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EMA6165-Spring-2005-EXAM2

Course: EMA 6165, Spring 2011
School: University of Florida
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PHYSICS POLYMER - Spring 2005 EMA 6165 - EXAM 2 STUDENT UFID#:______________________ (use the NEW UF ID No. ) INSTRUCTIONS: Read the entire exam carefully. Answer every question to the best of your ability, based upon the available information. State all assumptions you use in answers. SECTION I: Polymer Structures/Properties. State the polymerization mechanism, i.e., condensation, addition, ring opening.....

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PHYSICS POLYMER - Spring 2005 EMA 6165 - EXAM 2 STUDENT UFID#:______________________ (use the NEW UF ID No. ) INSTRUCTIONS: Read the entire exam carefully. Answer every question to the best of your ability, based upon the available information. State all assumptions you use in answers. SECTION I: Polymer Structures/Properties. State the polymerization mechanism, i.e., condensation, addition, ring opening.. State the relative Tg and/or Tm for each polymer (24pts) Polymer 1. poly(propylene) 2. poly(ethylene terephthalate) 3. poly(caprolactam) Nylon 6 4. poly(ethylene oxide) 5. poly(styrene) 6. poly(phenyl terepthalamide) Kevlar Polymerization Mechanism (2pt) Tg (1pt) Tm (1pt) POLYMER PHYSICS - Spring 2005 EMA 6165 - EXAM II Concepts. Answer the following statements with TRUE or FALSE. If the statement is false, state the reason(s). If you believe a statement can be made TRUE by a simple qualifier, then state it clearly. (Normally only a single word change is required.) (12 pts) 7. The retractive force of an ideal elastomer is predominantly controlled by the entropy at extension ratios below ca. 3.0 8. Single chains of an elastomer have a higher modulus for a phantom network compared to a Gaussian like network. 9. Increasing a solvent concentration in an ideal rubber reduces the recovery stress by 1/3 for a fixed temperature and elongation. 10. The entropy of a chain mixture with a solvent increases with increasing temperature above the LCST. 11. The differences in the principle recovery stress of an ideal elastomer scales directly with the square root of the product of the biaxial strains under biaxial loading conditions. 12. The osmotic pressure equals zero for conditions where the Flory interaction parameter, i.e., chi, equals . 2 POLYMER PHYSICS - Spring 2005 EMA 6165 - EXAM II II. Graphical Relationships: You must provide the appropriate equations for answering each question. You must label axes appropriately and provide appropriate units and orders of magnitude. STATE ALL ASSUMPTIONS required. SHOW ALL Equations required. It is preferred that the relationships are linearized. 13. Sketch the relationship between the Flory interaction parameter chi versus the (4pts) radius of gyration of a polymer at the theta condition. 14. Plot the relationship between intrinsic viscosity and the shift factor (4pts) 3 POLYMER PHYSICS - Spring 2005 15. Plot the Osmotic Pressure versus radius of gyration. EMA 6165 - EXAM II (4pts) 16. Plot the recovery stress of an ideal elastomer versus the root mean square radius of (4pts) gyration. 4 POLYMER PHYSICS - Spring 2005 EMA 6165 - EXAM II SECTION II: Definitions/Concepts: Give a BRIEF description for each of the following terms in the SPACE provided. 16 pts, Use equations or words or figures. 