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Evaluating the reliability of optical connectors<br />

Report 1<br />

Evaluating the reliability of optical connectors<br />

Yuichi Aoki Technical Development Headquarters, Reliability Research Section<br />

Kishichi Sasaki Reliability Center for Electronic Components of Japan, Environmental Testing Laboratory<br />

Kiyoyuki Mutaguchi Japan Aviation Electronics Industry, Limited, Connector Division<br />

W<br />

e performed the High Temperature Storage Test (Damp Heat) and the<br />

Temperature Cycling Test on optical connectors in conformance to<br />

the Telcordia standards. During these reliability tests, automatic<br />

measurements of the optical characteristics of the specimens were carried<br />

out and physical changes were compared. During the evaluation following<br />

the tests, we checked for physical changes in the tips of the optical connectors.<br />

We found pistoning changes occurring on the tips of the connectors, especially<br />

during the Temperature Cycling Test. However, these pistoning changes caused<br />

almost no perceptible changes in optical characteristics. The ferrule tips were<br />

distorted after 2000 hours at 85°C and 85 percent relative humidity, exhibited<br />

flattening distortion.<br />

1<br />

Introduction<br />

Next-generation technology infrastructure using optical fiber has been on the march<br />

toward achieving widespread use during recent years. Acceptance of this technology has<br />

resulted in demand for lower cost and miniaturized optical components, but such<br />

improvements must be based on information from reliability testing assuring that quality<br />

can be maintained. Testing to evaluate reliability of optical components is generally<br />

performed in conformance to the Telcordia standards. *1 These standards include<br />

requirements for simultaneously measuring optical characteristics of multiple specimens<br />

during environmental testing. 1) Measurement methods are not affected by measurement<br />

margin of error when measuring with the connectors either connected or disconnected.<br />

Additionally, automatic measuring is capable of efficiently gathering data at short<br />

measurement intervals. MTF (Mean Time to Failure) calculations are easy to perform using<br />

this system, for which published examples are available. 2,3) This report will focus on optical<br />

connectors, which exhibit the basic characteristics of optical components. We shall also<br />

consider the results of reliability testing that incorporates automatic measuring in<br />

conformance to the Telcordia standards.<br />

Fig.1 Overview of optical components<br />

- 1 -<br />

Espec Technology Report No20


Evaluating the reliability of optical connectors<br />

2<br />

The Telcordia standards that require simultaneously measuring optical characteristics of<br />

multiple specimens are mainly concerned with passive optical components. In this report<br />

the term "passive optical components" refers to such items as fiber, connectors,<br />

switches, couplers, attenuators, and all types of filters. Table 1 shows reliability tests for<br />

typical optical components.<br />

3<br />

Test standards for passive optical components<br />

Table 1 Telcordia test standards<br />

Standard Title<br />

GR-326-CORE<br />

Generic Requirements for Single-Mode Optical Connectors and<br />

Jumper Assemblies<br />

GR-1209-CORE Generic Requirements for Passive Optical Components<br />

GR-1221-CORE<br />

Generic Reliability Assurance Requirements for Passive Optical<br />

Components<br />

Structure of optical connectors and factors affecting their reliability<br />

Optical connectors are<br />

used to connect optical<br />

fiber. Photo 1 shows<br />

some typical<br />

connectors. Fig.2<br />

shows the composition<br />

of the optical<br />

connectors used in these tests.<br />

The fiber is inserted into the housing, which is called a zirconia ferrule, and the fiber is<br />

held in place with a hardening epoxy adhesive. The adhesive used for the connectors is<br />

Epo-Tek353ND (Epoxy Technology, Inc.). The degradation of this adhesive is a crucial<br />

element leading to the loss of the reliability of the optical connectors. A major factor<br />

producing degradation is the absorption of humidity, which causes degradation to occur<br />

over time. 1~5) Photo 1 Optical connectors<br />

The High Temperature Storage Test (Damp Heat) is used to evaluate<br />

humidity-induced degradation. As Fig.2 shows, adhesive degradation resulted in<br />

pistoning changes to the ferrule tip on the end of the optical connectors. A significant<br />

amount of pistoning causes such problems as an increase in air layers and an increase in<br />

leakage of insertion light. These problems result in an increase in optical loss.<br />

The Temperature Cycling Test was also run to evaluate the progression of cracking<br />

caused by micro-cracks in the fiber.<br />

- 2 -<br />

Espec Technology Report No20


Evaluating the reliability of optical connectors<br />

Fig.2 Structure of optical connectors and factors affecting their reliability<br />

4<br />

Environmental test system for optical components<br />

An environmental test system for optical components was developed to be used in this<br />

research for testing the reliability of passive optical components. Photo 2 shows the<br />

system, and Fig.3 shows a block diagram of the system.<br />

This measurement system selects the light source wavelength using an optical switch<br />

selector, and is capable of measuring a maximum of 170 channels simultaneously for<br />

multiple specimens during environmental testing. This capability puts the system in<br />

conformance to the requirements of the Telcordia standards. The system is capable of<br />

measuring insertion loss, *4 return loss, *5 and PDL (Polarization Dependent Loss). *6<br />

Photo 2 Environmental Test System<br />

- 3 -<br />

Espec Technology Report No20


Evaluating the reliability of optical connectors<br />

5<br />

Test method<br />

Fig.3 System block diagram<br />

The High Temperature Storage Test (Damp Heat) and the Temperature Cycling Test<br />

were run using optical connectors as specimens. Table 2 shows the test conditions, and<br />

Table 3 shows the specimens. The test conditions complied with the<br />

Telcordia-GR-1221-CORE standards. The specimens consisted of single mode *7 SC and FC<br />

connectors. As seen in Fig.4, the specimens were connected in groups of three optical<br />

connectors with fiber and with the measurement points n = 5 (groups). The<br />

measurement system was used to measure insertion loss and return loss. Table 4 shows<br />

the measurement conditions.<br />

The test specimens were measured after each 1000 hours of the High Temperature<br />

Storage Test (Damp Heat) and after the completion of the Temperature Cycling Test. A<br />

