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!"#$$%&#" #() *+#,$,&#" -./012)3(#1%&$ BIOCH 590: Biomacromolecules Spring 2010 Copyright: Jianhan Chen Key references: 1. Chapter 2 of van Holde (2 nd Ed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q # w dE = $q - $w dE = "q - PdV = "q if constant V #E = q v
11

Classical and Sta,s,cal Thermodynamics

Feb 11, 2017

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Page 1: Classical and Sta,s,cal Thermodynamics

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

-./012)3(#1%&$'

BIOCH 590: Biomacromolecules Spring 2010

Copyright: Jianhan Chen

Key references: 1. Chapter 2 of van Holde (2nd Ed.)

-./012)3(#1%&$'

•  -./'40#(&.'25'$&%/(&/'+.#+')/$&0%4/$'+./'4/.#6%20'25'1#7/0'

#()'+0#($5201#,2($'4/+8//(')%9/0/(+'5201$'25'/(/0:3'2('+./'

1#&02$&2;%&'"/6/"<''

•  !"#$$%&#"'+./012)3(#1%&$'

–  =/$&0%4/'+./'$3$+/1'%('+/01$'25'4>"?';02;/0,/$'

–  @'$/+'25'A#8$'25'-./012)3(#1%&$'

–  @4$+0#&+B'4>+':/(/0#""3'#;;"%&#4"/'–  =2/$'(2+'1#?/'0/5/0/(&/'+2'+./'1%&02$&2;%&')/+#%"$'

•  *+#,$,&#"'+./012)3(#1%&$'C$+#,$,&#"'1/&.#(%&$D'

–  E1;.#$%F/'G42721H>;I'#;;02#&.'

–  J026%)/'"%(?$'4/+8//('1%&02$&2;%&')/+#%"$'C+3;%&#""3'(2+'1/#$>0#4"/D'+2'

1#&02$&2;%&';02;/0,/$'C1/#$>0#4"/D'

–  K(&0/#$%(:"3'%1;20+#(+B'4>+')2'(2+'0/;"#&/'&"#$$%&#"'+./012)3(#1%&$'

L'C&D'M%#(.#('!./('

N>()#1/(+#"'!2(&/;+$'

•  *3$+/1'C#""'1#+/0%#"$'%(62"6/)'%('+./';02&/$$'>()/0'$+>)3D'#()'

$>002>()%(:$'C+./'0/$+'25'+./'>(%6/0$/D'

–  O;/('6$'&"2$/'C+0#($5/0'25'1#7/0D'

–  =%#+./01#"'6$'#)%#4#,&'C+0#($5/0'25'./#+D'

–  EP;#()#4"/'20'&2($+#(+H62">1/'C+0#($5/0'25'820?D'

–  K$2"#+/)'C(/%+./0'1#7/0'(20'/(/0:3'/P&.#(:/D'

•  *+#+/'25'+./'$3$+/1'

–  @'+./012)3(#1%&'$+#+/')/Q(#4"/'2("3'520'$3$+/1$'#+'/R>%"%40%>1'

•  @'&2()%,2('%('8.%&.'/R>%"%40%>1'/P%$+$'4/+8//('+./'$3$+/1'#()'%+$'

$>002>()%(:$'8%+.'0/$;/&+'+2'2(/'20'120/'$3$+/1'6#0%#4"/$'

–  *3$+/1'6#0%#4"/$S'/P+/($%6/'#()'%(+/($%6/'

•  ;0/$$>0/'CJD'#()'62">1/'CTD'

•  +/1;/0#+>0/'C-DS'#('#4$+0#&+'R>#(,+3B'1/#$>0/)'%()%0/&+"3'C2!B'NB'UB'VD'

–  K)/#"':#$S'JT'W'('X-B'+.>$'-'W'JTY(X'C#4$2">+/'+/1;/0#+>0/D'

•  &2(&/(+0#,2('C!DS'#('%(+/($%6/'6#0%#4"/'C0/"#,6/'R>#(,+3D'C&D'M%#(.#('!./(' Z'

N%0$+'A#8'25'-./012)3(#1%&$'

