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Heat Capacity and Stability How do you define and measure the stability of nanosystems (that you can’t see) The simula:on shows that you can find the mel:ng temperature by measuring the heat capacity as a func:on of T h=p://propka.ki.ku.dk/~jhjensen/calorimetry.html 1

Calorimetry

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Page 1: Calorimetry

HeatCapacityandStability

Howdoyoudefineandmeasurethestabilityofnanosystems(thatyoucan’tsee)

Thesimula:onshowsthatyoucanfindthemel:ngtemperaturebymeasuringtheheatcapacityasafunc:onofT

h=p://propka.ki.ku.dk/~jhjensen/calorimetry.html

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Page 2: Calorimetry

‐1

‐0.8

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0

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U(e

V)

T(K)

2

Thesimula:oncomputesTasafunc:onofUHereweswitchtheaxes

Page 3: Calorimetry

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Thedataisnoisyprimarilybecauseofthefasthea:ngrateWesmoothitbyfiPngittoapolynomial(bluecurve)

Page 4: Calorimetry

0

0.0002

0.0004

0.0006

0.0008

0.001

0.0012

0.0014

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V/K)

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Fromthesmootheddata(bluecurve)wecancomputetheheatcapacity(redcurve,righty‐axis)

CV =∂U∂T

⎛⎝⎜

⎞⎠⎟V

≈U(T2 ) −U(T1)

T2 − T1

Page 5: Calorimetry

Figurefrom:h=p://dx.doi.org/10.1016/S1631‐0705(02)01326‐9Thisar:cleisalsointes:ng:h=p://dx.doi.org/10.1021/ja802389d

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Reallifeapplica:ons

Page 6: Calorimetry

Whyistheheatcapacityhighestataphasetransi:on?

Heatcapacityandenergyfluctua:ons

CV =∂U∂T

⎛⎝⎜

⎞⎠⎟V

=E − E( )2kT 2

(Page230‐231inMolecularDrivingForcesrememberthat)U = E

Thesystemchangesmostataphasetransi:onsotheenergyfluctua:onsarelargesthere

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Page 7: Calorimetry

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h=p://propka.ki.ku.dk/~jhjensen/cvandt.html 7

Page 8: Calorimetry

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Page 9: Calorimetry

0

0.0002

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0.0008

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0.0012

0.0014

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h=p://propka.ki.ku.dk/~jhjensen/cvandt.html 9

Page 10: Calorimetry

0

0.0002

0.0004

0.0006

0.0008

0.001

0.0012

0.0014

0.0016

‐1

‐0.8

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0

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0 500 1000 1500 2000 2500 3000

Cv(e

V/K)

U(e

V)

T(K)

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