened screws holding t h e module's c o n t a c t s on a Jones terminal b lock t h a t r e s u l t e d i n an open-ci rcui t and unsoldered in te rconnec t s t o t h e r e a r c o n t a c t s of a s o l a r c e l l t h a t r e s u l t e d i n an open-c i rcu i t .

In te rconnec t s

There were numerous i n s t a n c e s where t h e s o l i d metal r ibbon in te rconnec t s between s o l a r c e l l s be- came work hardened and f r a c t u r e d open-ci rcui t dur ing thermal cyc l ing due t o improper o r inad- equate stress r e l i e f of t h e s e in te rconnec t s as shown i n F igures 1 A and 1 B . I n most i n s t a n c e s , v i s u a l examination of t h e s e in te rconnec t s a t a magnif ica t ion of 7 X t o 30X was s u f f i c i e n t t o de- t e c t t h e work hardened a r e a s , however, d e t e c t i o n of t h e a c t u a l f r a c t u r e s i t e s was n o t always pos- s i b l e . A non-dest ruct ive capac i t ance measurement technique was s u c c e s s f u l l y used t o d e t e c t an open- c i r c u i t me ta l in te rconnec t between s o l a r c e l l s . T h i s test procedure i s desc r ibed l a t e r under " F a i l u r e Analys is Techniques." Following t h i s non-dest ruct ive e l e c t r i c a l t e s t , t h e p r o t e c t i v e encapsulant d i r e c t l y above t h e f r a c t u r e d open- c i r c u i t me ta l in te rconnec t was removed a s w e l l a s a p o r t i o n of t h e f i b e r g l a s s s u b s t r a t e below t h e f r a c t u r e s i t e . The f r a c t u r e s i t e s were back- l i g h t e d and photographed a s shown i n Figure 1B.

There were s e v e r a l i n s t a n c e s where t h e open- c i r c u i t s occurred i n s o l i d me ta l r ibbon i n t e r - connects between s o l a r c e l l s a s a r e s u l t of t h e in te rconnec t s me l t ing a s shown i n Figure 1 C . Modules t h a t f a i l e d i n t h i s manner had been in- s t a l l e d i n 30 module s e r i e s s t r i n g s feeding a 240 v o l t b a t t e r y system i n a f i e l d a p p l i c a t i o n . I n a l l of t h e s e i n s t a n c e s t h e massive damage i n t h e f a i l e d a r e a s of t h e modules prevented d i r e c t determinat ion of t h e cause of f a i l u r e . Examin- a t i o n of t h e remaining c e l l in t e rconnec t s , a review of t h e f i e l d a p p l i c a t i o n c i r c u i t and of o t h e r JPL f a i l u r e s of s i m i l a r modules ind ica ted that one of t h e most probable causes of f a i l u r e r e s u l t e d from high v o l t a g e a r c i n g a c r o s s t h e small f r a c t u r e a i r gaps t h a t developed i n t h e c e l l i n t e r c o n n e c t s due t o inadequate s t r e s s r e l i e f . JPL f a i l u r e a n a l y s i s simulated t h e e l e c t r i c a l f i e l d t e s t cond i t ions and when t h e c e l l i n t e r - connects were c u t t o s imula te t h e f i e l d t e s t f r a c t u r e gaps , a r c i n g and smoking were observed a t t h e cu t in te rconnec t , a long w i t h occas iona l flames. Delamination and c h a r r i n g of t h e encapsulant and f i b e r g l a s s s u b s t r a t e was observed

i n a d d i t i o n t o s o l a r c e l l f r a c t u r i n g , mel t ing of t h e metal in terconnect and so lde r . I n f a c t , f a i l - u r e r e s u l t s s i m i l a r t o those observed i n t h e high vo l t age f i e l d a p p l i c a t i o n were c rea ted i n t h e JPL l abora to ry t e s t s imulat ion a s shown i n Figure I D . A s a r e s u l t of t h e s e f ind ings , t h e recommended cor- r e c t i v e a c t i o n included s u i t a b l e s t r e s s r e l i e f of t h e c e l l in t e rconnec t s and a v i s u a l inspect ion re- quirement t o minimize t h i s problem. Las t ly , it was recommended that high vo l t age c i r c u i t app l i - c a t i o n s be reviewed f o r p o s s i b l e c o r r e c t i v e a c t i o n such a s including a p r o t e c t i v e diode i n p a r a l l e l wi th each s o l a r module t o bypass t h e r e s u l t i n g high c u r r e n t through a f a i l e d module t o avoid com- p l e t e d i s r u p t i o n of power i n a 30 module s e r i e s s t r i n g .