•  !2($/06#,2('25'/(/0:3S'./#+'CRDB'820?C8DB'#()'C%(+/0(#"D'/(/0:3'CED'

•  K(+/0(#"'/(/0:3'CED'–  [#&02$&2;%&#""3S'2("3')/Q(#4"/'2('0/"#,6/'$&#"/'C$//'ER'#426/D'

–  [%&02$&2;%&#""3S'1>",;"/'&2(+0%4>,2($'%(&">)%(:S'?%(/,&B'6%40#,2(#"B'

02+#,2(#"B'C&./1%&#"D'42()%(:B'(2(H42()/)'%(+/0#&,2(B'(>&"/%'

C+3;%&#""3'(2+'0/"/6#(+'%('&./1%$+03Y4%2&./1%$+03D'&21;2(/(+$'

–  @'5>(&,2('25'$+#+/''•  =/;/()$'2('+./'$+#+/'2("3B'0/:#0)"/$$'25'+./';#+.'25'#00%6#"'

–  K5'2("3'J')T'820?B'

C&D'M%#(.#('!./(' \'

!

"E = q # w dE =$q -$w

!

dE ="q - PdV="q if constant V

#E = qv

Page 2: Classical and Sta,s,cal Thermodynamics

E(+.#";3'

•  E(+.#";3'C!"#$%&DS'#'$+#+/'5>(&,2('+.#+'&#;+>0/$'/(/0:3'&.#(:/'#+'&2($+#(+'J'

•  N20'"%R>%)';.#$/';02&/$$/$'C12$+'4%2&./1%&#"';02&/$$/$DB')T'%$'

$1#""'#()'+.>$'!E']'!^'

C&D'M%#(.#('!./(' _'

!

dE ="q - PdVd(E +PV ) = dE +PdV +VdP

="q - PdV +PdV +VdP= "q+VdP

dH = "q+VdP= "q if constant P

#H = qp

•  K(+/0(#"'/(/0:3'%$'0/"#+/)'+2'R6B'8.#+'#42>+'R

;`'

^/$$a$'A#8'

•  E(+.#";3'%$'#'$+#+/'5>(&,2(<'-.>$B'+./'/(+.#";3'&.#(:/'25'#'0/#&,2('%$'+./'$#1/'0/:#0)"/$$'25'8.#+';#+.8#3'%$'+#?/('+2'

#&.%/6/'+./';02)>&+$B'%</<B'2("3'+./'$+#0+'#()'/()'$+#+/$'1#7/0'

+2'+./'0/#&,2(B'(2+'+./'%()%6%)>#"'$+/;$'4/+8//(<'

C&D'M%#(.#('!./(' b'

Given:

B2O3(s) + 3H2O(g) ! 3O2(g) + B2H6(g) "H = +2035 kJ H2O(l) ! H2O(g) "H = +44 kJ H2(g) + (1/2)O2(g) ! H2O(l) "H = -286 kJ 2B(s) + 3H2(g) ! B2H6(g) "H = +36 kJ

Find the "H of:

2B(s) + (3/2)O2(g) ! B2O3(s)

Answer: "H = -1273 kJ

c2"+F1#(('=%$+0%4>,2('

•  @'$+#,$,&#"'6%/8'25'+./'$3$+/1'#+'12"/&>"#0'"/6/"'

–  [2"/&>"/$'C25'+./'$#1/'?%()D'8%+.%('+./'$3$+/1'#0/'%()%$,(:>%$.#4"/'

–  @+'#':%6/('121/(+B'/#&.'12"/&>"/'1%:.+'0/$%)/'%('2(/'25'+./';2$$%4"/'

)%$&0/+/'1%&02$&2;%&'$+#+/$'''8%+.'&200/$;2()%(:'/(/0:3'"/6/"'/%''

–  N20'6/03'"#0:/'$3$+/1'C0/1/14/0'@62:#)02'd>14/0S'b<eLPfeLZD'#+'

/R>%"%40%>1B'2("3'12$+';024#4"3'$+#+/'%$'0/"/6#(+<'