17. Extension ratio: 18. Fictive temperature: 19. Spinodal decomposition: 20. LCST: 21. Gaussian Chain: 22. Physical aging: 23. Bindoal decomposition: 24. Characteristic ratio: 5 POLYMER PHYSICS - Spring 2005 25. EMA 6165 - EXAM II SECTION III: Engineering Problems CLEARLY state any and all assumptions applied developing your the solution. Given the following information calculate the average molar mass of chains 12 pts between cross-link junctions. State all assumptions necessary. Density = 1.143 g/cm2; volume fraction of polymer in equilibrium = 0.56; Chi is estimated = 0.0082. and molar volume of 8.11 1 1005 m3 mol01 , 1 2 Gmix = RT ln (1 2 ) + 1 2 + 1 2 x 6 POLYMER PHYSICS - Spring 2005 EMA 6165 - EXAM II HONOR CODE: We, the members of the University of Florida community, pledge to hold ourselves and our peers to the highest standards of honesty and integrity. Signature:___________________________________________________________ 26. Compare, i.e., estimate the number of polymer chains that occupy the cross sectional area of one cylinder defined in the referenced paper. Use the radius of the cylinders which were generated by annealing for 60 minutes. Compare to the ideal dimensions of the poly(styrene-block-butadiene-block-styrene) using the information contained in the reference the on course web page listed as PaperEleven Hashimoto. Note that there are specific distributions provided for the configurations of the butadiene block. You will have to determine the appropriate value to calculate for the block copolymer. This paper is located on the course webpage at: http://brennan.mse.ufl.edu/dileup/ema6165/References/SBS_SB_Morphology_Macro molecules_1993_Hashimoto.pdf This is due by Friday, February 11 at 9AM. Limit response to one page. Show all work. (20 pts) 7 POLYMER PHYSICS - Spring 2005 EMA 6165 - EXAM II Rubber Elasticity: = NV kT ( 2 ) = = Thermodynamics of Mixing 2 RT 2 MC 1 ( 2 ) MC Mo RT MC H m = N 1 2 1, 2 k T 1 3 ( ) 2 ( 0 = N v kT x x 3y 2 x 0x = 0x = E 1 / 2 E 1 / 2 H m = Vm 1 + 2 (1 2 ) V V1 2 RT Mc 1/ 3 x ) 1 x 2 RT Mc 1 x 2 x f * 2 = N V RT( 2 ) * f 1 2 G mix = RT ln (1 2 ) + 1 2 + 1 2 x 1, 2 = B1 + C S E f = l T l T ,V T ,V E f + T f = l T T ,V l,V 2 (1 2 ) C 2 1 1 = 1+ 1 2 X2 RT V1 Nk S = c [ 2 2 ( x + y 2 + z 2 3 ) + (ln( x y z )) ] 2 C x (t ) = 2 C 1 2 ln(1 2 ) + 1 x 2 + 12 t a 1 c = 1 2 T Crystallization & Kinetics 4d N kT 1 P = 0 v3 * 7 R0 2G 1 1 = + 1 + 2 22 (1 2 )C X 2 = f * 2 ri 2 = N v RT 2 ( 2 ) * r0 f 1 = C V1 ( 1 2 )2 RT 1 1 = R V u T T o H V 1 f f f 1 T f = h Tm o Energy f 8 POLYMER PHYSICS - Spring 2005 EMA 6165 - EXAM II v = 2b l + 2v f ab e General Thermodynamics GI = boao nsi Q= G = Go expQ * RT *exp K * RT I D gI G = b S g aN I T 1 V V T P ,l P= 1 2g SK = = Nk i 0.5 n 1 1 V V P l ,T Chain Dimensions/Molecular Weight Tm T (t ) = 1 exp( kt n n 1 ) Physical Aging Behavior/Viscoelasticity ln t = = 05 . G n C Tm = kTC TC TC m1 mo 1 mo s (B f o )(T To ) ( f o f ) + (T To ) (B f o )(T To ) ln1 (t1 , T1 ) = ln 2 (t 2 , T2 ) ( f o f ) + (T To ) Mn = n p( r , n) = 2 l 2 3 n p ( x , y , z , n ) = 2 l 2 3 2 g r 3 2 ( ) 4 r 2 e ( 2 e 3 x 2 + y 2 + z 2 2 nl 2 3 r 2 2 nl 2 dr ) dxdydz nl 2 = = 6 6 r2 f = f o + T To f 3 ro2 ln1 (t1 , T1 ) 17.4 (T To ) = ln 2 (t 2 , T2 ) 51.6 + (T To ) = Ae i 2 Kc 1 1 16 2 r sin 2 + 2 A2 c = + 2 R M W M W 3 2 6 r 2 = nl 2 i i 8.86 (T To ) ln1 (t1 , T1 ) = ln 2 (t 2 , T2 ) 101.6 + (T To ) Vo B Vf N M N 1 + cos(180 ) 1 cos(180 ) 1 + cos (180 ) 1 + cos = nl 2 1 cos (180 ) 1 cos [ ] = 2 .5 4 3 2 R eo M 3 2 M 1 2 3 9 POLYMER PHYSICS - Spring 2005 r2 [ ] = M 3 2 M 1 2 EMA 6165 - EXAM II ln1 (t1 , T1 ) 17.4 (T To ) = ln 2 (t 2 , T2 ) 51.6 + (T To ) 3 f = f o + T To f [ ] = [ o ] 5 3 = 2Cm 1 1 M T 1 2 (t ) o e i = G= (t ) o Gf = n = K M * De = = Go P R 4 8LQ = A e E / RT = 1 + 2.5 + 14.1 2 (t ) = o cos t w = 0.5 max min = A eV/V 0 Fluid Dynamics (Rheology) Viscoelasticity and Mechanics EYoung 's = 2 G Shear (1 + ) = 3 B (1 2 ) ln t = (B f o )(T To ) ( f o f ) + (T To ) (B f o )(T To ) ln1 (t1 , T1 ) = ln 2 (t 2 , T2 ) ( f o f ) + (T To ) 8.86 (T To ) ln1 (t1 , T1 ) = ln 2 (t 2 , T2 ) 101.6 + (T To ) R 4 P Q= 8 L Wh 2 h P Q = 2 (s + 2 ) 2m * L S Dh 3 sin 2 P * QP = 12 L Dh 2 sin 2 = QP 2 (s + 2 ) h P 2m * L S 2 E h 2 & m = bulk D 2 tan D B D S 4 sin Q D = 1/2 2 D 2 Nh cos sin 10 POLYMER PHYSICS - Spring 2005 F2 P= 2 9 2 r1 r 2 2 8LQ P= R4 2 F P= 222 9 r1 r 2 P= 8LQ R4 h0 = B R DR hf x2 Bt = B 2 p vf DR = BR = X= v0 Rf R0 Z R0 yield = 0.028 ETensile F= t F0 = Re = EMA 6165 - EXAM II R0 fz Q E = 2 (1 ) G E = 2 (1 2 ) B DV R0 p Q 3 P= Q =V A = m (T )& (n 1 ) = (T ) = E = E f v f + E m vm vf v 1 = +m E Ef Em k Cp 4 h2 t cooling = Miscellaneous 8 (Tm T w ) ln 2 (T D TW ) Blow Molding 11
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Equations for Polymer Physics/ProcessingRubber Elasticity:Thermodynamics of Mixing = NV kT ( 2 )==RT 2 M C 1 ( 2 )MC Mo RT 13 ( 2 )MC( 0x = N v kT x x 3y 20 x0 x2 H m = N 1 2 1, 2 k T 12G mix = RT ln(1 2 ) + 1 2 + 1 2 x)1= x 2
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H = E + PV HE V P = + + l T, P l T, P l T, P l T, P V 10 4 for a good elastomer l =1 V V T P ,lP= 1 V V P l ,T P = T V ,lV = 0E ~ f ( l ,V ) E E dV + dldE = V l ,T l T ,V E E V E l = + l T ,P V l ,T l T , P l T
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University of Florida - EMA - 6165
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University of Florida - EMA - 6165
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University of Florida - EMA - 6165
T HE OURNAL IOLOGICALJOF BCHEMISTRYVol. 268, No. 22, Issue of August 5 , p p. 16241-16247,1993P rinted i n U .S.A.Leucine/IsoleucineNaline-bindingProtein Contractsupon Bindingof Ligand*(Received for publication, January 29, 1993, and in revised f
University of Florida - EMA - 6165
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Motions and Relaxations of Confined LiquidsSteve GranickScience, New Series, Vol. 253, No. 5026. (Sep. 20, 1991), pp. 1374-1379.Stable URL:http:/links.jstor.org/sici?sici=0036-8075%2819910920%293%3A253%3A5026%3C1374%3AMAROCL%3E2.0.CO%3B2-YScience is
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Macromolecules 2004, 37, 8098-81098098Chemical/Mechanical Analyses of Anhydride-Cured ThermosettingEpoxys: DGEBA/NMA/BDMAWei Chian and Delmar C. Timm*Department of Chemistry and Chemical Engineering, South Dakota School of Mines,Rapid City, South Da
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Macromolecules 1994,27, 5341-53495341A Neutron Reflectivity Investigation of Surface and InterfaceSegregation of Polymer Functional End GroupsJ . F. Elman,+*. D. Jobs, T.E. Long>*lland J. T. KobersteinstBInstitute of Materials Science and Department
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EMA 6165 - Polymer PhysicsStructure - Property Behavior of SemiCrystalline PolymersLecture 35Professor Anthony BrennanDepartment of Materials Science &EngineeringUniversity of Florida07/21/11EMA 6165 Polymer Physics - Lecture 341q Measuring Tm
University of Florida - EMA - 6165
Polymer Vol. 39 No. 20, pp. 4897-4903, 1998PII: S0032-3861(97)10252-XE LSEVIER~) 1998 Elsevier Science LtdP rinted in Great Britain. All rights reserved0 (132-3861/98/519.00+0.00C rystallization of polydimethylsiloxane: effecto f silica filler and