1 / 57

Modulated Differential Scanning Calorimetry MDSC

MDSC

Ava
Download Presentation

Modulated Differential Scanning Calorimetry MDSC

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


    1. Modulated Differential Scanning Calorimetry ® (MDSC®)

    2. MDSC® Training Course Topics What is actually measured by MDSC MDSC does not measure the reversibility of transitions Understanding heat flow from DSC and MDSC experiments Calculation of MDSC signals Heat capacity calculation Optimization of MDSC experimental conditions Characterization of transitions involving a change in heat capacity (glass transition etc.) Measurement of polymer melting and crystallinity When not to use MDSC

    3. What Does MDSC® Measure? As will be shown, MDSC separates the Total heat flow of DSC into two parts based on the heat flow that does and does not respond to a changing heating rate MDSC applies a changing heating rate on top of a linear heating rate in order measure the heat flow that responds to the changing heating rate In general, only heat capacity and melting respond to the changing heating rate. The Reversing and Nonreversing signals of MDSC should never be interpreted as the measurement of reversible and nonreversible properties

    4. MDSC® Separates the Total Heat Flow Signal of DSC into Two Parts

    5. Understanding Heat Capacity and the Benefits of Being Able to Measure It Understanding Heat Capacity Heat Capacity or Specific Heat is the amount of heat required to change the temperature of a specific mass of material (no transition in structure): Heat Capacity = Specific Cp (J/g°C) x Sample Weight (g) Heat capacity is a measure of molecular motion. Heat capacity increases as molecular motion increases. Vibration – occurs below and above Tg Rotation – polymer backbone and sidechains (in and above Tg) Translation – entire polymer molecule (above Tg) Transitions in the structure of a material are important because they result in changes in heat capacity (molecular mobility) and other important physical, and sometimes chemical, properties Thermodynamic property of material (vs. heat flow). Heat flow is relative; whereas, the heat capacity is absolute

    6. Changes in Heat Capacity Indicate Significant Changes in Physical Properties

    7. Understanding Heat Capacity and the Benefits of Being Able to Measure It (cont.) Understanding the Benefits Knowledge of the baseline due to heat capacity is important for almost all DSC and MDSC measurements because all transitions must be analyzed between two points on the heat capacity baseline for accurate temperatures and heats of transition. It is often impossible to identify the heat capacity baseline in DSC data The MDSC Reversing signals (Cp and Heat Flow) provide the heat capacity baseline Although melting is primarily seen in the Reversing signal, it is a latent heat (no change in sample temperature) and is not a heat capacity component

    8. Without Knowledge of the Baseline Due to Heat Capacity, Analysis of This Epoxy is Not Possible MDSC total heat flow signal (green), or standard DSC, cannot separate Tg from cure. Figure also shows the ability of MDSC to resolve the epoxy Tg (blue) from the kinetically controlled curing crosslinking reaction (red). MDSC total heat flow signal (green), or standard DSC, cannot separate Tg from cure. Figure also shows the ability of MDSC to resolve the epoxy Tg (blue) from the kinetically controlled curing crosslinking reaction (red).

    9. Understanding the Heat Flow Signal from DSC and MDSC® Experiments For a given sample, the rate of heat flow (mW = J/sec) due to heat capacity is linearly proportional to heating rate. At a heating rate of zero, the heat flow due to heat capacity is also zero. Any heat flow detected at a zero heating rate must be due to kinetic processes ƒ(T,t) in the sample. The purpose of MDSC is to separate the total heat flow into the part that responds to heating rate and the part that responds to absolute temperature.

    10. Heat flow due to heat capacity responds linearly to heating rate

    11. Comparison of DSC and MDSC Heat Flow and Heat Capacity Signals

    12. Selecting MDSC® Mode and Type of Experiment

    13. Storing MDSC® Signals

    14. Selecting MDSC® Signals for Plotting in Universal Analysis

    15. Average & Modulated Temperature

    16. Average & Modulated Heating Rate; MDSC® Does Not Require Cooling During Modulation

    17. Signal Calculations (cont.) Reversing Heat Flow Calculated from Reversing Heat Capacity signal

    18. Calculation of MDSC® Reversing Heat Flow and Heat Capacity Signals

    19. Signal Calculations (cont.) Nonreversing Heat Flow Calculated by subtracting the Reversing Heat Flow signal from the Total Heat Flow signal Total = Reversing + Nonreversing Nonreversing = Total – Reversing

    20. Calculated MDSC® Heat Flow Signals

    21. Separation of Transitions into Modulated DSC® Signals MDSC® Data Signals

    22. Calibration Cp Calibration is independent of heating rate 0-5°C/min Cp Calibration is independent of amplitude 0-1°C Cp Calibration is dependent on period and purge gas Calibrate with period that you intend to use for subsequent runs Use purge gas that you plan to use for subsequent runs

