H w u i J‘ ‘\ 1' ,INHW H w ‘HIH \ \ I ‘Hil RH] WWI! '—I 1308 I Imm4> THE DEVELGPMENT OF A MHHC-D 0? TEST FOR SHOCK ABSGRBWG iii-WEACTERES'H'CS 0F FOAM-ENePLACE CUSHQGRENG MATEREALS mesés for the Degree of M. S. MECHiGAN STME UREVERSETY EDWARD ALLEN CHURCH '5} “1-3 .3. if“ “‘3 LIBRARY Michigan State University ‘5 I!!! I”!!! 1W!!! LII/(111112!!! I!!! W Nil I!!! fill)! I! w 54 41 ‘I 5 n I» ‘ 'J “; fa an.” " ,.. "" "‘"‘~‘ ugh} r: F f «1-.- "-= 3.9 - " “t" "’ o ‘ - v-l C. ‘fifi' " fl (:94 21> Wm ABSTRACT THE DEVELOPMENT OF A METHOD OF TEST FOR SHOCK ABSORBING CHARACTERISTICS OF FOAM-IN-PLACE CUSHIONING MATERIALS BY Edward Allen Church The problem of this thesis was to establish a method for determining the shock absorbing characteristics of foam— in—place cushioning materials. This was done by evalua- ting existing testing procedures used for determining dynamic cushioning characteristics of other types of cushioning materials. These materials consisted of resilient sheet and loose fill materials. Drawing on some of the adaptable segments of each procedure and dis“ carding the remainder, a new test method was specifically developed for foam—in-place cushioning materials. The developed method offers a choice of procedures which utilize an actual package with a simulated product held in place by the foam—in—place material. The package is subjected to either free fall impact shocks or to con- trolled shock inputs from a shock machine. The simulated product using an accelerometer mounted within, monitors the input shock to the simulated product. Thus the Edward Allen Church effectiveness of the foam-in-place cushioning material can be evaluated. THE DEVELOPMENT OF A METHOD OF TEST FOR SHOCK ABSORBING CHARACTERISTICS OF FOAM-IN-PLACE CUSHIONING MATERIALS BY Edward Allen Church A THESIS Submitted to Michigan State University in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE School of Packaging 1972 ACKNOWLEDGMENTS For his outstanding direction and helpful guidance I would like to give my sincere thanks to Mr. Stephen R. Pierce, my major professor at Michigan State University. My profound appreciation goes to INSTAPAK CORPORA- TION for providing not only the equipment and material but their knowledge and experience in the field of foam— in-place. I would also like to thank LANSMONT CORPORATION for its understanding in allowing me time to conduct my thesis research.' I would like to dedicate this thesis to my wife, Kay, and our son, David. ii TABLE OF CONTENTS Page ACKNOWLE DGMENTS O O O O O O C O O O O I O O i 1 LIST OF FIGURES O O O O O C O O O O O O O 0 iv INTRODUCTION . . . . . . . . . . . . . . . 1 Chapter I. APPLICATION OF EXISTING TEST METHODS . . . . 4 Part I--Platen Dr0p Test Method . . . . . 4 Part II—-Platform Drop Test Method . . . . ll Part III--Shock Machine Method - Step Velocity . . . . . . . . . . 19 II. PROPOSED TEST METHOD . . . . . . . . . 24 Proposed Method of Test for Shock Absorbing Characteristics of Foam-in—Place Cushioning Materials for Packaging Applications . . . . . . . . . . 25 III. SUMMARY AND CONCLUSIONS . . . . . . . . 42 APPENDICES o o o o o o o o o o o o o o o 44 A. Foaming System and Safety Precautions . . 45 B. Monitoring System Used to RecOrd Peak Acceleration and Impact Velocities . . . 49 BIBLIOGRAPHY . . . . . . . . . . . . . . . 51 iii LIST OF FIGURES Figure Page 1. Platen Drop Tester . . . . . . . . . . 6 2. Platen Drop Test Specimens . . . . . . . 9 3. Foaming Fixture for Platen Specimens . . . . lO 4. Comparison of Test Results of Three Tes t Me thOdS O O I O O O O O O O O 12 5. Plywood Outer Box . . . . . . . . . . 15 6. Foaming Fixture for Drop Test and Shock Machine Specimens . . . . . . . . . . l7 7. Platform DrOp Tester . . . . . . . . . 18 8. Test Results Comparing Plywood and Corrugated Outer Containers . . . . . . . . . . 22 9. Shock Machine Set—Up . . . . . . . . . 23' 10. Test Block Diagram . . . . . . . . . . 31 ll. Foaming Fixture Diagram . . . . . . . . 34 12. Sample Test Specimen . . . . . . . . . 36 13. Velocity Change Calculation Method . . . . . 