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Differential Scanning Calorimetry

Introduction to DSC

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Page 1: Introduction to DSC

Differential Scanning Calorimetry

Page 2: Introduction to DSC

1

What is a DSC?

Differential: measurement of the difference in heat flow from sample and reference side

Scanning: the common operation mode is to run temperature or time scans

Calorimeter: instrument to measure heat or heat flow.

Heat flow: a transmitted power measured in mW

What is DSC?

Page 3: Introduction to DSC

2

Ice

Ts Tr

Hot Plate

Heat the hot plate from -20 °C to 30 °C,

What will happen to the ice?

How do Ts and Tr react?

How do the Ts and Tr relate to each other?

Air

DSC working principle

Page 4: Introduction to DSC

3

Timeor Tr

TemperatureTr

Ts

Tf

Time�T =Ts-Tr

0

-0.5

Tf

DSC raw signal

DSC working principle

Page 5: Introduction to DSC

4

DSC working principle

DSC raw signal,

Timeor Tr

�T =Ts-Tr

0

-0.5

Tf

Timeor Tr

Heat flow (mW)

0

-10DSC signal, Φ

Peak integral �� � �H

Φ=�T/Rth

Rth, thermal resistence of thesystem

�H

Page 6: Introduction to DSC

5

Baseline slope

Where,

m is the sample masscp is the specific heat capacity

of the sampleβ is the heating rate

Timeor Tr

Heat flow Φ(mW)

0

-10

Initial deflection

Φ

A normal DSC curve is not horizontal, its baseline shows a slope.

�⋅⋅=Φ pcm

Page 7: Introduction to DSC

6

ICTA and Anti-ICTA

ICTAC (International Confederation for Thermal Analysis and Calorimetry)

Direction of DSC signal

�������

���� ��

mW

-20

-10

0

°C120 130 140 150 160 170

�� �� �� ��� ��� ��� �

�� �� � �� �� �� ��� �� �� �� � �� �� �� �� �� �� �� �� �� �� �� �� �� �� �� �� �� �� �� ��� �� ���� ����

�������

���� ��

��

��

���� �� �� �� �� ��

�� ��� � ��� � ��� � ��� � ��

�� ��� �� �� �� ��� �� �! "�# $%�! "�# $%�! "�# $%�! "�# $%& �' () *& �' () *& �' () *& �' () * ++ ++ ,-,- ,-,-

ICTA (�T=Ts-Tr)endothermic downwards,

exothermic upwards.

Anti-ICTA (�T=Tr-Ts)endothermic upwards,

exothermic downwards.

Page 8: Introduction to DSC

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Endothermic and exothermic effects

Endothermic:

When the sample absorbs energy, the enthalpy change is said to beendothermic. Processes such as melting and vaporization are endothermic.

Exothermic:

When the sample releases energy, the process is said to be exothermic. Processes such as crystallization and oxidation are exothermic.

Page 9: Introduction to DSC

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Exothermic effect

DSC raw signal

Timeor Tr

TemperatureTr

Ts

Time

0

�T =Ts-Tr

Page 10: Introduction to DSC

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Schematic DSC curve of a polymer

1 23 4 5

6

Temperature

Hea

t flo

w

exo

endo

1. initial startup deflection; 2. glass transition; 3. crystallization; 4. melting; 5. vaporization; 6. decomposition.

Page 11: Introduction to DSC

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What is melting and crystallization?

amorphouscrystalline

Melting of Indium: 156.6 °C, -28.6 J/g (endothermic)

Crystallization of Indium: 153.5 °C, +28.6 J/g (exothermic)

Page 12: Introduction to DSC

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In: 6.18 mg10 K/min

Integral -193.95 mJ normalized -28.52 Jg -1Onset 156.58 °C

Integral 194.27 mJ normalized 28.57 Jg -1Onset 153.43 °C

mW

-10

0

10

20

°C140 145 150 155 160 165

exoexoexoexo prod 1prod 1prod 1prod 1 13.03.2006 13:58:2913.03.2006 13:58:2913.03.2006 13:58:2913.03.2006 13:58:29

SSSSTATATATARRRReeee SW 9.01 SW 9.01 SW 9.01 SW 9.01MSG2006: MarcoMSG2006: MarcoMSG2006: MarcoMSG2006: Marco

Melting and Crystallization with DSC

Page 13: Introduction to DSC

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How to evaluate melting peaks

• Pure materials:

- onset (independent of heating rate)

- ∆Hf baseline: line, integral tangential

• Impure materials:

- peak temperature (depends on β)

- ∆Hf baseline: line, tangential right - purity analysis for eutectic systems

(based on curve shape analysis)

• Polymers

- peak temperature (depends on β and m)

- ∆Hf baseline: line, spline, integral tangential

Page 14: Introduction to DSC

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amorphous solid,rigid, brittle

liquid (non polymers)rubber like (polymers)

What is glass transition?