•  c2"+F1#((')%$+0%4>,2(S'$;/&%Q/$'+./'12$+';024#4"/'C%</<B'

/R>%"%40%>1D';024#4%"%+3'25'24$/06%(:'#'&/0+#%('/(/0:3'$+#+/'#+'

#'$;/&%Q/)'+/1;/0#+>0/''

–  (cS'c2"+F1#(('&2($+#(+'CWf<Zgeb_eZ'h'feHLZ'M'UHfDi''(

cWXYd

@'

–  -./'12$+'5>()#1/(+#"'0/"#,2($.%;'%('$+#,$,&#"'1/&.#(%&$'C20'

$+#,$,&#"'+./012)3(#1%&$'

C&D'M%#(.#('!./(' j'!

Pi "e#ei / kBT

=/0%6#,2($'25'c2"+F1#(('=%$+0%4>,2('CfD'

•  !2($%)/0'#'+.0//H$+#+/'$3$+/1'C/fB'/

LB'/

ZD<'@+'#':%6/('-B'"/+k$'

80%+/')28('+./';024#4%"%+3'25'Q()%(:'+./'$3$+/1'%('+./$/$'

$+#+/$'#$';fB';

L'#()';

Z<'''

•  *%(&/'/(/0:3'%$'#'0/"#,6/'R>#(,+3B';%Y;

l'W'5C/

%H/

lD''

•  ;ZY;

L'W'5C/

ZH/

LDW'5C/

ZH/

fDY5C/

LH/

fD'

•  <<<'+.%$'1/#($'+.#+'5CPm3D'W'5CPD'5C3D'

•  n.#+'?%()'25'5>(&,2(#"'5201'82>")':%6/'0%$/'+2'$>&.'

;02;/0+3`'

•  V'/P;2(/(,#"'5>(&,2($o'•  V';

%'W'"'/P;'C'H'#'/

%D''

•  V'+.%$'%$'/P#&+"3'8.#+'C(2+'.28D'c2"+F1#((')/0%6/)'f_e'3/#0$'

#:2o'K+'+>0($'2>+'+.#+'#'W'fY?c-'

C&D'M%#(.#('!./(' g'

Page 3: Classical and Sta,s,cal Thermodynamics

=/0%6#,2($'25'c2"+F1#(('=%$+0%4>,2('CLD'

•  !2($%)/0%(:'#('%$2"#+/)'$3$+/1'25')*8%+.'#'+2+#"'/(/0:3'0/$+0%&+/)'+2'EW+,'8./0/'/#&.';#0,&"/'1%:.+'#&&/$$'/(/0:3'

"/6/"$'#0/'-,.*8%+.*-"/.*0.*1.*V'''' '-/*$*-0*$*-1$**2*"*)*

' ',*-0*$*1,*-1*$*3,*-3*$'V'W'+/''

•  c2"+F1#((';2$+>"#+/)'+.#+'%5'2(/'&#('24$/06/'$>&.'#('

#$$/14"3'26/0'#'"2(:';/0%2)'25',1/B'/#&.'1%&02$+#+/'8%""'

2&&>0'8%+.'/R>#"';024#4%"%+3'#()'+.#+'2(/'8%""'Q()'+.#+'+./'

(>14/0'25'2&&>00/(&/$'520'#(3';#0,&>"#0'$/+'25')%$+0%4>,2('%$'

;02;20,2(#"'+2'+./'(>14/0'25'&200/$;2()%(:'1%&02$+#+/$B'

8.%&.'%$':%6/('43S*

C&D'M%#(.#('!./(' p'

!

W =N!

n0!n1!n2!...

=/0%6#,2($'25'c2"+F1#(('=%$+0%4>,2('CLD'

C&D'M%#(.#('!./(' fe'

•  @'&#$/'25'dWjB'EWj/B'+./'+2+#"'(>14/0'25';2$$%4"/'$+#+/$S'fjfb'

!

W1 =7!1!"6!

=5040720

= 7

!

W10 =7!