B. Cracked Cells

This f a i l u r e mode was one of t h e types most f r equen t ly observed. Cracked s o l a r c e l l s i n many ins tances were t h e d i r e c t cause of open-ci rcui ts and/or power degradat ion of t h e modules. I n a d d i t i o n , many of t h e s e s o l a r c e l l s showed evidence of being d i sco lo red , burned, charred and t h e so lde r had melted and reflowed. There a r e numerous pos- s i b l e and in te r - re l a t ed causes f o r cracked c e l l s t h a t include overheating a s a r e s u l t of r e v e r s e b ias ing caused by c e l l shadowing o r by c e l l power degradat ion and, inadequate mechanical stress r e l i e f t o prevent f r a c t u r e s n o t only i n t h e s o l i d metal r ibbon in te rconnec t s between t h e s o l a r c e l l s but f r a c t u r e s i n t h e s o l a r c e l l s a s we l l . I n some ins tances , c e l l f r a c t u r i n g was probably caused by mishandling, environmental s t r e s s e s o r t h e f r ac - t u r e s may have occurred i n t h e manufacturing process and may not have been detected dur ing t h e i n i t i a l v i s u a l inspec t ion and e l e c t r i c a l tests . During t h e JPL f a i l u r e a n a l y s i s of d e f e c t i v e s o l a r modules, it was observed t h a t not & cracked c e l l s produced e l e c t r i c a l degradat ion o r ca ta- s t r o p h i c f a i l u r e of a module. There were many ins tances where t h e cracks were s m a l l and/or d id no t s i g n i f i c a n t l y reduce t h e c u r r e n t c o l l e c t i o n c a p a b i l i t i e s of t h e s o l a r c e l l . However, t h e r e were many ins tances where power degradat ion was caused by c racks s i g n i f i c a n t l y reducing t h e cur- r e n t c o l l e c t i n g a r e a s and where i n t e r m i t t e n t o r permanent open-ci rcui t conditons were c rea ted by c racks i n t e r s e c t i n g t h e main c u r r e n t c o l l e c t o r s of a s o l a r c e l l .

I n many ins tances , JPL f a i l u r e a n a l y s i s found t h a t a v i s u a l examination a t a magnif ica t ion of 7X t o 30X was s u f f i c i e n t t o d e t e c t l a r g e width cracks i n s o l a r c e l l s , however, d e t e c t i o n of t h e narrow width o r microcracks was no t always poss ib le . During t h e s e v i s u a l examinations, it was necessary i n some ins tances , t o u s e s p e c i a l s i d e l i g h t i n g techniques t o h i g h l i g h t some of t h e cracks t h a t might o therwise have gone undetected.

Another non-destruct i v e f a i l u r e a n a l y s i s method t h a t was sometimes success fu l i n t h e d e t e c t i o n of cracked s o l a r c e l l s was x-ray a s descr ibed l a t e r under "Fa i lu re Analysis Techniques." Some examples a r e shown i n Figures 2A and 2B. It w i l l

be noted t h a t i n both examples, no t only a r e t h e c e l l f r a c t u r e s c l e a r l y observed but it i s a l s o evident t h a t both c e l l s were overheated t o t h e e x t e n t t h a t t h e so lde r on t h e r e a r s i d e had melted and reflowed. The minimum temperature had t o be +18OoC s i n c e t h e s o l d e r was 60140, Sn/Pb. Rapid and excess ive hea t ing is one of t h e known e f f e c t s of r e v e r s e b ias ing on a s i l i c o n s o l a r c e l l . S ince cracked c e l l s and- reverse b i a s i n g a r e i n t e r - r e l a t e d , t h e r e were many i n s t a n c e s where JPL f a i l u r e a n a l y s i s could n o t determine whether t h e crack occurred f i r s t and thereby c rea ted a r e - v e r s e b i a s cond i t ion o r whether t h e c e l l f i r s t be- came r e v e r s e b iased , overheated and then cracked a s a r e s u l t of c e l l shadowing o r c e l l power degra- da t ion . It w i l l be noted t h a t c e l l f r a c t u r e s were one of t h e e f f e c t s t h a t were c r e a t e d dur ing t h e JPL l abora to ry t e s t which simulated t h e high v o l t a g e f i e l d a p p l i c a t i o n . This was discussed p rev ious ly under I' I n t e rconnec t s . I t

One promising non-dest ruct ive f a i l u r e a n a l y s i s method was t h e " ~ o l a r C e l l Laser Scanner'' (SCLS) descr ibed l a t e r under "Fa i lu re Analys is Tech- niques." This technique was r e c e n t l y developed by JPL f a i l u r e a n a l y s i s and some examples a r e shown i n Figures 2C through 2F. The d e t a i l s covering each of t h e s e f i g u r e s a r e summarized a s follows:

Figure 2C - This i s an o s c i l l o g r a p h showing t h e scanning l a s e r beam induced c u r r e n t output of a s o l a r c e l l . The l i g h t a r e a of t h i s image repre- s e n t s t h e p o r t i o n t h a t was found e l e c t r i c a l l y con- nected t o t h e o t h e r c e l l s i n t h i s module, whereas t h e da rke r a r e a r e p r e s e n t s t h e c rack separa ted ha l f of t h e c e l l . A 120 ohm r e s i s t a n c e was con- nected a c r o s s t h e f r a c t u r e d p o r t i o n s of t h e main c u r r e n t c o l l e c t o r s f o r t h i s t e s t i n o rde r t o i l l u m i n a t e t h e c rack separated ha l f of t h i s c e l l f o r t h i s photo. Without t h i s 120 ohm r e s i s t a n c e t h i s c rack separated ha l f would have remained da rk and t h e e n t i r e c e l l would no t have been viewed. During e l e c t r i c a l probe t e s t s of t h i s c e l l , under t h e s teady s t a t e l a r g e a r e a i l lumina t ion t e s t e r , t o be discussed l a t e r , a r e s i s t a n c e of 900 ohms w a s de tec ted ac ross both of t h e c r a c k separa ted main c u r r e n t c o l l e c t o r s on t h e s u r f a c e of t h i s c e l l . F igure 2D - T h i s i s a l s o an SCLS image of another s o l a r c e l l s i m i l a r t o Figure 2C except t h a t t h e r e s i s t a n c e a c r o s s t h e c rack was undeter- mined. Again, t h e l i g h t a r e a r e p r e s e n t s t h e p o r t i o n of t h e c e l l s t i l l connected t o t h e o the r c e l l s i n t h i s module, whereas t h e da rke r a r e a r e p r e s e n t s t h e c rack separated por t ion . F igure 2E - This i s a l s o an SCLS image of another s o l a r c e l l s i m i l a r t o Figure 2C except t h a t t h e f r a c t u r e does not c r o s s t h e main c u r r e n t c o l l e c t - o r s on t h e s u r f a c e of t h i s c e l l . F igure 2F - This is a l s o an SCLS image of another s o l a r c e l l simi- lar t o Figure 2C except t h a t t h e v a l u e of re- s i s t a n c e a c r o s s t h e c rack was undetermined.

Another non-dest ruct ive f a i l u r e a n a l y s i s method t h a t was success fu l i n t h e d e t e c t i o n of cracked s o l a r c e l l s was t o shadow t h e c e l l wi th t h e mod- u l e i l luminated. The suspect s o l a r c e l l would be shadowed using a s u i t a b l e mask and t h e c e l l ' s

shunt r e s i s t a n c e could be determined a s de- sc r ibed l a t e r under " F a i l u r e Analys is Techniques."

A s a r e s u l t of t h e s e f i n d i n g s , t h e recommended c o r r e c t i v e a c t i o n included cont inued development of t h e SCLS t e s t system t o improve t h e d e t e c t i o n of h a i r l i n e c r a c k s i n s o l a r c e l l s . It was a l s o recommended t h a t t h e v i s u a l i n s p e c t i o n requ i re - ments used f o r c r a c k d e t e c t i o n should be reviewed and upgraded. It was recognized t h a t v i s u a l i n s p e c t i o n acceptance c r i t e r i a should be s p e c i f i e d t o cover c r a c k s i n e l e c t r i c a l l y "good" c e l l s t h a t might propagate w i t h t ime and c a u s e degrada t ion o r c a t a s t r o p h i c f a i l u r e s . L a s t l y , s i n c e s o l a r c e l l s can be e a s i l y f r a c t u r e d dur ing shipment, s t o r a g e and handl ing, i t was recommended t h a t t h e s e a r e a s be reviewed f o r p o s s i b l e upgrading.

C . Delamina t ion

There were numerous i n s t a n c e s where t h e p r o t e c t i v e encapsulant delaminated from t h e s o l a r c e l l s and/or t h e module s u b s t r a t e s . Examples of t h i s c o n d i t i o n a r e shown i n F igures 3A and 3 B . I n many i n s t a n c e s , t h e delaminat ion was caused by phys ica l movement of t h e s o l a r c e l l i n t e r c o n n e c t s due t o inadequate s t r e s s r e l i e f and by phys ica l movement of t h e s o l a r c e l l s due t o overhea t ing . It w i l l be noted t h a t delaminat ion of t h e pro- t e c t i v e encapsulant was one of t h e e f f e c t s t h a t was c r e a t e d dur ing t h e JPL l a b o r a t o r y test which simulated t h e high v o l t a g e f i e l d a p p l i c a t i o n . I n some i n s t a n c e s , delaminat ion of t h e p r o t e c t i v e - encapsulant was caused by environmental e f f e c t s . I n all i n s t a n c e s , delaminat ion was e a s i l y d e t e c t - a b l e by v i s u a l examination. Based upon t h e s e f i n d i n g s , t h e recommended c o r r e c t i v e a c t i o n was s i m i l a r t o t h o s e p rev ious ly shown f o r i n t e r - connect s and cracked c e l l s .

D. D i e l e c t r i c Breakdown

There were some i n s t a n c e s of d i e l e c t r i c breakdown, a l l of which were r e l a t e d t o poor workmanship, poor manufacturing p r o c e s s and/or q u a l i t y c o n t r o l s . One example i s shown i n Figures 4A and 4B. It w i l l be noted t h a t a 300- 350 Vdc breakdown s i t e occurred between a sha rp ben t s t r and of t h e wire mesh i n t e r c o n n e c t and t h e aluminum s u b s t r a t e . The bent s t r and pene t ra ted t h e i n s u l a t i o n m a t e r i a l between t h e in te rconnec t and t h e m e t a l s u b s t r a t e . Another f a i l u r e re- s u l t e d from a nicked i n s u l a t e d c a b l e t h a t caused a d i e l e c t r i c breakdown t o t h e me ta l s u b s t r a t e o r connector box on t h e module. The f a i l u r e a n a l y s i s techniques used t o d e t e c t t h e s e f a i l u r e s cons i s t ed of v i s u a l examination, e l e c t r i c a l tests and p a r t i a l disassembly of t h e module t o i s o l a t e t h e exact f a i l u r e s i t e s .