38 iv INTRODUCTION Polyurethane materials have been known for more than a quarter of a century. Remarkable advances have been made with this material in the past few years. One of the advances in the packaging area is the polyurethane foam-in-place system. In the past, polyurethane foam has been used in packaging in sheet form (1.2 pounds per cubic foot) and has been a good cushioning medium for rela- tively light loadings (up to .5 p.s.i.). The polyurethane foam manufactured by the foam-in—place system is a low density (.5 pounds per cubic foot), semi—rigid material that can be used over a wider static stress range and is less costly. The foam-in—place urethane recently developed has been used as a dunnage and cushioning material for pack— aging. With foam—in—place urethane being used as a cushion material, the problem has arisen as to how to design the package to protect the item for a specific acceleration level. Present and potential users of this material are requesting technical cushioning data from the suppliers in the form of peak acceleration level versus statis stress loading. The problem explored in this thesis was the development of a realistic testing procedure for evaluating the dynamic cushioning characteristics of foam-in-place polyurethane foam. The approach used was to evaluate currently existing test procedures used to evaluate other types of cushioning materials and to determine their adaptability as a testing procedure for foam-in—place polyurethane foam. Three existing test methods and varia- tions of these methods were evaluated. The test methods were evaluated on the basis of correlation of data with the performance of the material in the shipping environment, and repeatability of the test results. If the test method is designed to reflect the way the material is used then the data can be used as a predictive measure for designing optimum cushioning. It is also as important to be able to reproduce the test results. When the data is reproducible and indictive of the behavior of the material in usep'a cushioned package can be designed with confidence. Before proceeding with the test methods, the foam- in-place method will be defined and briefly discussed. The urethane foam is obtained by dispensing two liquids through a dispensing device. The liquids are dispensed into a container. Then the foam begins to expand and within fifteen seconds expands one hundred times its liquid volume to an approximate density of 0.5 pounds per cubic foot. A plastic film is layed over the rising foam and the product is then centered on the foam and covered with another sheet of film. More foam is then injected to fill the container and the container is closed. The two liquids used to make the foam are crude M.D.I. isocyanate or diphenyl methane di-isocyanate and the resin or polyol part of the formulation. The resin part is made up of many chemical components. Some of these components are water, 11B type fluorocarbon "blow- ing agent" and polyhydroxy compounds used in making the urethane polymer, and minor concentrations of catalysts and surfactants. The fabricated foam is an Open fine cell material from .48 to .55 pounds per cubic foot if it is allowed to foam free, a compressive strength of normally 2 p.s.i., and a thermal conductivity (K—factor) of .26 Btu/hr. (ftz) . CHAPTER I APPLICATION OF EXISTING TEST METHODS The first chapter is a review of three existing methods currently used for evaluating the dynamic cushion characteristics of both resilient sheet and loose fill cushioning materials. These three test methods and their modifications, the procedures used and the findings of the tests are each discussed in the three parts that follow. The foam—in-place material as well as the foaming system were supplied by INSTAPAK CORPORATION. The poly“ urethane foam was used for evaluating all of the test procedures and was not meant to be used to provide any final data. A brief discussion of the foaming system is included in Appendix A. Because the monitoring system used to record data was identical for all of the test procedures, it is detailed in Appendix B. Part I--Platen Drop Test Method The first existing test method that was evaluated was the platen test method. This method has been in use for approximately ten years for the evaluation of resilient sheet or slab cushioning materials. There are two speci- fications that cover this method. One is MIL-C-26861B (USAF) and the other is ASTM 1596-64. The two methods are basically the same. The sections of the test methods that were evaluated in relation to the testing of foam-in—place urethane were the sections relating to the dynamic testing of cushions to produce peak acceleration versus statis stress data. Although this method has been found to have ‘ITU'AJv ,..\ ‘ .