Ferrule Tip Condition Surveyor (Direct Optical Research Company) was used to measure<br />

ferrule tip curvature radius, *8 eccentricity, *9 and pistoning. Failure was determined using<br />

the Telcordia-GR-1221-CORE evaluation standards shown in Table 5.<br />

The Temperature Cycling Test was not effective for determining degradation, since<br />

changes occurred in both insertion loss and return loss in the optical fiber temperature<br />

characteristics in this test. The PVC sheath *10 coating in particular exhibited major<br />

changes at low temperatures, and so the test was run using Hytrel ® core *11 , which<br />

exhibited minimal loss at low temperatures as seen in Fig.5.<br />

- 4 -<br />

Espec Technology Report No20


Evaluating the reliability of optical connectors<br />

Table 2 Reliability test conditions<br />

Test items Test Conditions<br />

High<br />

Temperature<br />

Storage Test<br />

(Damp Heat)<br />

Temperature<br />

Cycling Test<br />

85°C, 85%rh,<br />

2000 h<br />

-40°C ←→ 85°C,<br />

1 hour each, 500<br />

cycles<br />

Fig.4 Test method<br />

Table 4 Measurement conditions<br />

Items Details<br />

Measurement items<br />

Insertion loss and<br />

return loss<br />

Light source<br />

wavelength<br />

1310 nm, 1550 nm<br />

Light source power 1 mW<br />

6<br />

Measurement<br />

intervals<br />

Test results<br />

Every 10 to 15 min.<br />

Specimens<br />

No. of<br />

specimens<br />

Evaluation<br />

method<br />

- 5 -<br />

Table 3 Specimens<br />

FC connectors, SC connectors<br />

(single mode)<br />

n = 5<br />

Insertion loss and return loss<br />

(optical component<br />

environmental test system)<br />

Tip condition measurement<br />

(pistoning, eccentricity, and<br />

curvature radius)<br />

Fig.5 Fiber temperature<br />

characteristics<br />

Table 5 Evaluation standards<br />

(from Telcordia GR-1221-CORE)<br />

Requirement Objective<br />

Insertion<br />

loss<br />

change<br />

0.3dB 0.2dB<br />

Return<br />

loss<br />

change<br />

6-1 Test results from the High Temperature Storage Test (Damp Heat)<br />

5dB 2dB<br />

Fig.6 shows the measurement results for the light source wavelength of 1310 nm for the<br />

first 1000 hours of the 2000-hour High Temperature Storage Test (Damp Heat). After<br />

1000 hours and again after 2000 hours, we verified that fluctuation did not exceed any<br />

evaluation standards. In addition, identical trends were exhibited for both light source<br />

wavelengths, 1310 nm and 1550 nm. No major difference was seen between the FC<br />

connectors and the SC connectors.<br />

Espec Technology Report No20


Evaluating the reliability of optical connectors<br />

Test time (h)<br />

(a) SC connector insertion loss<br />

Test time (h)<br />

(c) FC connector insertion loss<br />

- 6 -<br />

Test time (h)<br />

(b) SC connector return loss<br />

Test time (h)<br />

(d) FC connector return loss<br />

Fig.6 Results of the High Temperature Storage Test (Damp Heat)<br />

(light source wavelength: 1310 nm)<br />

6-2 Results of the Temperature Cycling Test<br />

Almost no differences were seen between the FC connectors and the SC connectors in<br />

the Temperature Cycling Test. Fig.7 shows partial measurement results for the SC<br />

connectors. Some insertion loss change and return loss change was seen following<br />

temperature changes in the temperature chamber during the Temperature Cycling Test,<br />

but these changes did not exceed the evaluation standard limits. The changes included<br />

insertion loss occurring at low temperatures, but no major fluctuation was seen at high<br />

temperatures. Return loss, however, tended to increase at high temperatures. Looking at<br />

the return loss changes over the long term confirms that as soon as return loss increases,<br />

the fluctuation stabilizes. This is thought to indicate that return loss quality stabilizes due<br />

to the adhesion of the connectors over time.<br />

Espec Technology Report No20


Evaluating the reliability of optical connectors<br />

(a) Insertion loss<br />

(b) Return loss<br />

Fig.7 Results of the Temperature Cycling Test<br />

(SC connectors; light source wavelength, 1310 nm)<br />

6-3 Pistoning measurement results<br />

Measurement results for the ferrule tip surfaces did not indicate major changes in<br />

eccentricity and curvature radius, but the measurements confirmed that changes<br />

occurred in pistoning compared to the initial values.<br />

Fig.8 shows pistoning measurements after 1000 and 2000 hours of the High<br />

Temperature Storage Test (Damp Heat), and after 500 cycles of the Temperature Cycling<br />

Test. This report represents the direction of pistoning as a negative value. In the IEC, the<br />

standard for tolerance is recommended as -50 to 100 nm, and this level is exceeded, but<br />

the insertion loss and return loss measurements did not exhibit conspicuous fluctuation.<br />

On the other hand, optical connectors with powerful insertion light may be subject to<br />

influence by pistoning. Because of this, we face the challenge of investigating the<br />

relationship between pistoning and optical characteristics in such areas as manufacturing<br />

conditions.<br />

In this research, more pistoning occurred in the Temperature Cycling Test than in the<br />

High Temperature Storage Test (Damp Heat), regardless of whether the type of fiber<br />

coating included Hytrel ® core or the PVC sheath. The cause for the increased pistoning is<br />

thought to include stress in the direction of the pistoning from contraction and peeling of<br />

the adhesive. This, in turn, is thought to be possibly caused by the effects of humidity and<br />

the re-hardening of the adhesive at the test temperature (85°C) for reliability testing.<br />