The recommended c o r r e c t i v e a c t i o n included im- proved v i s u a l inspec t ion and upgrading t h e man- u f a c t u r e r ' s process and q u a l i t y c o n t r o l s .

E. Corrosion

There were s e v e r a l i n s t a n c e s of power degra- d a t i o n and/or open-c i rcu i t s t h a t were d i r e c t l y

caused by cor ros ion as shown i n F igures 5A through 5D. I n one i n s t a n c e , a rubber i n s u l a t e d s t randed w i r e c a b l e t o a module became t a rn i shed and corroded w i t h a b lack colored contaminant. A s a r e s u l t , t h e dc r e s i s t a n c e of t h e c a b l e increased s u f f i c i e n t l y t o degrade t h e peak power p o i n t of t h e module s i g n i f i c a n t l y . The cor ros ion products were examined us ing t h e scanning e l e c t r o n microscope (SEM) and t h e energy d i s p e r s i v e a n a l y s i s of x-rays (EDAX) u n i t s . The cor ros ion is shown in F igure 5A and t h e co r ros ion p roduc t s a r e i d e n t i f i e d a s CuS and Cu a s shown i n F igure 5B The recommended c o r r e c t i v e a c t i o n was t o r e p l a c e t h e rubber covered s t r anded w i r e c a b l e s w i t h a more s u i t a b l e neoprene jacketed t inned copper s t randed wi re c a b l e i n o rde r t o avoid t h e s u l f u r co r ros ion problems. I n ano the r i n s t a n c e , cor- r o s i o n of t h e w i r e mesh in te rconnec t between a s o l a r c e l l and t h e end t e rmina t ion of t h e module caused a n open-ci rcui t a s shown i n F igures 5C and 5D. Th i s oper,-circuit was bel ieved t o be caused by a combination of a r e a c t i v e chemical such a s c h l o r i n e and improper i n s t a l l a t i o n of t h e s o l d e r t a b and in te rconnec t ing mesh. Cracking of t h e RTV p r o t e c t i v e encapsulant around t h e s o l d e r t a b permit ted mois tu re t o p e n e t r a t e and a c c e l e r a t e t h e co r ros ion process . The recommended c o r r e c t i v e a c t i o n i n t h i s i n s t a n c e included improved v i s u a l i n s p e c t i o n and upgrading t h e manufacturer ' s process and q u a l i t y c o n t r o l s .

Workmanship

Poor workmanship r e s u l t e d i n numerous and va r i ed types of f a i l u r e modes i n s o l a r modules. Severa l t y p i c a l examples a r e shown i n Figures 6A through 6E. The d e t a i l s cover ing each of t h e s e Figures a r e summarized a s fo l lows:

Figure 6A - A s shown i n t h i s photo, a c u t i n an i n s u l a t e d w i r e near t h e t e rmina t ion box of t h i s module r e s u l t e d i n a s i g n i f i c a n t d e c r e a s e i n in - s u l a t i o n r e s i s t a n c e between t h e s o l a r c e l l s and t h e aluminum frame. The i n s u l a t i o n r e s i s t a n c e dec rease was observed d i r e c t l y fo l lowing a s a l t - fog environmental test. The f a i l u r e a n a l y s i s technique used t o d e t e c t t h e exact f a i l u r e s i te included p a r t i a l immersion of t h e module i n a s a l i n e s o l u t i o n and then removing p o r t i o n s of t h e me ta l frame u n t i l t h e f a i l u r e s i t e was i s o l a t e d us ing a megohm br idge . Visual examination of t h e i n s u l a t e d w i r e d i s c l o s e d t h a t it had been c u t dur ing t h e manufacturing p rocess . F igure 6B - Excess s o l d e r a t t h e edge of t h i s s o l a r c e l l r e - s u l t e d i n a low shunt r e s i s t a n c e of 2 5 ohms and caused a smal l power degrada t ion i n t h e module. When t h e s o l d e r splashed p o r t i o n of t h i s c e l l was removed by c u t t i n g through t h e c e l l j u n c t i o n w i t h a diamond s c r i b e , t h e c e l l ' s shunt r e s i s t a n c e in- creased t o a normal va lue . T h i s f a i l u r e a n a l y s i s technique was d e s t r u c t i v e s i n c e i t was necessary t o remove t h e RTV p r o t e c t i v e encapsulant over t h e c e l l w i t h an x-act0 k n i f e whi le v i s u a l l y monitor- ing t h i s procedure under a microscope. The c e l l ' s shunt r e s i s t a n c e was measured us ing e l e c t r i c a l probes through t h e RTV encapsu lan t . Figure 6 C - This photo shows a s o l a r module term- i n a t i o n box w i t h i t s cover removed. The screws

