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phase transitions and phase diagrams diffusion, osmosis Introduction to Physics I For Biologists, Geoscientists, & Pharmaceutical Scientists Laws of thermodynamics & thermal properties of matter

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Page 1: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

phase transitions and phase diagrams

diffusion, osmosis

Introduction to Physics I For Biologists, Geoscientists, & Pharmaceutical Scientists

Laws of thermodynamics & thermal properties of matter

Page 2: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

1

T=TH, const. (hot reservoir)

T=TC, const. (cold reservoir) 3

2

4

Reversible heat-work transformation Carnot cycle

Trautwein, Tipler

quasi-static, isothermal absorption of heat from a hot reservoir

quasi-static, adiabatic expansion to a lower temperature

quasi-static, isothermal release of heat to a cold reservoir

quasi-static, adiabatic compression back to the original state

1

3

2

4

Page 3: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

2nd law of thermodynamics

A process whose only net result is to absorb heat from a cold reservoir and release the same amount of heat to a hot reservoir is impossible.

Clausius statement

Tipler

It is impossible for a heat engine working in a cycle to produce only the effect of absorbing heat from a single reservoir and performing an equivalent amount of work.

Heat-Engine statement

Page 4: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

Laws of thermodynamics

Page 5: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

real gas law: van der Waals

Tipler

Van der Waals equation of state

Page 6: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

PV & PT phase diagrams

Uni Bristol

extended PV diagram PT diagram

melting curve

sublimation curve

vapour – pressure vs T curve

Page 7: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

phase transitions

Uni Bristol

Page 8: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

phase transitions… a general class of phenomenon

MIT, mathworld.wolfram

For instance, percolation: phenomenon of a liquid passing through a porous material. Below a certain critical porosity, the material would be unable to allow the liquid to pass - phase transition.

Page 9: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

phase transitions… more For instance, percolation: phenomenon of a liquid passing through a porous material. Below a certain critical porosity, the material would be unable to allow the liquid to pass - phase transition.

https://diracseashore.wordpress.com/2008/09/08/everyday-physics-coffee/

Page 10: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

phase transitions… more

MIT

The boiling of a liquid to a gas exhibits a decrease in order as the molecules are no longer bound and are only weakly interacting The freezing of a liquid to a solid exhibits an increase in order as the atoms occupy locations on a regular crystal lattice The alignment of liquid crystals shows an increase in directional order (although not necessarily spatial order) as the long liquid crystal molecules align and point in the same direction

Kato et al., Chem. Soc. Rev. 2017

Page 11: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

phase transitions… more

MIT

The boiling of a liquid to a gas exhibits a decrease in order as the molecules are no longer bound and are only weakly interacting The freezing of a liquid to a solid exhibits an increase in order as the atoms occupy locations on a regular crystal lattice The alignment of liquid crystals shows an increase in directional order (although not necessarily spatial order) as the long liquid crystal molecules align and point in the same direction The appearance of a permanent magnetic moment in a ferromagnet is an example of an increase in order as the individual magnetic spins point together in the same direction (Curie temperature) The segregation of block copolymers in a polymer melt demonstrates an increase in order as the individual monomer chains separate and aggregate The formation of a Bose Einstein Condensate demonstrates an increase in order as the wavefunctions of the individual atoms become coherent Superconductivity exhibits an increase in order as pairs of electrons (Cooper pairs) act coherently

Phase transitions occur in a variety of materials & systems Phase transition change in constituents' order (order parameter) Different phases variety of properties, technological applications

Page 12: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

entropy during phase transitions

chem.libretexts.org

Page 13: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

vapor pressure

Page 14: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

vapor pressure

Boiling point of water vs pressure

Tipler

Page 15: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

PV diagram

Page 16: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

PVT phase diagram

Uni Bristol

Page 17: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

phase diagrams

Uni Bristol

PV diagram PT diagram

supercritical fluid

Page 18: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

PT phase diagrams

water

NB: The pressure and temperature scales are not linear but are compressed to show the points of interest.

melting curve

sublimation curve

vapour – pressure vs T curve

Page 19: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

scale of things: down to the nanometer

10 cm

x 108

1 nm

7 Carbon atoms

C60

x 108

Page 20: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

surface vs bulk

Atome and der Oberfläche oder tief in Festkörper sind nicht "egal"

?

Page 21: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

at the nanoscale…, the surface becomes more important

1 atom ~ (0.1nm)x(0.1nm)x(0.1nm)

R (micro) ≈ 0.004 %

R (nano) ≈ 40% !

micro

atomsnbtotal

atomssurfacenbR

.

.

100 micrometers (mm)

10 m

m

nano

10 nanometers (nm)

1 n

m

Oberfläche/Volumen

important surface effects

e.g.: lower melting temperature, higher chemical reactivity

Page 22: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

example: melting temperature of nanoparticles

mc /

Lai et al., Phys. Rev. Lett. (1996)

Sn nanoparticles Au nanoparticles

Buffat et al., Phys. A (1976)

Page 23: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

phase diagram: mixing substances

melting curve

sublimation curve

vapour – pressure vs T curve

e.g.: salt in water

Page 24: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

diffusion

Page 25: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

osmosis

Biological physics, P. Nelson

osmotic flow

reverseosmosis

decrease of sugar concentration

increase of sugar solution & heat generation

Page 26: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

osmosis: electrical power generation

Radenovic et al., Nature (2016)

Page 27: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

osmosis: electrical power generation

Radenovic et al., Nature (2016)

Page 28: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

Merry Christmas and

a happy new year!

Page 29: Laws of thermodynamics & thermal properties of matter · thermal properties of matter . 1 T=T H, const. (hot reservoir) 3 T=T C, const. (cold reservoir) 2 4 Reversible heat-work transformation

Merry Christmas and

a happy new year!

Is the 2nd law of thermodynamics ("law of increasing entropy") driving the origin and evolution of life ? see the article by Natalie Wolchover, Scientific American, Jan. 28, 2014