- 1‘." .. ' ' limitations for testing materials other than sheet mater- ial, it was thought it was worthy of investigation because of the ease of testing and the acceptance of the method. This method uses a dynamic cushion tester like the one shown in Figure l. The machine consists of a base or anvil, a dropping head platen, guide rods, and an adjust— able crosshead and release mechanism. The weight of the dropping platen is adjustable by adding weights. The anvil or base must weight at least fifty times the maximum dropping platen weight. The platen is dropped vertically and guided in a parallel manner to the base of the machine. Because all machines have a certain amount of friction present in the system, a certain impact velocity is specified which is equivalent to.a free fall drop height. This allows for standardization of impact veIOv cities between different testing laboratories. The test specimens are right square prisms with minimum dimensions of 4" x 4" x 1" thick. Larger test specimens are 1.--P1aten Drop Tester. Figure recommended. The test specimen is positioned on the base below the platen. The platen is then drOpped from a pre- determined drop height onto the cushion. The platen is dropped on the cushioning material five times with a minimum of one minute between each drop. The acceleration time data for each drOp is recorded. The acceleration data for the final four drops is averaged and that average is used as the peak acceleration at that static loading. The static loading is determined by dividing the weight of the dropping mass by the area of the cushion impaCt surface. After five to seven static loadings have been tested a dynamic cushion curve can be drawn. This curve is graphed as peak acceleration versus static loading. Once the curve has been drawn, the material can be classified according to MIL—C~268GlB. According to this specification, a material can be classified as to the grade for each of their classes. There are six classes. The classes are divisions of loading ranges. For example, class one is the very light loading range (less than 0.08 p.s.i.) and class six is the extremely heavy loading range (1.5—4.0 p.s.i.). The specification also grades a cushion. The grades refer to the peak acceleration of the material at the various loadings. For example, Grade A is very low peak acceleration (less than 20 g‘s), Grade D is high peak acceleration (less than 100 g's). The cushion curve is the final result of the testing. This method was used to test foam—in-place urethane in three different ways. The first way was to test it as a sheet material without "skins" on either side of the material. The second method of testing was with "skin" on both top and bottom of the foam. The last method was to test the material with "skin" in a corrugated tray. These three types of samples can be seen in Figure 2. The test specimens for the first method of testing were 9" x 9" x 4" thick blocks cut from the center of larger blocks of foam by means of a band saw. The speci— mens therefore had no "skin" and were not confined in any way. The data generated using this test and method of sample preparation indicates that this method is not a realistic test for the evaluation of foam-innplace. The cushioning material actually blew apart at .3 p.s.i. and above. Where in actual use this material is used at much higher loadings. The findings indicate that confinement of the foam within a container is a significant factor in its ability to effectively cushion. The test specimens for the second method of testing were 9" x 9" x 4" thick blocks of foam. These samples were made using a fixture to control a flat surface area and thickness. This fixture is shown in Figure 3. These specimens had both skin and polyethylene top and bottom. The specimens were cut on a band saw from a 10" x 10" block and therefore had no side skin or confinement when tested. The test results of this method confirm the Figure 2.--P1aten Drop Test Specimens. 10 Figure 3.--Foaming Fixture for Platen Specimens. ll findings of the first method in that the cushion holds up and performs over a wider loading because the specimens were more confined by the skin and polyethylene. However, the lack of cushion confinement on the sides of the cushion makes this an unrealistic test and lead to an early break- down of the material. FT; The test specimens for the third method were 10" x 10" x 4" thick blocks of foam confined in a corru— gated tray. These specimens were made by foaming directly into a corrugated tray. The impact surface and thickness E! were controlled by the same fixture as used in the previous method. A piece of polyethylene film was placed over the top of the foam as it was expanding. These specimens therefore had skin and polyethylene on the impacting sur— face. The results of the tests for this method further confirms the necessity for confinement during tests. The data from the three different test methods explored is shown in Figure 4. Methods one and two are graphed as only one point because beyond that p.s.i. loading the test specimens were destroyed upon impaCt before the completion of the tests. Part II--Platform Drop Test Method Drop test methods have been proposed by several groups and individuals for establishing peak acceleration versus static stress curves. All of these relate to the evaluation of loose fill materials. The drop test method is popular for two distinct reasons. The first reason is 12 .mcoeumz puma mouse mo muasmmm umma mo GOOHHmmEooul.v ousmfim A.w.m.av mmmmhm Osp4m Foam-in-Place Top Cushion Test Block Foam-in-Place Bottom Cushion < TZL-—Corrugated Box 7//////////// .V////7/Z////F]/Z//7///f/ K\\\\\\\\\\\.