holding both ends of a metal jumper on t h e Jones terminal b lock were n o t t igh tened dur ing t h e manufacturing process and t h e r e f o r e caused an open-ci rcui t i n t h e module. Figure 6D - An un- soldered in terconnect t o t h e r e a r con tac t of t h i s s o l a r c e l l r e s u l t e d i n an i n t e r m i t t e n t open- c i r c u i t . The exact f a i l u r e s i t e was loca ted us ing t h e non-des t ruc t i v e capac i t ance measurement procedure descr ibed l a t e r under "Fa i lu re Analys is Techniques .'I Following t h i s non-dest ruct ive e l e c t r i c a l t e s t , t h e aluminum s u b s t r a t e was mi l l ed away from t h e unders ide o f t h e module t o expose t h e r e a r of t h i s c e l l . F igure 6E - An unsoldered in te rconnec t t o t h e r e a r con tac t of a s o l a r c e l l a l s o r e s u l t e d i n an open-ci rcui t i n t h i s module. The exact f a i l u r e s i t e i n t h i s i n s t a n c e was lo- ca ted us ing t h e non-dest ruct ive x-ray method descr ibed l a t e r under "Fa i lu re Analys is Tech- niques." A s shown i n t h i s x-ray photo, t h e un- soldered in te rconnec t s t o t h e r e a r c o n t a c t s of one c e l l a r e l i g h t colored a r e a s whereas t h e da rk colored a r e a s on t h e o t h e r c e l l s i n d i c a t e t h a t they were soldered. A s a r e s u l t of these f i n d i n g s t h e recommended c o r r e c t i v e a c t i o n in- cluded improved v i s u a l inspec t i o n and upgrading t h e manufacturer ' s process and q u a l i t y c o n t r o l s .

111. FAILURE ANALYSIS TECHNIQUES

Use of d i f f e r e n t types of m a t e r i a l s , s t r u c t u r e s , s i l i c o n s o l a r c e l l processes and c e l l in t e rconnec t s i n t h e des ign of c u r r e n t l y manufac- tu red s o l a r c e l l modules p resen t s a l a r g e number of v a r i a b l e s t h a t a f a i l u r e a n a l y s t must contend wi th . To be a b l e t o cope wi th t h e s e problems, new a n a l y t i c a l techniques need t o be developed and, i n many c a s e s , e x i s t i n g techniques need t o be modified t o accommodate s t r u c t u r a l f e a t u r e s unique t o modules.

Experience gained i n f a i l u r e a n a l y s i s wi th in t h e p a s t two yea r s has l e d t o t h e development and a p p l i c a t i o n of numerous a n a l y t i c a l techniques . It i s c l e a r t h a t a s f a i l u r e a n a l y s i s technology matures, numerous o t h e r u s e f u l techniques w i l l be developed. Some of t h e techniques which have been p a r t i c u l a r l y u s e f u l w i l l be descr ibed here . They can be divided i n t o two c a t e g o r i e s : non- d e s t r u c t i v e and d e s t r u c t i v e . Non-destructive techniques a r e p a r t i c u l a r l y important because they a l low f o r non-dest ruct ive inspec t ion , examination, t e s t i n g , eva lua t ion and charac te r - i z a t i o n of a f a i l e d / d e f e c t i v e module. Des t ruc t ive techniques a r e u s e f u l f o r disassembly of en- capsula ted modules without des t roy ing f a i l u r e evidence. Th i s is important f o r i s o l a t i o n and i d e n t i f i c a t i o n of f a i l u r e s i t e s and f o r macro- scopic and microscopic a n a l y s i s of f a i l u r e s i t e s .

A . X-Ray Radiography

Problems a s s o c i a t e d wi th t h e backside of s o l a r c e l l s a r e not r e a d i l y a c c e s s i b l e f o r v i s u a l examination f o r most module des igns . However, x- r a y radiography has proven t o be a very va luab le non-dest ruct ive technique f o r observing unsoldered back c o n t a c t s , opens i n in te rconnec t s and so lde r r e f low on back c o n t a c t s r e s u l t i n g from c e l l

overheating. Figures 2A and 2B a r e radiographs showing solder ref low and present c l e a r evidence of a c e l l overheating problem. Figure 6E shows an unsoldered back contact . This technique is now commonly used i n f a i l u r e ana lys i s .

B. Capacitance Measurement Technique

It may not always be poss ib le t o l o c a t e an e l e c t r i c a l open o r a high r e s i s t a n c e con tac t i n a l a r g e c e l l s t r i n g by x-ray radiography o r o p t i c a l inspect ion. I n such a case , a capaci tance measure- ment technique may prove t o be very use fu l . I n t h i s non-destructive technique one of t h e wire l e a d s from a module c e l l s t r i n g and a wire lead from a f l a t metal p l a t e with t h e same sur face dimensions a s a c e l l a r e connected t o a capaci tance m e t e r . The o t h e r wire l ead from t h e c e l l s t r i n g is l e f t f l o a t i n g . A capaci tance measurement i s made f o r each placement of a f l a t p l a t e on t h e in- s u l a t i n g encapsulant d i r e c t l y over a c e l l . A sig- n i f i c a n t change i n capaci tance f o r two neighboring c e l l p o s i t i o n s is considered t o be t h e suspect area . Measurements a r e repeated by interchanging t h e connections on t h e s t r i n g . This technique i s app l icab le i f t h e r e a r e no more than two d i f f e r e n t f a i l u r e site loca t ions .