1!"1!"2!"3!=504012

= 420

=/0%6#,2($'25'c2"+F1#(('=%$+0%4>,2('CLD'

C&D'M%#(.#('!./(' ff'

•  N20'6/03'"#0:/'dB'2("3'+./'12$+';024#4"/'1%&02$+#+/'1#7/0$o'

•  [#P%1%F/'n'20'/R>%6#"/(+"3'"('n'8%+.'d'#()'E'0/$+0%&,2('

=/0%6#,2($'25'c2"+F1#(('=%$+0%4>,2('CLD'

C&D'M%#(.#('!./(' fL'

Page 4: Classical and Sta,s,cal Thermodynamics

=2/$'%+'1#?/';.3$%&#"'$/($/ '̀

•  q%6/('+./'+82'$+#+/'$3$+/1'$.28('+2'+./'0%:.+'

*-$*4*,5678,9(:;****-8*4*,56*7*,9(:;*

C&D'M%#(.#('!./(' fZ'

e

-e

!

P+ =exp -ei /kT( )

exp -e /kT( ) + exp ei /kT( )

P" =exp ei /kT( )

exp -e /kT( ) + exp ei /kT( )

•  n./('+/1;/0#+>0/'%$'(/#0'F/02'C-HreDB'6$'!'eB'68'!f'

•  n./('+/1;/0#+>0/'#;;02#&./$'%(Q(%+3B'p+ = p- = 0.5'

J#0,,2('N>(&,2('

•  q%6/('+./'c2"+F1#((')%$+0%4>,2(B'+./';024#4%"%+3'25'24$/06%(:'

#(3'/(/0:3'$+#+/'%$':%6/('#$S'

•  s'%$')/Q(/)'#$'+./'C&#(2(%&#"D';#0,,2('5>(&,2('•  K5'&2($%)/0%(:')/:/(/0#&3'25'/(/0:3'$+#+/$'

•  !2(+#%($'#""'%(5201#,2('#42>+'+./'$3$+/1'C:%'#()'/

%Do'@""'

&"#$$%&#"'+./012)3(#1%&$'R>#(,,/$'&#('4/')/0%6/)'5021's'

•  ^28'+2'&21;>+/'s`'

–  -./203'#()'$%1>"#,2('

C&D'M%#(.#('!./(' f\'

!

Pj =n j

N=exp "e j /kT( )exp -ei /kT( )

i#

=1Qexp "e j /kT( )

!

Q = gi exp -ei /kT( )i"

*+#,$,&#"'-./012)3(#1%&$'

•  -./012)3(#1%&'/($/14"/$S'#'&2""/&,2('25'%)/(,&#"'>(%+$'

C%</<B'#+21$'20'12"/&>"/$D'25'#'$3$+/1'

–  @'+./20/,&#"'&2(&/;+'+.#+'0/"#+/'1%&02$&2;%&';02;/0,/$'+2'

&200/$;2()%(:'+./012)3(#1%&$';02;/0,/$'

–  ER>%6#"/(&/'25'/($/14"/'#6/0#:/'#()',1/'#6/0#:/'

•  !#(2(%&#"'/($/14"/S'dB'T'#()'-'#0/'&2($+#(+'

•  CK(+/0(#"D'/(/0:3'E'W'tErWdt/r'

C&D'M%#(.#('!./(' f_'

!

Pj =1Qexp "e j /kT( ) =

1Qexp "#e j( )

e = e jj$ Pj =

1Q

e jj$ exp "#e j( )

= "d lnQd#

= kBT2 d lnQdT

*;2(+#(/2>$'J02&/$$/$'

•  X/#"H820")';02&/$$/$'.#6/'#'(#+>0#"')%0/&,2('25'&.#(:/<''–  ^/#+'+0#($5/0$'5021'.%:.'-'+2'"28'-'

–  CK)/#"D':#$'$;2(+#(/2>$"3'Q""$'>;'#""'+./'#&&/$$%4"/'62">1/'

•  E(/0:3'#()'/(+.#";3')2'(2+';026%)/'%(5201#,2('$>&.'