\\ Figure 12.--Sample Test Specimen. 37 (b) Test Machine 1. Procedure A--Shock Test Machine (i) Calculate the required carriage velocity change from V = /§§H— where V = required velocity change in inches per second (centi- meters per second). G = the acceleration F of gravity in inches per second per second (centimeters per second per second).' h = the desired simulated free-fall drop height. E (ii) Following the shock machine manufac— turer's recommendations, adjust the machine to produce a shock pulse of not greater than 2 milliseconds total duration and having a velocity change equal to that calculated in paragraph 8.(b)1.(i) above.* The carriage acceleration versus time histories shall be measured by an accelerometer rigidly mounted on the carriage as close as possible to the outer container mounting position. (ii) Take care to insure that the machine holds and releases the test specimen in such a way as to produce a flataface impact of the *Velocity change equals the area under the accelera— ticul versus time pulse. This area may be obtained directly frxnn an accurate graph or trace of the pulse by use of a planimeter or equivalent technique. In those cases where the pulse shape may be described mathematically (i.e. half Silug, triangle, etc.), the area may be calculated. If it is required to "fair" or smooth the actual acceleration 38 test specimen with the dropping surface. This shall be verified either before each test series by monitoring the outputs of 4 accelerometers, one each mounted in the bottom 4 corners of a wooden container equal in size to the corrugated outer container. [K An adequate flat-face drop shall be defined g as one which produces outputs from the four accelerometers such that the maximum time lapse between the initial onset of any 2 Le outputs is less than 10 percent of the average total pulse durations. If this verification is performed prior to each test series but not for each actual test, enough trials must versus time history to obtain the correct mathematical shape prior to calculation, take care to insure that the area of the faired pulse is the same as the area of the actual pulse. Example: Figure 13 shows a velocity change calculation method which may be used if the shock pulse closely approximates a half sine shape. ’ jleration actual pulse cce / ----- faired pulse IL} time A AV 252 where AV velocity change i, ’ A peak acceleration \ of the faired pulse time duration of |<%____ T 9 the faired pulse If A is measured in G and T in milliseconds, AV = 0.245AT in./sec., or AV = 0.624AT cm/sec. '9 II Procedure 9. (a) 39 be conducted to indicate that the machine can reliably reproduce the above-defined flat-drop. Procedure A--Shock Machine Test 1. Securely fasten the properly prepared test ET specimen to the carriage of the shock test I machine. Attach the input-pulse-monitoring accelerometer to the carriage as close as L_ possible to the outer container. Properly connect and make ready the block accelera— tion and input acceleration measuring channels. Operate the machine in accordance with the manufacturer's instructions to produce the acceleration versus time pulse determined in paragraph 9. (b)l.(ii). Examine the carriage acceleration versus time history to verify that the proper pulse is being obtained. Record the following data: (i) Input pulse parameters or an actual trace or plot of the acceleration versus time curve. (ii) Peak acceleration recorded by the block accelerometer. Repeat paragraphs 9.(a)2. and 9.(a)3. for a total of 5 trials at the specified test condition. (b) Procedure B--Package Drop Machine Fe 1. 40 The maximum number of tests to be conducted with one sample of the cushioning material is 5. If more tests are to be run (i.e. at different drop heights or static loadings), new material must be used. Place the properly prepared test specimen on the machine such that it will be released to "AB—‘Z‘WTWM ~1' -‘ ‘A produce a flat-face impact with the dropping n‘ 137$]- surface. Properly connect and make ready the t- block acceleration and outer container accel- eration (if used) measuring channels. Operate the machine in accordance with the manufacturer's instructions to produce the desired free—fall drop. Insure that an adequate flat-face impact is produced. Record the following data: (i) Height of free-fall drOp (ii) Peak acceleration recorded by the block accelerometer. Repeat paragraphs 9.