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Polymer Characterization

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Presentation on theme: "Polymer Characterization"— Presentation transcript:

1 Polymer Characterization

2 Topics

3 Topics Molar Mass And Molar Mass Distribution Structure And Morphology
Molecular Weight Determination Laser Light Scattering Chromatography Size Exclusion (GPC) Mass Spectroscopy Structure And Morphology Infrared Spectroscopy Nuclear Magnetic Resonance X-ray Microscopy Scanning Electron Microscopy Atomic Force Microscopy Dynamic Properties Thermal Analysis

4 References

5 References

6 References

7 References

8 References

9 References

10 References

11 References

12 Find them Collectively on one CD

13 Development of Polymers

14 Development of Polymers
Product Synthesis Concept Design Properties Fundamentals

15 Role of Polymer Characterization
Structure Synthesis Properties Characterization

16 Molecular Weight

17 Molecular Weight Effect on Properties
Limiting Value Mechanical Property Strength, Modulus, etc General Relationship sB = A - (B\Mn) DP Critical Degree of Polymerization

18 Molecular Weight Effect on Flow
General Relationship [h] = K Ma K and a are constants Viscosity Mark-Houwink-Sakurada Relation Degree of Polymerization

19 Optimization of Molecular Weight
Mechanical Property* Useful Range Viscosity Degree of Polymerization

20 Molecular Weight Distribution
Low molecular weight molecules Single Value # of Molecules Molecular Weight Synthetic Polymers # of Molecules Broad Range of Values Molecular Weight Biological Polymers Single Value # of Molecules Molecular Weight

21 Methods of Molecular Weight Determination
Number Average Molecular Weight End-group analysis determine the number of end-groups in a sample of known mass Colligative Properties most commonly osmotic pressure, but includes boiling point elevation and freezing point depression Weight Average Molecular Weight Light scattering translate the distribution of scattered light intensity created by a dissolved polymer sample into an absolute measure of weight-average MW

22 Methods of Molecular Weight Determination
Viscosity Average Molecular Weight Viscometry The viscosity of an infinitely dilute polymer solution relative to the solvent relates to molecular dimension and weight. Molecular Weight Distribution Gel permeation chromatography fractionation on the basis of chain aggregate dimension in solution.

23 Measurement of Number Average Molecular Weight
2.3.1 End-group Analysis A. Molecular weight limitation up to 50,000 B. End-group must have detectable species     a. vinyl polymer : -CH=CH2    b. ester polymer : -COOH, -OH    c. amide and urethane polymer : -NH2, -NCO    d. radioactive isotopes or UV, IR, NMR detectable functional group

24 Measurement of Number Average Molecular Weight
2 x 1000 x sample wt Mn = C. meq COOH + meq OH D. Requirement for end group analysis    1. The method cannot be applied to branched polymers. 2. In a linear polymer there are twice as many end of the chain and groups as polymer molecules. 3. If having different end group, the number of detected end group       is average molecular weight. 4. End group analysis could be applied for polymerization mechanism identified E. High solution viscosity and low solubility : Mn = 5,000 ~ 10,000

25 ? 1: Find a procedure for End group Analysis for one kind of Polymer

26 Colligative properties
Properties determined by the number of particles in solution rather than the type of particles. Vapour pressure lowering Freezing point depression Boiling point elevation Osmotic pressure

27 How Vapor Pressure Lowering Occurs
Solute particles take up space in a solution. Solute particles on surface decrease number of solvent particles on the surface. Less solvent particles can evaporate which lowers the vapor pressure of a liquid.

28 Vapor Pressures of Pure Water and a Water Solution
The vapor pressure of water over pure water is greater than the vapor pressure of water over an aqueous solution containing a nonvolatile solute. Solute particles take up surface area and lower the vapor pressure

29 Vapor Pressure Lowering
Let component A be the solvent and B the solute. solute B is nonvolatile Applying Raoult’s Law: where: PA= vapor pressure of the solvent in solution = vapor pressure of the solution PA*= vapor pressure of the pure solvent XA= mole fraction of the solvent

30 The lowering in vapor pressure,
where: = mole fraction of solute

31 Boiling Point Elevation
When a non volatile solute is added to solvent: • Vapor pressure of solvent is lowered • solution formed must be heated to higher temperature than boiling point of pure solvent to reach a vapor pressure of 1 atm. • This means that non volatile solute elevates the boiling point of the solvent which we call boiling point elevation

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35 Boiling Point Elevation
(for dilute solutions) where is the molar mass of the solvent and the molality of the solute in mol/kg

36 Boiling Point Elevation
for dilute solutions where Kb= boiling point constant or ebullioscopic constant of the solvent

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38 Boiling-point elevation (Ebulliometry)
            Tb   : boiling point elevation      H v  : the latent heats of vaporization     We use thermistor to major temperature. (1×10-4℃)     limitation of Mn : below 20,000 HvMn Tb )C=0 = RT2 + A2C ( C

39 Freezing Point Depression
Addition of a nonvolatile solute to a solution lowers the freezing point of the solution relative to the pure solvent.

40 Freezing Point Depression
(for dilute solutions) Kf= molal freezing point depression constant or cryoscopic constant

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42 Freezing-point depression (Cryoscopy)
Freezing-point depression (Cryoscopy)              Tf  : freezing-point depression,         C :  the concentration in grams per cubic centimeter         R :  gas constant         T : freezing point       Hf: the latent heats of fusion         A2 : second virial coefficient ( C Tf )C=0 = Hf Mn RT2 + A2C


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