C. C e l l Shunt Resistance Measurement by Shadowing Technique

C e l l leakage c u r r e n t s due t o a shunt resist- ance c o n t r i b u t e t o power l o s s e s i n modules. Therefore, i n many ins tances , i t is important t o be a b l e t o measure t h e shunt r e s i s t a n c e of indi- v idua l c e l l s i n a module, p re fe rab ly without d i s - rup t ing o r destroying t h e encapsulation. Th is can be accomplished by using a shadowing technique.

Procedures f o r measuring t h e shunt r e s i s t a n c e (RSH) of ind iv idua l c e l l s i n a module cons i s t ing of a s i n g l e s t r i n g with N s e r i e s connected c e l l s i s a s follows: Measure t h e open c i r c u i t vo l tage (VoC) of t h e module under i l luminated condi t ions . Place shadow mask over test c e l l and apply t o t h e module a c u r r e n t load 10 where 10 is considerably smal ler than t h e module short c i r c u i t cur ren t ( I S C ) . IO i s t y p i c a l l y 100-250 mA. Measure v o l t a g e (VO) ac ross load. The module should be maintained a t t h e same temperature f o r both sets of measurements. The equation f o r RSH:

where (N-1) Voc/N is t h e photovoltage ac ross t h e N-1 unshadowed c e l l s and (N-1) vOC/N - Vo i s t h e reverse b i a s vo l tage across t h e shadowed c e l l .

Typical ly , t h e reverse b i a s I-V c h a r a c t e r i s t i c s f o r a c e l l is non-linear and t h e r e f o r e RSH is ex- pected t o vary somewhat with 10. There w i l l be some l i g h t leakage c a r r e n t due t o s i d e i l lumin- a t i o n and i n t e r n a l r e f l e c t i o n s of l i g h t s c a t t e r e d from neighboring c e l l s and subs t ra te . P a r t i c u l a r - l y f o r t h e c e l l s wi th a high shunt r e s i s t a n c e , t h i s leakage cur ren t may in t roduce a s i g n i f i c a n t e r r o r i n t h e ca lcu la ted value of RSH i f not ap- p ropr ia te ly accounted f o r .

D. Steady-State I l lumina t ion Test S t a t i o n f o r Module Performance Evaluat ion

A t e s t s t a t i o n i n which a f a i l e d l d e f e c t i v e module can be t e s t e d under c o n t r o l l e d i l lumina t ion condi t ions i s needed f o r v e r i f i c a t i o n of reported f a i l u r e s and f o r eva lua t ion of photovol ta ic re - sponse c h a r a c t e r i s t i c s of c e l l s wi th in t h e module. An i l lumina t ion s t a t i o n shown i n Figure 7 was fabr ica ted with t h e fol lowing s p e c i f i c a t i o n s : F i r s t , it provides an i l lumina t ion over a two by four f o o t a r e a i n order t o accommodate t h e l a r g e r modules c u r r e n t l y being manufactured. Second, t h e s p a t i a l v a r i a t i o n i n t h e l i g h t i n t e n s i t y is l e s s than t e n percent . Third, t h e range of i l lumin- a t i o n i n t e n s i t y i s wide t o be a b l e t o eva lua te performance of modules under t h e var ious perform- ance of modules under t h e var ious exposure con- d i t i o n s t y p i c a l l y observed i n f i e l d opera t ions . Fourth, t h e dwell t ime f o r t h e s teady s t a t e i l lumina t ion can be s e t from a few seconds t o hours, making it poss ib le t o observe e f f e c t s of d i f f e r e n t exposure t imes on module c h a r a c t e r i s t i c s .

The i l lumina tor c o n s i s t s of a bank of quar tz tung- s t e n lamps powered by ganged v a r i a c s wi th a motor- d r ive . The s p e c t r a l response for t h e s e lamps i s much higher i n t h e i n f r a r e d region and lower i n t h e s h o r t e r wave l e n g t h region a s compared with t h e s o l a r s p e c t r a l response. Even though t h e in f ra red response can be reduced by f i l t e r i n g , it is no t poss ib le t o be a b l e t o o b t a i n a good i t c h with t h e s o l a r s p e c t r a l response. However, i n many ins tances , t h i s i l lumina t ion system i s more than adequate f o r performing f a i l u r e a n a l y s i s on fa i l ed /def e c t i v e modules. I f a more d e t a i l e d eva lua t ion of a module i s needed a JPL l a r g e a r e a pulsed s o l a r s imulator t e s t f a c i l i t y i s used.