- 7 -<br />

Espec Technology Report No20


Evaluating the reliability of optical connectors<br />

Test time (h)<br />

(85°C, 85%rh, PVC sheath coating)<br />

Test cycles<br />

(-40/85°C, 1 hour each, PVC sheath coating)<br />

Test cycles<br />

(-40/85°C, 1 hour each, Hytrel ® core)<br />

Fig.8 Changes in pistoning<br />

- 8 -<br />

Espec Technology Report No20


Evaluating the reliability of optical connectors<br />

6-4 Observation of the tip shape<br />

Fig.9 shows the results of observations made on the shape of the ferrule tip before and<br />

after the High Temperature Storage Test (Damp Heat). After 2000 hours at 85°C and 85<br />

percent relative humidity, the surface of the ferrule tip showed signs of pitting and was<br />

rougher than before testing. This roughness did not appear on the surface of the tip after<br />

the Temperature Cycling Test, leading to the conclusion that the roughness was caused<br />

by humidity. Fig.10 shows a three-dimensional computer graphics rendition of the shape<br />

of the tip. After 2000 hours at 85°C and 85 percent relative humidity, the ferrule tip<br />

exhibited flattening distortion. However, pistoning measurements with the Ferrule Tip<br />

Condition Surveyor measured the position of the apex of the tip from the sphericity of the<br />

ferrule tip, and, using that position as a standard, calculated the amount of pistoning.<br />

Accordingly, if the position of the tip section differs from these measurements, the<br />

amount of pistoning could be greater than that calculated.<br />

(a) Initial period<br />

(b) After testing<br />

Fig.9 Ferrule tip observation (85°C, 85%rh, 2000 h)<br />

(Initial period) (-40 /85°C, 500 cycles) (85°C, 85%rh, 2000 h)<br />

Fig.10 Three-dimensional shape of the ferrule tip<br />

- 9 -<br />

Espec Technology Report No20


Evaluating the reliability of optical connectors<br />

7<br />

The optical characteristics of the optical connectors reviewed for this study were<br />

automatically measured during the High Temperature Storage Test (Damp Heat) (at<br />

85°C and 85 percent relative humidity for 1000 hours) and the Temperature Cycling Test<br />

(at 85°C / -40°C for 500 cycles of one hour each). We obtained the following results.<br />

(1)No changes occurred in optical characteristics, but pistoning increased in the<br />

connectors.<br />

(2)Increased pistoning of the ferrule tips was observed in both the Temperature Cycling<br />

Test and the High Temperature Storage Test (Damp Heat), but the major changes<br />

occurred in the Temperature Cycling Test.<br />

(3)The post-test condition of the ferrule tips after testing at 85°C and 85 percent relative<br />

humidity for 2000 hours exhibited flattening distortion. This result could indicate that<br />

the actual pistoning was greater than the calculated amount.<br />

8<br />

Conclusion<br />

Topics for future discussion<br />

Many aspects of the relationship between pistoning and optical characteristics have yet<br />

to be confirmed, and topics such as manufacturing conditions also require research.<br />

[Terminology]<br />

*1.Telcordia<br />

The breakup of the American communications giant AT&T (Bell Telephone) created<br />

seven regional telephone providers (the so-called "Baby Bells") and established a<br />

research and development company initially called Bellcore. Later, when this<br />

subsidiary was sold to a company unrelated to the original Bell, the company became<br />

known as Telcordia Technologies. In the field of communications in the U.S., the<br />

Telcordia standards are widely referenced as the baseline standards for this field.<br />

*2.SC connectors, and *3. FC connectors<br />

Both of these optical connectors are zirconia ferrule (refer to Fig.2 above) connectors<br />

developed in Japan that are widely used throughout the world. The stationary part of<br />

the SC connector is made of plastic, and can be connected by merely being pressed<br />

on. The stationary part of the FC connector, though, is made of metal and must be<br />

attached with screws.<br />

*4.Insertion loss<br />

The transmission loss occurring when light passes through the part. This value<br />

compares the insertion light with the outgoing light, and is expressed in decibels.<br />

*5.Return loss<br />

This value compares the insertion light power and the reflected light power of the<br />

reflected light returning inside the part. This value is expressed in decibels.<br />

- 10 -<br />

Espec Technology Report No20


Evaluating the reliability of optical connectors<br />

*6. PDL (Polarization Dependent Loss)<br />

The PDL value measures the change occurring in insertion loss caused by<br />

polarization. Polarization is a condition of deviation in the vibrational direction of<br />

light.<br />

*7. Single mode<br />

Single mode is a condition which provides light with a single pathway of propagation.<br />

This mode contrasts with multi-mode, which consists of multiple pathways of light<br />

propagation. Due to the mode-dispersed loss occurring in multi-mode, single mode<br />

is used for long-distance transmission.<br />

*8. Curvature radius<br />

The length (in mm) of the radius of a circle from a circumference projected from a<br />

curved surface.<br />

*9. Eccentricity<br />

The length (in µm) of the deviation between the center of the ferrule and the center<br />

of the core of the optical fiber.<br />

*10.PVC sheath<br />

This polyvinyl chloride (PVC) sheath, referred to as optical fiber cable, has a<br />

protective fiber coating. This type of sheath is mainly used indoors.<br />

*11.Hytrel ® core<br />

Hytrel ® is a polyester elastomer made of thermoplastic resin that was developed by<br />

the Dupont Corporation. This substance is an engineering plastic with superb<br />

features such as strength and heat characteristics. Hytrel ® core is a fiber optic<br />

stranded conductor coated with this elastomer.<br />

[Bibliography]<br />

1) "Generic Reliability Assurance Requirements for Passive Optical Components",<br />

Telcordia GR-1221-CORE Issue 2, 1999<br />

2) T. Tomasi, I. De Munari, V. Lista, L. Gherardi, A. Righetti, M. Villa: "Passive optical<br />

components: from degradation data to reliability assessment-preliminary results",<br />

Microelectronics Reliability 42, p.1333-1338, 2002<br />

3) A. Piccirillo, G. Zaffiro, T. Tambosso, G. Gallo: "Reliability of Optical Branching<br />

Devices", IEEE (Institute of Electrical and Electronics Engineers), Journal of Selected<br />

Topics in Quantum Electronics, Vol.5 No.5, 1999<br />

4) F. Caloz, D. Ernst, P. Rossini, L. Gherardi, L. Grassi, J. Arnaud: "Reliability of optical<br />

connectors - Humidity behavior of the adhesive", Microelectronics Reliability 42,<br />

p.1323-1328, 2002<br />

5) Tetso Kumazawa, Makoto Shimaoka, Kazuyuki Fukuda: "Moisture Absorbency of<br />

