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Experimental Thermodynamics (30 common techniques)

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Experimental Thermodynamics (30 common techniques)

Therm al analysis Calorim etry

D ifferential Scanning Calorim etry M odulated D SC

M icrocalorim etry

D ifferential Therm al A nalysis Therm al G ravim etric A nalysis

Bom b Calorim etry/Com bustion Calorim etry Colligative A nalysis

M em brane O sm om etry Vapor Pressure O sm om etry M elting point/Boiling point D ensity

A rchim edes M ethod Pynchom etry

D ensity G radient Colum n D ilatom etry

Sound Velocity Shock Com pression

Surfaces

G as A dsorption Contact A ngle Zeta Potential Phase Structure

Light, X -ray, N eutron Scattering O sm otic Com pressibility O M , SEM , TEM , A FM

X RD Chem ical M ethods

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Calorimetry

Therm al analysis Calorim etry

D ifferential Scanning Calorim etry M odulated D SC

M icrocalorim etry

D ifferential Therm al A nalysis Therm al G ravim etric A nalysis

Bom b Calorim etry/Com bustion Calorim etry

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Calorimetry

H ow to build a scanning calorim eter

W hat is needed?

O ne or Tw o A diabatic/Isolated Cells Therm ocouples, T

H eating rate, dQ /dt M ass, m

Sim plest approach and useful for very low or very high tem peratures is differential therm al analysis D TA

D TA is a sim ple design for difficult environm ents

Tw o cells heated at sam e rate and the difference in tem perature is recorded

D ifferences in heat capacity and latent heats create differences in tem peratures through transitions.

dT/dQ is m easured in the D TA dQ /dT is m easured in the D SC

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Measure the Temperature

Seebeck Effect: Thermocouple

Electrons (or holes) flow from the hot side w here they have high kinetic energy to the cold side w here they have less kinetic energy. They w ill spend m ore tim e in the cold side, som ething like condensing in the cold side. This effect is different in m agnitude for different m etals or sem iconductors. The difference in potential at the cold side betw een tw o m etals is proportional to the tem perature. (Sim ilar to therm ophoretic sam pling.)

Therm oelectric generator

Therm ally insulating Electrically conducting

Therm ocouple

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Calorimetry

Cryostat

U se liquid H e or a H e refrigerator 4.2K boiling point

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Calorimetry

dQ /dt = Cp dT/dt + DHtransitions

DQ = Cp (Tf-Ti)+ DHtransitions

Tf = Ti + (DQ – DHtransitions)/Cp

DQ = (dQ/dt) t

dT/dQ is m easured in the D TA dQ /dT is m easured in the D SC

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Calorimetry

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Experimental Thermodynamics (30 common techniques)

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