(b)2. and 9.(b)3. for a total of five trials at the specified test condition. The maximum number of tests to be conducted with one sample of the cushion material is five. If more tests are to be run (i.e. at different drop heights or static loadings), new material must be used. 41 Calculations 10. For each series of five trials, make the following calculations: (a) The static stress value. Static stress is defined as the weight of the test block divided by the area of its bottom surface. r- (b) The equivalent free-fall drop height (Procedure A). Report 11. The report shall include the following information: (a) The number of specimens tested, conditioning parameters, description of material, and date tested. (b) The original thickness of the cushion material layer, immediately prior to start of the test series. (c) The static stress value and the dimensions of the test block's bottom surface. (d) The equivalent or actual free-fall drop height. (e) If this test method is used to generate complete curves of peak transmitted acceleration versus static stress for a given drop height and cushion material thickness, the average of the last four (4) shall be plotted. (f) Detailed description of any deviations from the procedure as specified herein. CHAPTER III SUMMARY AND CONCLUSIONS wan-11":J This chapter offers a short summary of the problem and conclusions. The problem was one of evolving a workable and applicable method for evaluating the dynamic shock absorbv é, ing characteristics of foam-in—place cushioning materials. A proposed method of test is presented in Chapter II that allows evaluation of the dynamic cushioning characteristics of foam—in-place materials as they are being used for product protection in packaging. The method is written in a format that could be used as an industry standard. The proposed test method is a combination of Parts II and III of Chapter I of this thesis. They ful— filled the objectives of being realistic and repeatable. PartI, Platen Drop Test, was omitted because it caused Inaterial failure at very low static stress loadings which is; contrary to the actual ability of the material to perv .form1in.the real use environment. Peak acceleration versus static stress loading currves can be drawn from this procedure. They will permit 42 43 the packaging engineer to scientifically predict the amount of protection he can expect from an optimal amount of foam-in-place material. The method of testing in an actual package with a monitored test block is adaptable to evaluate all other presently used cushioning materials. This is yet another F“ step toward the final development of a single testing pro- cedure for all cushioning materials. APPENDICES 44 APPENDIX A FOAMING SYSTEM AND SAFETY PRECAUTIONS 45 FOAMING SYSTEMS AND SAFETY PRECAUTIONS The system used for foaming samples to be tested was an INSTAPAK Model 501 supplied by INSTAPAK CORPORATION F:‘ of Danbury, Connecticut. It consisted of the following pieces: Temperature control system (base heater for two canisters) Applicator gun Gun cables Two filled chemical canisters They also supplied a nitrogen regulator and two nitrogen bottles. The system is assembled by attaching the applicator gun to the cable or air lines and the other end to the two canisters. The nitrogen regulator ‘ is attached to a bottle and the pressure line is attached to the applicator gun. A pressure of 100 p.s.i. is applied to the system. Then both canisters are placed on the base heater and raised to a temperature of 1309F. The applicator gun is then filled with "INSTAPAK gun solvent" and then the system is ready for operation. The following safety precautions and health hazards are reproduced from INSTAPAK CORPORATION's technical data sheet 72-002 and should be followed. 