Optical Components Resin Adhesive" Journal of Japan Institute of Electronics<br />

Packaging, Vol.4, No.7, p.621- 624, 2001<br />

- 11 -<br />

Espec Technology Report No20


Measuring conductivity of proton conductive membranes in the direction of thickness<br />

Report 2<br />

Measuring conductivity of proton conductive membranes in the<br />

direction of thickness<br />

Shuhua Ma, Akiko Kuse Technical Development Headquarters, Espec Corp.<br />

Zyun Siroma, Kazuaki Yasuda National Institute of Advanced Industrial Science and Technology (AIST)<br />

P<br />

roton conductive membrane is generally evaluated by measuring its<br />

conductivity along the planes of the membrane. However, in view of the<br />

possibility of this membrane exhibiting anisotropy in the direction of<br />

membrane thickness compared to measuring along the longitudinal and<br />

transversal planes, the need to measure its conductivity in the direction of<br />

thickness has recently been receiving greater attention. The research work<br />

for this report is aimed at finding a way to stably and precisely measure the<br />

conductivity of a Nafion ®1) membrane in the direction of thickness.<br />

Measurements can be conducted with either 2- or 4-probe methods, but<br />

measuring with 2 probes is much easier than with 4, and this method yields<br />

more stable results as fewer inconsistencies occur with multiple specimens.<br />

This report presents the results with the 2-probe method for membrane<br />

conductivity measurements with an emphasis on the effect of interface<br />

complexity between membrane and electrodes and the feasibility of using<br />

this method for measurements.<br />

1<br />

Polymer electrolyte membrane fuel cells (PEFCs) are promising energy systems for use<br />

as automotive power supplies and for stationary as well as portable applications, due to<br />

their low operating temperature, high energy density, and acceptable levels of<br />

miniaturization. Since it is one of the most important criteria, proton conductivity is<br />

always used to evaluate the practicability of newly-developed membranes as well as the<br />

cell performance of the perfluorosulfonic acid (PFSA) polymer membrane often used with<br />

PEFC. 2)<br />

Introduction<br />

Compared to the conductivity in the direction of thickness, the resistance measured in<br />

along the plane reaches as high as 1000Ω, which features a large cell constant *1 (L/A in<br />

σ=L/(R·A)). The four-probe method *2 yields narrower data dispersion and smaller<br />

relative errors, thus this method is commonly used to measure the proton conductivity of<br />

the PFSA membrane *3 along the plane.<br />

- 12 -<br />

Espec Technology Report No20


Measuring conductivity of proton conductive membranes in the direction of thickness<br />

However, it is highly likely that treatments the membrane undergoes in the<br />

manufacturing and processing processes, such as stretching and hot-press, will change<br />

not only its crystalline structure and dimensional stability in the longitudinal, transverse,<br />

and thickness directions but also exert some influence on its proton conductivity. There<br />

is a high probability of anisotropy3) in the proton conductivity of the membrane. On the<br />

other hand, PFSA membranes are being used in the direction of thickness for the solid<br />

polymer electrolyte fuel cells, and an anisotropically conductive membrane that was<br />

newly-developed must also be evaluated in various directions. Therefore, a reliable<br />

measuring technique with high stability, reproducibility and accuracy is required to<br />

evaluate proton conductivity in the direction of thickness of the membrane. The research<br />

for this report focuses on developing a stable and precise method of measuring<br />

conductivity in the direction of thickness for the proton-conductive polymer electrolyte<br />

membrane. 4)<br />

Measurements in the direction of thickness can be conducted with 2-probe *4 and<br />

4-probe methods, but measuring with two probes is much easier than with four, and<br />

results are more stable as there are fewer inconsistencies with multiple specimens. This<br />

report presents the results obtained using the 2-probe method for conductivity<br />

measurements of ion exchange membranes.<br />

2<br />

Experimental method<br />

2-1 Equipment and materials<br />

Table 1 lists the equipment and materials used in this research.<br />

Table 1 Equipment and materials<br />

Equipment/materials Manufacturer<br />

Impedance gain/phase<br />

analyzer<br />

- 13 -<br />

Model/registered<br />

product name<br />

Solartron Instruments SI 1260<br />

Electrochemical interface Solartron Instruments SI 1287<br />

Temperature & humidity<br />

chamber<br />

Ion exchange membrane<br />

ESPEC Corporation PL-1KPH<br />

E. I. du Pont de Nemours<br />

and Company<br />

Nafion ® 117<br />

Espec Technology Report No20


Measuring conductivity of proton conductive membranes in the direction of thickness<br />

2-2 Specimen preparation<br />

MEA specimens were made by hot-pressing electrodes to a Nafion ® 117 membrane. In a<br />

preliminary test, measurements were made with two kinds of MEAs. One type of MEA<br />

specimen was produced by hot-pressing two Pt foil electrodes, coated with Nafion ®<br />

solution on one side each, to a membrane. The other MEA specimen was produced by<br />

hot-pressing two Pt foil electrodes to a membrane without using the Nafion ® coatings.<br />

Results showed good reproducibility with the Nafion ® -coated specimen, therefore, in this<br />

report specimens were prepared by coating a Nafion ® solution onto one surface of the<br />

electrodes for voltage impression unless otherwise specified.<br />

For 2-probe measurements in the direction of thickness, specimens were prepared by<br />

hot-pressing a Nafion ® membrane sandwiched into electrodes consisting of two pieces of<br />

metal sheets (5 mm x 5 mm x 10 to 20µm) or carbon papers (5 mm x 5 mm x 190µm)<br />

situated opposite each other. On one face of the metal sheets, a coating was applied with<br />

5 µl of 5 wt. % Nafion ® dispersion solution in lower aliphatic alcohols followed by vacuum<br />

drying one hour at room temperature. No coating was used on the carbon paper<br />

electrodes. Photo 1 shows the configuration of the membrane/electrode assembly<br />

(MEA *5 ) used in this report for the 2-probe measurements in the direction of thickness.<br />

The assembly is made of platinized Pt black sheets and Nafion ® 117 membrane.<br />