)%0/&,2(#"%+3'25'&.#(:/<'

–  @426/';02&/$$/$'2&&>0'(#+>0#""3'%('%$2"#+/)'$3$+/1$'8./0/'/(/0:3'

)2/$'(2+'&.#(:/'CN%0$+'A#8'25'-./012)3(#1%&$D'

•  n.#+'R>#(,,/$'82>")'./";'>$'+2';0/)%&+'+./')%0/&,2('25'

&.#(:/'%('&21;"/P'$3$+/1$`''

–  !"#$%#&''#&()*"#+,)(&($'$"-o'•  !2(&/;+'25'/(+02;3'#()'*/&2()'A#8'25'-./012)3(#1%&$'

–  O0%:%(#"'&2(&/;+'&21/$'25'$+>)%/$'25'./#+'/(:%(/'C&2(6/0$%2('4/+8//('

./#+'#()'820?D'

–  *+#,$,&#"')/0%6#,2(S';026%)/$'/(+02;3'#'+#(:%4"/'1/#(%(:'

C&D'M%#(.#('!./(' fb'

Page 5: Classical and Sta,s,cal Thermodynamics

E(+02;3'

•  @'1/#$>0/'25'%(+/0(#"'./#+'&2(+/(+B'20B'+./'>(#6#%"#4%"%+3'25'#'

$3$+/1a$'/(/0:3'+2')2'820?'C*WR0/6Y-D<'

•  c#$/)'2('+./'$#1/'"2:%&'+.#+'%$'>$/)'520')/0%6%(:'c2"+F1#(('

)%$+0%4>,2(B'/R>%"%40%>1'#8/'+2'"%/'8./0/'+./';024#4%"%+3'%$'#+'

1#P%1>1<'

C&D'M%#(.#('!./(' fj'

E(+02;3'

•  *+#,$,&#"')/Q(%,2('CfDS'<*"*(=*>-*?************************************CfD'–  EP+/($%6/S'*'W'*

f'm'*

L'

–  @'5>(&,2('25'$+#+/'C#$'n'%$D'

•  *+#,$,&#"')/Q(%,2('CLDS'''''''''''''''''''''''''''''''''''''''''''''''''''''''''CLD'

•  -82')/Q(%,2($'#0/'/R>%6#"/(+''

C&D'M%#(.#('!./(' fg'

!

S = "kB pi ln pii#

!

W =N!

n0!n1!n2!...

lnW = (N lnN " N) " (ni lnni " nii# )

= N lnN " ni lnnii#

X/"#,2('25'!"#$$%&#"'#()'*+#,$,&#"'E(+02;3'

•  -./'$+#,$,&#"')/Q(%,2('25'/(+02;3'+.>$';026%)/$'#'&"/#0"3')/Q(/)'1%&02$&2;%&'1/#(%(:'25'+./'&"#$$%&#"'/(+02;3<'

C&D'M%#(.#('!./(' fp'

!

dS = kBd lnW = "kBd ni lnnii#

= "kB lnnidnii# (remember dni

i# = 0)

ni = n1 exp("ei /kBT) (in reference to e1 = 0)

lnni = lnn1 "eikBT

dS = kBeikBTi

# dni =1T

eii# dni =

dqrev

T

X/"#,2('+2'J#0,,2('N>(&,2('

C&D'M%#(.#('!./(' Le'

!

S = "kB pi ln pii#

= "kBe"ei / kBT

Qln e

"ei / kBT

Qi#

= kB (lnQ+ E /kBT)

=$$T

kBT lnQ( )

= "$A$T

!

E = "d lnQd#

= kBT2 d lnQdT

!