46 47 INSTAPAK CORPORATION Technical Data Sheet Safety Precautions and Health Hazards of Instapak Packaging System Introduction As in any mechanicalvchemical industrial system, all personnel packaging with and servicing the Instapak Packaging System should be thoroughly trained and know— ledgeable of the Instapak System. A supervised training course and reading of the Instapak Instruction Manual should be minimum requirements. Nitrogen Supply The customer is responsible for the supply of nitrogen which is used as a propellent of the chemicals. Instapak will supply the nitrogen regulator which attaches to the nitrogen tank and to which the Instapak air hose attaches. Nitrogen supplied should be H.P. (high purity) dry nitrogen. (Do not use water primed nitrogen.) The nitrogen fitting should be a female, right hand fitting to properly accept the regulator supplied by Instapak. Instapak supplies a pressure relief valve to pre- vent excess pressure being allowed to flow into the chemical tanks. The pressure relief valve should never be removed from the regulator. Nitrogen size "T" tanks are normally used and these tanks should be secured properly to the wall or steel support. A dangerous situation exists if filled nitrogen tanks are handled carelessly. If the tank is dropped and the fitting is jarred loose, the 2000+ lbs. of nitrogen pressure will act as a dangerous propellent. Extreme caution should be employed when handling filled nitrogen tanks. Handling of Chemicals The Instapak System has been designed to reduce to an absolute minimum the exposure of the chemicals to the atmosphere. The Instapak chemicals are completely closed to the atmosphere during normal operation of the system, and there is never a situation where raw Component A or Component B should be exposed to the atmosphere for more than 60 seconds. 48 Care should be taken at all times to bleed off the 100 p.s.i. nitrogen before removing a manifold from one of the tanks or removing a foam gun. If there is a machine malfunction, immediately bleed and shut off the nitrogen supply. This will stop the flow of chemicals to the gun. While changing guns or chemical tanks, it is advisable to wear rubber gloves. Handling Component A (Red Container) Direct contact of Component A, isocyanate, with the skin or eyes should be avoided. If Component A comes in contact with the skin, it should be rinsed immediately . with Instapak Gun Solvent and then with soap and water. f It is possible that isocyanate can irritate the skin and g it will cause temporary discoloration of the skin. It is strongly advised that rubber or P.C.V. gloves be worn when changing chemical tanks or foam guns. The vapors of Instapak Component A do not present a health hazard. (Refer to "Precautions and Health Hazards Involved in Operation"). Handling Component B (Blue Container) Component B is light and sticky and can be washed away with soap and hot water. Component B should not irritate the skin. APPENDIX B MONITORING SYSTEM USED TO RECORD PEAK ACCELERATION AND IMPACT VELOCITIES 49 MONITORING SYSTEM USED TO RECORD PEAK ACCELERATION AND IMPACT VELOCITIES The acceleration measuring equipment consisted of a Kistler model 818 piezoelectric accelerometer and coupler. The accelerometer was mounted directly on the dropping head during the platen drop. Also for the platen drop the impact velocity of the platen was measured and calibrated to provide an equivalent 24 inch drop height. This was accomplished by using a Sanborn linear velocity transducer. For both the free fall and shock machine methods the accelerometer was attached to the base of the test blocks and was protected from the weights by means of wooden spacers. In the case of the platen and free fall drOp tests a Krohn—Hite band-pass filter was used to filter out high frequency noise. This does not affect the peak accelera— tion signal because the filter was set with the upper limit at 1000 cycles per second. This will filter out the noise of the bearings as the platen free falls. The peak accelerations were recorded on a Tektronix model 564B storage oscilloscope triggered by either a microswitch arm (platen drop and shock machine) or with a light beam device (free fall drop test). 50 BIBLIOGRAPHY 51 BIBLIOGRAPHY Sperry, C. R. Personal Communication, Instapak Corpora— tion, July 25, 1972. . "Military Specification Cushion Material, Resilient Type, General." MIL—C-26861B United States Air Force, December 29, 1970. . 1972 Annual Book of ASTM Standards. "Shock Absorbing Characteristics of Package Cushioning Materials." ASTM 1596-64, Part 15, Easton, Maryland, American Society for Testing and Materials, 1972. . "Determination of the Cushioning Properties of Loose Fill Materials." Testing Procedure used by PIRA (The Research Association for the Paper and Board, Printing and Packaging Industries). Leatherhead, England, 1972. Pierce, S. R. "Drop Test--Step Velocity Comparison." Unpublished manuscript, Michigan State University School of Packaging, 1969. . "Safety Precautions and Health Hazards of Instapak Packaging System." Instapak Corporation Technical Data Sheet, No. 72-002, 1972. 52 "‘MATT“