Photo.1 MEA of Pt black/Nafion ® 117 for 2-probe measurements in<br />

the direction of thickness<br />

For 4-probe measurements in the direction of thickness, the specimens were prepared<br />

by sandwiching and hot-pressing platinum wire electrodes between three Nafion ®<br />

membranes and then, as with the specimens for the 2-probe measurements,<br />

hot-pressing metal sheets that had been coated with Nafion ® solution and vacuum-dried<br />

onto both outside faces of the assembly.<br />

- 14 -<br />

Espec Technology Report No20


Measuring conductivity of proton conductive membranes in the direction of thickness<br />

Since 4-probe measurements in the surface direction obtained results with better<br />

reproducibility, these measurements were used as comparison reference against the<br />

measurements in the direction of thickness of the membrane. The specimens for 4-probe<br />

surface direction measurements were prepared by press-fitting metal sheets to both<br />

ends of the Nafion ® membrane and vertically piercing into the membrane near the center<br />

with platinum wires.<br />

Fig. 1 (a) and (b) respectively show schematics of the specimens for the 2-probe and<br />

4-probe measurements in the direction of thickness, while (c) shows the same for the<br />

4-probe surface direction measurements.<br />

Fig.1 Sample arrangements for (a) the 2-probe method, (b) the 4-probe<br />

method in the direction of thickness, and (c) the 4-probe method in<br />

the surface direction<br />

2-3 Conductivity Measurements<br />

A specimen fixed to a measuring cell was placed inside a temperature and humidity<br />

chamber under constant temperature and humidity (80°C, 30 to 90% rh). AC impedance<br />

measurements were taken using a computer-controlled Solartron Instruments model<br />

1260 impedance gain/phase analyzer and a computer-controlled 1287 electrochemical<br />

interface, and Cole-Cole (Z’-Z’’) and Bode (log|Z|-log Frequency and theta-log<br />

Frequency) plots were obtained. The frequency limits of the sinusoidal signals were<br />

typically set between 5 MHz and 0.01 Hz, with an oscillation of 10 mV. Assuming a circuit<br />

equivalent to the one shown in Fig.3, a best-fitting curve was overlaid onto the<br />

measurements taken by the 2-probe method. Conductivity was calculated from the<br />

obtained membrane resistance, Rbulk, using the following formula.<br />

…(1)<br />

Where σ is conductivity (Scm-1 ), L is membrane thickness (cm), A is electrode area<br />

(cm2 ), and R is resistance (Ω).<br />

- 15 -<br />

Espec Technology Report No20


Measuring conductivity of proton conductive membranes in the direction of thickness<br />

Equipment connection for the impedance gain/phase analyzer (IGPA), the<br />

electrochemical interface (EI) and the membrane/electrode assembly (MEA) was shown<br />

in Fig. 2 for 2-probe conductivity measurements used in this report.<br />

3<br />

Fig.2 Connections for impedance measured by the 2-probe method, with an<br />

IGPA in combination with potentiostat/galvanostat (electrochemical<br />

interface) mode.<br />

Results and observations<br />

3-1 Humidity dependency of resistance and capacity components of impedance<br />

In the Cole-Cole plot obtained from the 2-probe measurements, two loops appeared.<br />

They were named loop 1 and loop 2 in order of descending frequency and were treated as<br />

RY parallel circuits. The resistance and capacity components obtained from the fit were<br />

R1, R2, Y1 and Y2 (Y is a constant phase element and substituted for the equivalent<br />

capacity component in the fitting process). Fig. 3 shows a diagram of the equivalent<br />

circuit.<br />

Fig.3 Equivalent circuit for the membrane/electrode interface studied<br />

- 16 -<br />

Espec Technology Report No20


Measuring conductivity of proton conductive membranes in the direction of thickness<br />

Measurements were taken at an ambient temperature of 80°C using 4 types of<br />

electrodes made of gold, platinum, platinum black and carbon paper. Fig. 4 shows the<br />

humidity dependency of Rbulk (membrane resistance), R1, Y1, R2, and Y2 using the various<br />

electrode materials.<br />

As ambient relative humidity during measuring increased, Rbulk, R1, and R2 decreased.<br />

This phenomenon indicates that the conductivity of proton-conductive polymer materials<br />

such as Nafion ® depend on their water content. In particular, minimum resistance was<br />

obtained for R1 and R2 when using the platinum black electrode with higher active<br />

surface area, suggesting that both loop 1 and loop 2 with R/Y parallel connections are<br />

strongly correlated to the interface between membrane and electrode. With capacitance<br />

components of Y1 and Y2, regular increases in electrical capacity were found to<br />

correspond to increases in ambient humidity. Increases in this electrical capacity can be<br />

considered to result from improved contact between membrane and electrode concurrent<br />

to the hygroscopic swelling of the moisture-absorbent membrane. Types and surface<br />

morphology of electrode materials also notably affect interface resistance and capacity<br />

due to their varied surface area and differences in membrane contact. However, with Rbulk<br />

membrane resistance, equivalent measurement values have been obtained for various<br />

electrode materials with no major influence based on material types found. Therefore, it<br />

can be concluded that membrane resistance (Rbulk) can be separated from interface<br />

elements (R1, Y1, R2, and Y2) regardless of electrode materials used, since the<br />

multi-layer complexity of contact of the interface between membrane and electrodes,<br />

e.g., multiple semicircles in Cole-Cole plot, can be removed by equivalent circuit fitting.<br />

- 17 -<br />

Espec Technology Report No20


Measuring conductivity of proton conductive membranes in the direction of thickness<br />

Fig. 4 Dependence on relative humidity of various electric elements in<br />

equivalent circuits at 80°C<br />

- 18 -<br />

Espec Technology Report No20


Measuring conductivity of proton conductive membranes in the direction of thickness<br />

3-2 Conductivity<br />

Conductivity was calculated using Rbulk from Fig. 4 (a) and formula 1. Fig. 5 shows the<br />

conductivity values measured at an ambient temperature of 80°C and various humidity<br />

levels. For comparison, the results from 4-probe measurements in surface direction were<br />

also plotted. As shown in Fig. 5, conductivity results using 2-probe measurements in the<br />

direction of thickness were similar to those using 4-probe measurements in the surface<br />

direction for all electrode materials, demonstrating the validity of using the 2-probe<br />

method in the direction of thickness.<br />

4<br />

Fig. 5 Comparison of conductivity results at 80°C using the 2-probe<br />

Method in the direction of thickness and the 4-probe method in<br />

the surface direction.<br />

Conclusions<br />

Conductivity of Nafion ® membranes in the direction of thickness was measured using the<br />