E . Laser Scanning Techniques f o r So la r Cells

Response c h a r a c t e r i s t i c s r e s u l t i n g from an il lurninat ion of microscopic a r e a s on s o l a r c e l l s can provide very u s e f u l information about micro- scopic inhomogeneities a £ f ec t ing t h e e l e c t r i c a l performance of a module. This type of information can r e a d i l y be obtained by using a l a s e r scan technique, b r i e f l y described below. More d e t a i l e d information w i l l be presented elsewhere. (Ref. 1)

A focused laser beam i s def lec ted i n a r a s t e r p a t t e r n over t h e sur face of a s o l a r c e l l . This r a s t e r p a t t e r n i s a l s o displayed on a cathode ray tube (CRT) of an osc i l loscope . The e l e c t r i c a l response s i g n a l s measured e i t h e r a t t h e module t e rmina l s o r ac ross t h e test c e l l a r e amplif ied. These amplified s i g n a l s a r e used t o modulate t h e b r igh tness c o n t r o l on t h e osc i l loscope . That i s , t h e s t ronger t h e s i g n a l , t h e b r i g h t e r t h e focused beam spot on t h e CRT. With t h i s se tup , an image of t h e t e s t c e l l i s displayed on t h e CRT. Photo- graphs of l a s e r scan images of severa l d i f f e r e n t c e l l s a r e shown i n Figures 2C through 2F.

A g r e a t d e a l of va luab le information i s contained i n t h e d i sp lay image. The p o s i t i o n of a po in t on t h e image of t h e t e s t c e l l corresponds t o t h e same po in t i n t h e t e s t c e l l . The d i f f e r e n c e i n

b r i g h t n e s s between tw d i f f e r e n t p o i n t s on t h e image is d i r e c t l y r e l a t e d t o d i f f e r e n c e s in t h e e l e c t r i c a l response c h a r a c t e r i s t i c s between t h e two corresponding p o i n t s on t h e t e s t c e l l . Th i s is a non-des t ruc t ive technique because t h e aur- f a c e of a t e s t s o l a r c a l l can b e scanned w i t h t h e encapsulant i n t a c t ,

Scanning E lec t ron Uicroscope

The scanning e l e c t r o n microscope (SEH) is a very u s e f u l a n a l y t i c a l t o o l f o r which t h e r e a r e many a p p l i c a t i o n s . Only a few a r e l i s t e d here. I t is u s e f u l f o r exanining s u r f a c e f e a t u r e s of microecopic f laws in s o l a r c a l l a under very high magnif icat ion (100,000X). By opera t ing t h e SEH i n t h e e l e c t r o n baam induced c u r r e n t mode, micro- scopic d e f e c t s o f f e c t b g t h e performance of a s o l a r c e l l can be inves t iga ted . With an energy d i sper - s i v e x-ray ana lyzer on an SEH, an e l m e n t a l analy- sis can be performed f o r i d e n t i f i c a t i o n of element- a l c o n s t i t u e n t s of m a t e r i a l s used in t h e s o l a r c e l l .

The SEH i s b a s i c a l l y a d e s t r u c t i v e technique be- cause t h e test chamber is designed t o acco~rnodate small a r e a speciaens .

Other Techniques

Three a d d i t i o n a l f a i l u r e a n a l y s i s techniques w i l l be discussed he re . They include a p a r t i a l corona d i scharge d e t e c t o r , a hot-spot d e t e c t o r and a sand b l a s t e r .

For many a p p l i c a t i o n s modules need t o be designed t o have a high d i e l e c t r i c wi ths tanding vo l t age be- tween t h e s u b s t r a t e and t h e encapsulated s o l a r c e l l s . Therefore , i t i s i s p o r t a n t t o be a b l e t o measure non-dest ruct ively , t h e d i e l e c t r i c with- s tanding vo l t age c h a r a c t e r i s t i c s i n o rder t o de- termine t h e adequacy of t h e design and t o i d e n t i f y and i n v e s t i g a t e breakdovn s i t e s in f a i l e d / d e f e c t i v e modules. A p a r t i a l corona d i scharge d e t e c t o r system s p e c i a l l y designed t o accommodate l a r g e modules provide6 t h i s c a p a b i l i t y .

A bubble t e s t technique can be used f o r de tec t ing hot-spots on t h e su r face of a s o l a r c e l l . A s o l a r c e l l is immersed in a b a t h containing a non- conductive f l u i d wi th a b o i l i n g po in t s l i g h t l y above room temperature. A good candidate f l u i d is fluorocarbon PC-88 which has a 30°C b o i l i n g point . Power t o t h e s o l a r cel l is Increased u n t i l minute bubbles begin t o QLanate from t h e hot spot a reas . These bubbles can be de tec ted wi th t h e a i d of a low power microscope. This is u s u a l l y a des t ruc - t i v e technique because ordinarily t h e encapsulant i s s t r ipped i n o rder t o be a b l e t o d e t e c t t h e hot-spots.