    25. Sapphire Cp data

    26. Sapphire Cp data

    28. Cp Data Table

    29. Determining K

    30. Sapphire Cp Values

    31. Determining K @ 1 temperature

    32. Determining K(multiple temperatures)

    35. Optimization of MDSC® Experimental Conditions MDSC® controls the Heating Rate(s) applied to the sample through three experimental parameters: Average Heating Rate (°C/min) Typically less than 5°C/minute in order to get a minimum of 4-5 temperature modulations during a transition Temperature Modulation Amplitude (± °C) Typically ± 0.1 to 2°C Temperature Modulation Period (Seconds) Typically 40 – 100 seconds

    36. Optimization (cont.) Proper selection of the three experimental parameters is important in order to maximize the quality of the results. Specific recommendations for different types of transitions will be provided in later sections. In general, temperature is controlled to either provide or not provide cooling during the temperature modulation. The combination of temperature modulation amplitude and period control the range in heating rate while its average is defined by the specified heating rate.

    37. MDSC® Heat-Iso Amplitudes (no cooling/measure crystallinity)

    38. MDSC® Heat-Iso Temperature Modulation

    39. MDSC® Heat-Cool Temperature Modulation

    40. Optimization of MDSC® Conditions for Glass Transitions w/ a Q Series MDSC (heat-cool)

    41. MDSC® Analysis of the Glass Transition The following measurements will be illustrated Measurement of Tg in Complex Samples Quantitative Measurement of Amorphous Structure in Materials Quantitative Measurement of Enthalpic Recovery (Relaxation) in Aged Samples Glass transition is frequency dependent MDSC applies a frequency (Period) during the measurement and this affects the measured temperature of the Reversing signal It is necessary to do a “Frequency Correction” in order to measure absolute values of enthalpic recovery

    42. Measuring Tg in Complex Samples with MDSC® Complex samples are ones that have overlapping transitions which make it difficult to detect or measure Tg MDSC experimental conditions which provide some cooling during temperature modulation are recommended Use an underlying heating rate that is slow enough to provide 4 or more modulation cycles over the transition of interest in order to improve separation of overlapping events (resolution)

    43. Figure 25 - MDSC® of Frozen Sucrose Solution

    44. Advantage of MDSC® for Post Cure Scan MDSC total heat flow signal (green), or standard DSC, cannot separate Tg from cure. Figure also shows the ability of MDSC to resolve the epoxy Tg (blue) from the kinetically controlled curing crosslinking reaction (red). MDSC total heat flow signal (green), or standard DSC, cannot separate Tg from cure. Figure also shows the ability of MDSC to resolve the epoxy Tg (blue) from the kinetically controlled curing crosslinking reaction (red).

    45. DSC of Complex Polymer Blend

    46. MDSC® of Complex Polymer Blend

    47. Optimization of MDSC® Experimental Conditions for Analysis of Melting and Crystallinity Sample Size; 10-15mg Period 40 sec. Q Series for crimped pans 60 sec. Q Series for hermetic pans Heating Rate Slow enough to get a minimum of 4-5 cycles at half-height of the melting peaks Amplitude Use “Heat-Iso” amplitude which provides no cooling during temperature modulation (see Table) Crystallization will not be caused by a lowering of the temperature

    48. Optimization of MDSC® Conditions for Melting (cont.) Issues with Use of MDSC in Melting Region Before discussing how MDSC® can be used to analyze melting and crystallinity, it is necessary to discuss some technical issues with the measurement. Issue 1: MDSC® cannot provide a meaningful measurement on samples that have a narrow melting range (pure metals and chemicals). The reason is that the temperature of the sample cannot be modulated during melting (Figures 43-44). Issue 2: Because there are two simultaneous endothermic processes occurring during melting (heat capacity and latent heat of fusion), and because those processes respond differently to temperature modulation, the separation of the Total signal into the Reversing and Nonreversing components changes when experimental conditions are changed (Fig 45-53).

    49. MDSC® Should Not Be Used on Sharp Melting Transitions

    50. MDSC® of Water Melting/Boiling

    51. MDSC® Raw Data Signals on Polymer Blend

    52. MDSC® of 57/43 % PET/PC Blend

    53. DSC Analysis of Cycoloy C2950: Standard DSC Ramp

    54. DSC Analysis of Cycoloy C2950: MDSC Heat Cool Heat Method/ First Heat

    55. Using the TMA Q400 to Observe the Glass Transitions in Cycoloy C2950

    56. Summary MDSC® is a slow technique. Always start the analysis of a new material with standard DSC and only use MDSC if you need. Improved sensitivity Better resolution Separation of overlapping transitions Most accurate measurement of polymer crystallinity Don’t forget that MDSC can be used while cooling Optimum results require the selection of optimum experimental conditions When in doubt, ask TA Instruments for help?

    57. What if I need help? On-site training & e-Training courses - see Website Call the TA Instruments Hotline 302-427-4070 M-F 8-4:30 Eastern Time thermalsupport@tainstruments.com Call the TA Instruments Service Hotline 302-427-4050 M-F 8-4:30 Eastern Time Check out our Website www.tainstruments.com

More Related