2-probe AC impedance method. These experiments confirm that equivalent circuit fitting<br />

can separate membrane resistance from the interface components. Moreover, good<br />

contact at the interface between the membrane and electrode can be attained by coating<br />

the electrode with Nafion ® solution, and conductivity results are similar to results using<br />

4-probe measurements in the surface direction. These experiments demonstrate the<br />

validity and feasibility of using the 2-probe method for measuring in the direction of<br />

thickness.<br />

- 19 -<br />

Espec Technology Report No20


Measuring conductivity of proton conductive membranes in the direction of thickness<br />

[Terminology]<br />

*1.Cell constant<br />

Typically, electrical conductivity of a material can be expressed as<br />

σ=L/(A·R)=k/R, where L is the length (cm) of the material in electronic flow, A is<br />

the sectional area (cm2 ) across the flow of the material, R is the measured resistance<br />

(Ω), and k=L/A, the proportionality factor, is called the cell constant. The electrical<br />

conductivity of the material is in direct proportion to the reciprocal of the measured<br />

resistance between the electrodes by the scale factor, k, which represents the<br />

influence of the dimensions of the measuring cell.<br />

*2.Conductivity measurement using the 4-probe method<br />

As one method for measuring the electrical conductivity of materials, the 4-probe<br />

method possesses much higher measurement precision than the 2-probe method.<br />

Two terminals are used to conduct a current through the sample, and another two<br />

terminals measure the potential drop across the sample.<br />

*3.Proton-conductive membrane<br />

When potential difference exists in a conductor, electrical charges move in the<br />

direction required to weaken the difference. The property of this conductor is called<br />

its electrical conduction. When protons exist in the conductor as the main current<br />

carriers, the material is referred to as proton conduction, and the quality or power of<br />

the conduction is called proton conductivity. Some membrane materials, typically<br />

consisting of such as inorganic compounds of ceramics and/or glass, organic<br />

polymer compounds, and inorganic/organic hybrid materials, exhibit high H + ion<br />

conduction. Proton exchange membranes based on fluorinated polymers as typified<br />

by Nafion ® have been widely used in solid polymer electrolyte fuel cells (PEFCs) due<br />

to their high proton conductivity (to 0.1 Scm-1 ) and chemical stability.<br />

*4.Conductivity measurement using the 2-probe method<br />

As the simplest and most straightforward method for measuring electrical<br />

conductivity, the 2-probe method uses only two terminals that share the functions<br />

of both introduction of current (I) and measurement of voltage (V) across the<br />

sample. The electrical conductivity of a specimen can be calculated with the formula<br />

of σ=(I·L)/(V·A), provided that sectional area (A) and length (L) of the specimen are<br />

measured.<br />

*5.Membrane electrode assembly (MEA)<br />

An electrode layer composed of platinum black or platinum-supporting carbon and a<br />

porous supporting collector layer composed of carbon paper or carbon cloth<br />

arranged in succession on both sides of a cation exchange membrane, with the<br />

assembly unified by hot-pressing, is called a membrane electrode assembly (MEA).<br />

[Bibliography]<br />

1)http://www.fuelcells.dupont.com/<br />

2)Y. Sone, et al., J. Electrochem. Soc., 143, p.1254, 1996<br />

3)K. M. Cable et al., Chem. Mater., 7, p.1601, 1995<br />

4)A. Kuse, S. Ma, A. Mizugaki, H. Okuda, Z. Siroma, T. Ioroi, K. Yasuda, Y. Miyazaki;<br />

11th FCDIC Fuel Cell Symposium Proceedings, p.262, 2004<br />

- 20 -<br />

Espec Technology Report No20


New product focus: Ultra View Temperature (& Humidity) Chamber<br />

Topic 1<br />

New product focus: Ultra View Temperature (& Humidity) Chamber<br />

Toshimi Ishida,<br />

Takehiko Umehara,<br />

1<br />

Introduction<br />

Environmental Test Business Headquarters, Business Control Department,<br />

Product Planning Group<br />

Environmental Test Business Headquarters, Development & Design Department,<br />

Product Development Group<br />

The Ultra View Temperature (& Humidity) Chamber is based on the overwhelmingly<br />

popular Espec Platinous K series of environmental test chambers that has become<br />

established as our flagship product line. The new chambers are equipped with large glass<br />

viewing windows that enable the user to visually inspect the condition of specimens<br />

during tests. We are pleased to offer these products that we have developed to meet this<br />

basic need of our customers.<br />

When large viewing glass windows were provided on temperature and humidity<br />

chambers in the past, the design imposed limits on product performance, but this new<br />

chamber utilizes multilayer deposit metal electro-coated (EC) glass panes, enabling these<br />

models to maintain performance at the highest level.<br />

Potential market applications for these chambers include testing a wide variety of<br />

products such as automotive parts, household appliances, display devices ranging from<br />

cellular telephones to LCD monitors, and all types of information technology equipment.<br />

Display devices in particular are now being rushed to market as quickly as possible.<br />

Providing the ability to visually confirm the changes induced by temperature and humidity<br />

to these products fills a basic need of our customers for visual observation and inspection.<br />

Naturally, this advantage is not limited to display devices, but can also be applied to a<br />

wide range of product testing.<br />

Photo 1 Ultra View Temperature (& Humidity) Chamber<br />

- 21 -<br />

Espec Technology Report No20


New product focus: Ultra View Temperature (& Humidity) Chamber<br />

2<br />

Product features<br />

The features offered with these new chambers include full visibility from a widely<br />

expanded viewing area, anti-fogging viewing window panes, markedly improved<br />

performance, improved reliability of the viewing glass, and greatly improved ease of use.<br />

2-1 Full visibility<br />

The glass viewing windows provide full visibility from a widely expanded viewing area,<br />

offering a better view of the chamber interior and maintaining adequate light.<br />