Polymeric encapsulants can r e a d i l y be penetra ted with sharp-pointed probes f o r in-s i tu e l e c t r i c a l probing of eo la r c e l l s . T h i s approach is not f e a s i b l e f o r modules wi th a g l a s s cover. However, d i r e c t probing is poss ib le provided that whdows a r e cu t i n t h e g l a s s cover. This can be achieved by using a micro sandb las te r . The a r e a s where windows a r e t o be c u t a r e ~ur rounded with a mask- ing t ape . Exposed a r e a s a r e r a p i d l y cu t away with a j e t stream of a b r a s i v e materiel. Usually t h e r e i s a t h i n l a y e r of polymeric mate r ia l such a s RTV d i r e c t l y under t h e g l a s s cover. Th i s l a y e r w i l l p r o t e c t t h e s o l a r c e l l s and t h e metal r ibbon in te rconnec t s from abras ion damage. This tech- nique does des t roy t h e i n t e g r i t y of t h e module.

I V . AcKNOWLEmmNTS

The au thors wish t o thank Emmett Mi l l e r and Richard P i e t y f o r t e c h n i c a l a se ie tance , Ken Evans and Gordon Thomas f o r scanning e l e c t r o n microscope support and Larry Dumas and Steve Sol lock f o r numerous d i scuss ions and encouragements.

V. REFERENCE

1. E. L . Mi l l e r , A. Shurnka, M. Gauthier , "A Laser Scanner f o r S o l a r C e l l Evaluation and F a i l u r e Analysis" t o be published i n t h e Advanced Techniques i n F a i l u r e Analysis Symposium, 1978 Proceedings .

M e t a1 Work Frac tu red I n t e r c o n n e c t s Hardened Apa ,Solar C e l l

P e t a l m t e r c o n n e c t B

Figure 1, A - D I n t e r c o n n e c t F a i l u r e s

A - Fractured meta l in te rconnec t f r o n t l i g h t e d ; B - Frac tu red metal i n t e r c o n n e c t back l i g h t e d ; C - Charred f a i l u r e s i t e w i t h mel tea i n t e r c o n n e c t t h a t occurred dur ing a f i e l d a p p l i c a t i o n . C e l l f r a c t u r e a t arrows; D - F a i l u r e r e s u l t s s i m i l a r t o t h o s e shown i n "C" obta ined dur ing a s imula ted f i e l d f a i l u r e t e s t .

A B

Figure 2 , A - B Cracked C e l l s

A - X-ray showing s e v e r e m u l t i p l e f r a c t u r e s t h a t c rossed through t h e main c u r r e n t c o l l e c t o r i n t h r e e (3) p l a c e s and evidence of s o l d e r mel t ing on r e a r s i d e of c e l l ; B - F a i l u r e r e s u l t s similar t o t h o s e shown i n "A" except t h a t c e l l was f r a c t u r e d i n a c i r c u l a r p a t t e r n .

E

Figure 2 , (cont inued) C - Cracked C e l l s : C - "Solar c e l l l a s e r scanner (SCLS) scope image of c e l l . The l i g h t a r e a of t h e c e l l r e p r e s e n t s t h e por- t i o n e l e c t r i c a l l y connected t o t h e o t h e r c e l l s i n t h i s module whereas t h e da rke r a r e a r e p r e s e n t s t h e c rack separa ted p o r t i o n ; D - F a i l u r e r e s u l t s s i m i l a r t o those shown i n "C"; E - F a i l u r e r e s u l t s s i m i l a r t o those shown i n "C" except t h a t t h f r a c t u r e does no t c r o s s t h e main c u r r e n t c o l l e c t o r s ; F - Same a s "D".

A B F igure 3 , A - B Delamination

A - Delamination of RTV ( s i l i c o n rubber) encapsulant from module; B - F a i l u r e r e s u l t s s i m i l a r t o t h o s e shown i n "A".

I - 300-d2, Vdc Breakdown S i t e .

Figure 4 , A - B D i e l e c t r i c Breakdown

A - D i e l e c t r i c breakdown between wire mesh interconnect and aluminum s u b s t r a t e caused by a sharp bent s t rand of interconnect that penetrated t h e i n s u l a t i o n m a t e r i a l t o t h e s u b s t r a t e . (See "B"); B - Closer view of breakdown s i t e shown i n "A".

C D Figure 5 , A - D Corrosion

A - SEM photo showing blackened a r e a s found on stranded c a b l e wire; B - EDAX photo of contaminants shown i n "A". This condi t ion caused abnormally high s e r i e s r e s i s t a n c e i n module; C - Open c i r c u i t between wire mesh interconnect and module termination caused by corrosion; D - Closer vtew of open-circui t f a i l u r e site.

Figure 6, A - E Workmanship

A - Cut s o l i d wire; B - Excess s o l d e r a t c e l l edge (upper arrow). Mark made with diamond s c r i b e a t lower arrow t o i s o l a t e t h i s 25 ohm s h o r t caused by s o l d e r b a l l ; C - Termination box of module wi th cover removed and p a r t i a l l y depot ted. Both screws a t arrows were not t igh tened during manufacturing process r e s u l t i n g in an open-circui t ; D - Wire mesh in te rconnec t t o r e a r s i d e of c e l l unsoldered, r e s u l t i n g i n an i n t e r m i t t e n t open-circui t ; E - X-ray of module showing unsoldered in te rconnec t s t o r e a r s i d e of c e l l 26 t h a t r e s u l t e d i n an open-circui t .

Steady state illumination station for performance evaluation of large area solar c e l l modules.