Glass transition is cooperative molecular movement.

Glassy state Rubbery stateGlass transition

Page 15: Introduction to DSC

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The glass transition with DSC

dTdH

mcp ⋅= 1

β⋅⋅=Φ pcm

Temperature

cp

Temperature

Φex

othe

rm

Page 16: Introduction to DSC

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Chemical reaction

A chemical reaction is a process that one or more substances (reactants) are converted to one or more new chemical substances(products) with different properties. e.g. oxidation, decomposition, polymerization etc.

Chemical reactions always involve a change in energy. Depending on whether the energy is absorbed or released during the process, theycan be endothermic or exothermic.

Page 17: Introduction to DSC

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Chemical reaction

Homogeneous decomposition of dibenzoyl peroxide; peak temperature and peak shape depend on heating rate; peak area is independent of heating rate.

Page 18: Introduction to DSC

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MaterialsAdditivesPlasticizersImpuritiesFillers

ProcessingThermal treatment

Mechanical stressingShaping

Storage and use

MaterialProperties

Where to use DSC?

PolymersPharmaceuticalsChemicalsFoodCosmetics

Page 19: Introduction to DSC

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DSC

� Multiple Thermocouples increase sensitivity and reduce noise

� For Best Resolution: Low signal time constant e.g1.7 s (20-�L Al crucible, N2 gas)

� High baseline stability using chemically resistant ceramic substrate and relatively inert silver furnace

Resolution and Sensitivity

Page 20: Introduction to DSC

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Sensor technology

∆∆∆∆TSR

S R �Temperature gradients on the sensor lead to baseline deviation from zero

∆∆∆∆TR0 ∆∆∆∆TS0

S RT0

� A single sensor temperature (T0) is measured.

� Inhomogeneous temperature distribution of the sensor is not considered.

Page 21: Introduction to DSC

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� Inner ring of thermocouples measure TR and TS

� Outer ring measures sensor temperatures at reference and samples sides, TS0 and TR0

� Thermocouples act as thermal resistence, R.

TSS R

TS TR

TS0 TR0

Sensor technology

Page 22: Introduction to DSC

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� Heat flow on the sample and reference sides are separately measured

� N is the number of thermocouples (TC) per ring.FRS5 sensor (56 TC): N = 14

HSS7 sensor (120 TC): N = 30

TSS R

TS TR

TS0 TR000 RSdt

dq Φ−Φ=

�=

−=Φ

N

i i

iSiSS R

TT

1

,0,0

�=

−=Φ

N

i i

iRiRR R

TT

1

,0,0

Sensor technology

Page 23: Introduction to DSC

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Noise and sensitivity

Peak Height 137 uW

Lysozyme dissolved in 0.1 M HCl/glycinebuffer at pH = 3Heating rate 3 K/minSample Mass around 105 mg

1.7 % Lysozyme

uW100

°C50 60 70 80 90

Peak Height 6.5 uW

Step 0.69 uW

0.1 % Lysozyme

uW5

min

°C60 65 70 75 80

18 20 22 24

Page 24: Introduction to DSC

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Noise and sensitivity

Page 25: Introduction to DSC

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Resolution

Page 26: Introduction to DSC

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� How long does the system take to equilibrate?

� How fast does the signal come back to the baseline?

� Small τSignal �better resolution

ττττSignal = Rth⋅⋅⋅⋅Cs, Cs = Cpan+ Csample+ Csensor

FRS5 sensor (Rth ≈ 0.04 K/mW) & Al40 µl (50 mg)

Cpan ≈ 50 mJ/KCsample (10 mg, 1.5 J/gK) ≈ 15 mJ/K => τSignal ≈ 3 sCsensor ≈ 10 mJ/K

FRS5 sensor (Rth ≈ 0.04 K/mW) & Al20 µl (20 mg)

Cpan ≈ 20 mJ/K => τSignal ≈ 1.8 s

Signal time constant

Page 27: Introduction to DSC

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Signal time constant

How to improve τSignal?

� Cs can be strongly influenced by the choice of the pan.

Recommendations for better resolution:

-> Al20 ul pan instead of Al40 ul pan

-> Al pans instead of alumina pans

� Cs can be reduced by using smaller sample size

� τSignal can be further decreased by using He as purge gas.

Page 28: Introduction to DSC

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Cooling behavior

0 5 10 15 20 25

-150

-100

-50

0

50

100

150

200

250

Air cooled Intracooler Liquid nitrogen

Tem

pera

ture

[°C

]

Time [min]

Page 29: Introduction to DSC

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