Table 1 Viewing window effective size<br />

New product Established Espec products<br />

Type 2 470×720 310×650<br />

Type 3 570×820 410×750<br />

Type 4 970×970 810×900<br />

Effective viewing dimensions W×H (mm)<br />

These new chambers use twin type fluorescent lighting attached to the upper section of<br />

the chamber door, maintaining good lighting inside the test area. Conventional halogen<br />

lighting gives off a yellow hue that provides an unnatural tint to the specimens from the<br />

lighting, but the twin type fluorescent lighting utilized in the new test chamber makes it<br />

possible to reproduce natural colors. As an additional benefit, replacement parts can be<br />

obtained at reasonable prices.<br />

Table 2 Twin type fluorescent bulbs<br />

(1 bulb for types 2 and 3; 2 bulbs for type 4)<br />

Type 3 Type 4<br />

Lighting at the center<br />

of the chamber<br />

650 lux 1000 lux<br />

<br />

In Japan, domestic regulations for safety and health require businesses to provide the<br />

following lighting levels for workers in the workplace (excluding special types of work).<br />

Table 3 Lighting and illumination standards<br />

Workplace Standard<br />

Fine work 300 lux min.<br />

Normal work 150 lux min.<br />

Simple rough work 70 lux min.<br />

- 22 -<br />

Espec Technology Report No20


New product focus: Ultra View Temperature (& Humidity) Chamber<br />

2-2 Anti-fogging viewing window panes<br />

Environmental test chamber not only requires interior lighting and the effective visibility<br />

noted on the previous page, the chamber must also prevent the glass panes from fogging<br />

up due to the temperature and humidity conditions inside the chamber. Fogging occurs<br />

when the moisture in the air condenses on the surface of the glass. The conventional<br />

method of preventing fogging was to install a heater to warm the surface of the glass, but<br />

this approach required maintaining the glass surface temperature above the dew-point<br />

temperature, which was not economical. Also, during tests using such conditions as high<br />

temperature and low humidity, a heater is not required to maintain the glass surface<br />

temperature above the dew-point temperature. These new chambers prevent fogging on<br />

the glass surface using a heater control inside the glass, so instead of merely applying<br />

constant heat to the glass, only the minimum amount of heat required is used, thus<br />

conserving energy. (Patent pending)<br />

Glass using conventional heat-reflecting film or incorporating heating wires required the<br />

chamber design to incorporate upper and lower heat limits that were suited to the<br />

thermal limits of the glass panes. When reach-in ports were added to provide a means of<br />

operating the specimens, the glass surface in the vicinity of the reach-in ports tended to<br />

fog up, and localized hot spots occurred. This fogging was caused by not being able to<br />

place heaters near the reach-in ports (due to the processing on the glass for the ports) so<br />

that the heater current did not flow near the reach-in ports, resulting in a difference in<br />

current density in the vicinity of the reach-in ports. These new chambers are designed so<br />

that the current density is the same in all areas of the glass, including the areas around<br />

the reach-in ports, with no unevenness in current. Even when reach-in ports must be<br />

provided, there is no fogging on the surface of the glass, and the specimens can be clearly<br />

observed and operated. (Fig.1) (Patent pending)<br />

<br />

Fig.1 Current flow with viewing window reach-in ports in glass doors<br />

- 23 -<br />

Espec Technology Report No20


New product focus: Ultra View Temperature (& Humidity) Chamber<br />

2-3 Markedly improved performance<br />

Using conventional heat-reflecting film or incorporating heating wires in the glass panes<br />

required design limits on the performance of the chambers, but by utilizing glass<br />

reinforced with layers of deposit metal film, performance can be markedly upgraded. This<br />

design permits a wide temperature range, from –40°C to +120°C.<br />

Table 4 Comparison of lowest and highest achievable temperatures<br />

Lowest achievable emperature Highest achievable temperature<br />

New chambers -40°C *1 +120°C *2<br />

Established chambers -20°C to -35°C +80°C to +100°C<br />

*1 This performance table conforms to JTM K01-1998.<br />

*2 With the optional “viewing window reach-in ports”, the limit is +100°C.<br />

Expanding this temperature range makes it possible to apply the following types of test<br />

conditions as well.<br />

<br />

(1)LCD device environmental tests<br />

Storage (at high temperature) test: +30 to +100°C<br />

Storage (at low temperature) test*: -50 to 0°C<br />

Damp heat, steady state test: +40°C, 93%rh to +85°C, 93%rh; 85°C, 85%rh<br />

Composite temperature/humidity cyclic test: +25°C, 93%rh to +65°C, 93%rh;<br />

-10°C<br />

Standards: IEC61747-5 (JIS C60068-2-38), EIAJ ED-2531A<br />

(2)Automotive parts environmental tests<br />

High Temperature, Low Temperature Test: +120°C to –40°C<br />

High Temperature Exposure Test: +120°C<br />

Low Temperature Exposure Test: -30°C<br />

Standards: JIS D 0204, 0208<br />

(3)PDP environmental tests<br />

High Temperature (storage): +30 to +100°C<br />

Low Temperature (storage)*: -50 to 0°C<br />

High Temperature, High Humidity (constant): +40 to +60°C, 85% or 93%rh<br />

Low Temperature Operation: -20 to 0°C<br />

(*The Ultra View Temperature (& Humidity) Chamber is compatible down to<br />

-40°C.)<br />

To meet the demand for these standards, Espec has utilized glass reinforced with deposit<br />

metal, broadly extending the temperature range from –40°C to +120°C.<br />

The new chambers offer a greatly extended range of control for humidity as well as for<br />

temperature.<br />

- 24 -<br />

Espec Technology Report No20


New product focus: Ultra View Temperature (& Humidity) Chamber<br />

Fig.2 Temperature and humidity control range<br />

The new chambers also offer improvement in the temperature heat-up time and<br />

pull-down time.<br />

Table 5 Comparison of temperature heat-up time and pull-down time<br />

New chambers<br />

Established<br />

chambers<br />

Temperature heat-up time Temperature pull-down time<br />

50 minute max.<br />

(-40°C to +120°C)<br />

100 minute max.<br />

(-35°C to +100°C)<br />

- 25 -<br />

60 minute max.<br />

(+20°C to –40°C)<br />

90 minute max.<br />

(+20°C to –35°C)<br />

2-4 Improved reliability of the viewing window glass<br />

Glass using heat reflective film suffers deterioration of the film with long-term use,<br />

resulting in impaired visibility. Glass incorporating heating wires can suffer wire breakage<br />

leading to fogging of the glass surface. Utilizing glass reinforced with deposit metal film<br />

has eliminated these defects, providing solidly improved reliability.<br />

2-5 Greatly improved ease of use<br />

Not only responding to the need for visual inspection, we at Espec have responded to the<br />

desire to touch, operate, and measure the specimens by offering optional “reach-in ports”<br />

on the viewing window (one each on the right and left sides, for a total of two ports).<br />

Conventional reach-in ports had screw-on covers, requiring extra time and effort to open<br />

and close. There was also a danger of scratching the glass around the reach-in ports when<br />

opening and closing the screw-on covers, and finding where the covers were put after<br />

they had been removed could cause problems for the operator.<br />

These new chambers have incorporated one-touch swing covers for the reach-in ports.<br />

These covers are easy to open and close, and the operator never has to look for the<br />

covers. (Photo 2)<br />

Espec Technology Report No20


New product focus: Ultra View Temperature (& Humidity) Chamber<br />

<br />

Photo 2 Opening and closing the reach-in port on the viewing window<br />

- 26 -<br />

Espec Technology Report No20


New product focus: Ultra View Temperature (& Humidity) Chamber<br />

When the job requires continual work using the hands inside the reach-in ports, the<br />

releasing hinges allow for completely removing the covers.<br />

→ →<br />

Photo 3 Removing the reach-in port covers on the viewing window<br />

Interior lighting (fluorescent) is built into the upper section of the door. The bulbs can be<br />

easily replaced with no halt in testing. A dew condensation tray is also built into the lower<br />

section of the door to prevent water dripping onto the floor when the door is opened.<br />

Photo 4 Removing the interior lighting cover<br />

- 27 -<br />

Espec Technology Report No20


New product focus: Ultra View Temperature (& Humidity) Chamber<br />

3<br />

Table 6 shows the main specifications of the new chambers.<br />

Table 6 Main specifications<br />

Model PWL-2KP PWL-3KP PWL-4KP PWU-2KP PWU-3KP PWU-4KP<br />

Power supply<br />

Temperature (& humidity)<br />

control system<br />

- 28 -<br />

200V AC 3Ф 3W 50/60Hz,<br />

220V AC 3Ф 3W 60Hz,<br />

380V AC 3Ф 4W 50 Hz<br />

Balanced temperature and humidity<br />

Balanced temperature control (BTC)<br />

control (BTHC)<br />

Working temperature range 0 to +40°C<br />

Temperature range -40 to +120°C<br />

Humidity range 20 to 98%rh ----------<br />

Temperature<br />

-40 to<br />

+100°C<br />

±0.3°C<br />

fluctuation +100.1 to<br />

+120°C<br />

±0.5°C<br />

Humidity fluctuation ±2.5%rh ----------<br />

Performance<br />

*1<br />

Temperature<br />

-40 to<br />

+100°C<br />

±0.5°C ±1.0°C ±0.5°C ±1.0°C<br />

uniformity +100.1 to<br />

+120°C<br />

±0.75°C ±1.5°C ±0.75°C ±1.5°C<br />

Humidity uniformity ±3.0%rh ±5.0%rh ----------<br />

Temperature<br />

heat-up time<br />

Within 50 min from -40 to +120°C<br />

Temperature<br />

pull-down time<br />

Within 60 min from +20 to -40°C<br />

Effective viewing dimensions<br />

(W×H mm)<br />

Dimension<br />

*2<br />

Specifications<br />

Test area dimensions<br />

(W×H×Dmm)<br />

Outer dimensions<br />

(W×H×D mm)<br />

470x720 570x820 970x970 470x720 570x820 970x970<br />

500×<br />

705×<br />

600<br />

910×<br />

1590×<br />

1039<br />

600×<br />

850×<br />

800<br />

1010×<br />

1690×<br />

1239<br />

1000×<br />

1000×<br />

800<br />

1410×<br />

1970×<br />

1239<br />

500×<br />

705×<br />

600<br />

910×<br />

1590×<br />

1039<br />

600×<br />

850×<br />

800<br />

1010×<br />

1690×<br />

1239<br />

1000×<br />

1000×<br />

800<br />

1410×<br />

1970×<br />

1239<br />

Loading capacity (L) 225 408 800 225 408 800<br />

Weight (kg) 310 370 560 300 360 550<br />

* 1:・Performance values are given for +23°C ambient temperature and no specimens<br />

inside chamber.<br />

・Temperature/Humidity fluctuation and uniformity are based on JTM (Standard of<br />

Testing Machinery Association of Japan) K 01-1998.<br />

・Loading capacity is given for an effective area up to 1/6 the distance from walls in<br />

all direction.<br />

* 2: Excluding projections.<br />

Espec Technology Report No20


New product focus: Ultra View Temperature (& Humidity) Chamber<br />

4<br />

Conclusion<br />

The new Ultra View Temperature (& Humidity) Chamber was designed to respond to the<br />

basic need during environmental tests and evaluation tests to see, touch, operate, and<br />

measure the specimens being tested.<br />

To meet the special needs presented by the current trend of increasingly complex<br />

functions combined with miniaturization, finer tolerances, lighter weight, and the<br />

environmentally friendly materials required by current products, all of which are impacted<br />

by the increasing demand for speeding up the product development cycle, we at Espec<br />

are committed to meeting our customers’ needs for all kinds of tests needed for<br />

development, evaluation and reliability for all our customers’ new products.<br />

・For further information<br />

Please feel free to contact the Espec International Operations Center or drop in to your<br />

nearest overseas dealer for further information or to request a catalog regarding the<br />

Ultra View Temperature (& Humidity) Chamber.<br />

- 29 -<br />

Espec Technology Report No20

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