A = "kBT lnQ

A: Helmholtz free energy

Page 6: Classical and Sta,s,cal Thermodynamics

n.#+')2/$'/(+02;3'&#;+>0/ '̀

•  !200/&+'%(+/0;0/+#,2($S'#$':%6/('43'+./')/Q(%,2($''–  @'1/#$>0/'25'%(+/0(#"'./#+'&2(+/(+'C+./'>(#6#%"#4%"%+3'25'#'$3$+/1a$'

/(/0:3'+2')2'820?D'

–  @'$+#,$,&#"'1/#$>0/'25'+./';024#4%"%+3'520'#':%6/('1#&02'$+#+/'

–  @'1/#$>0/'25'>(&/0+#%(+3'C5021'%(5201#,2('+./203D'

•  !2(5>$%(:Y%(&200/&+'%(+/0;0/+#,2($'–  @'1/#$>0/'25'G)%$20)/0I'20'G0#()21(/$$I'

–  @'1/#$>0/'25'G&21;"/P%+3I'

C&D'M%#(.#('!./(' Lf'

!

S = "kB pi ln pii#S = kB ln W

!#"&>"#,2('25'E(+02;3'

•  EP#1;"/S'%$2+./01#"'/P;#($%2('25'%)/#"':#$'5021'Tf'+2'T

L'

C&D'M%#(.#('!./(' LL'

1. Classical approach

!

dE = dq " dw = 0

dq = dw = PdV = RT dVV

#S =qrevT

= R dVV

= R ln V2V1

$

% &

'

( ) V1

V2*

2. Statistical approach: V1 = n1 V0 V2 = n2 V0

!

W1 " n1N W2 " n2

N

#S = kB lnW2 $ kB lnW1

= kB ln n2N

n1N

%

& '

(

) * = R ln n2

n1

%

& '

(

) * = R ln V2

V1

%

& '

(

) *

*/&2()'A#8'25'-./012)3(#1%&$'

•  K('#('%$2"#+/)'$3$+/1B'/(+02;3'0/#&./$'1#P%1>1'#+'

/R>%"%40%>1'C+./'12$+';024#4"/')%$+0%4>,2(D<'K('#(2+./0'820)B''

!*re';026%)/$'#'&0%+/0%2('520'$;2(+#(/2>$'&.#(:/'C2("3'%5'%('#('%$2"#+/)'$3$+/1B'%</<B'8%+.2>+'/(/0:3'/P&.#(:/'%('+./'5201'

25'./#+'20'820?D<'

C&D'M%#(.#('!./(' LZ'

G=/0%6#,2(IS'#+'/R>%"%40%>1B'#('%(Q(%+/$%1#"'&.#(:/'%$'

0/6/0$%4"/<'

K('#))%,2(B'520'%$2"#+/)'$3$+/1B'@#We.*@AWe<'-.>$B'

+./0/520/B'/(+02;3'%$'/%+./0'#+'1#P%1>1'20'1%(%1>1<'!

dE = dq " dw = TdS " PdV

!

dS = 0

N0//'E(/0:%/$'

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' ' 'CT')J'u'*')-'D'm')E'u'C-')*'u'J')TD'W'e'

' ' ')E'm'T')J'm'J')T'u'C'*')-'m'-')*D'W'e'

' ' ')'C'E'm'JT'u'-*'D'W'e'

•  K5'8/')/Q(/'#'(/8'R>#(,+3'q'W'E'm'JT'u'-*'W'^'u'-*B''' ' ')q'W'e'''''''520'#'0/6/0$%4"/';02&/$$'#+'dJ-'

•  q'%$'0/5/00/)'+2'#$'Gq%44$'50//'/(/0:3IB'8.%&.'%$'#+'1%(%1>1'#+'

/R>%"%40%>1'>()/0'dJ-'&2()%,2('C12$+'&2112(D<'

•  *%1%"#0"3B'^/"1.2"+F'50//'/(/0:3B'@'W'E'u'-*B'%$'#+'1%(%1>1'#+'

/R>%"%40%>1'>()/0'dT-'&2()%,2(<'

•  -./'50//'/(/0:%/$';026%)/'+./')%0/&,2('25'$;2(+#(/2>$'&.#(:/$'>()/0'&200/$;2()%(:'&2()%,2($<'

C&D'M%#(.#('!./(' L\'

Page 7: Classical and Sta,s,cal Thermodynamics

N0//'E(/0:3'#()'J024#4%"%+3'

•  X/1/14/0B'5021'+./'$+#,$,&#"'1/&.#(%&#"';2%(+'25'6%/8B'

)%0/&,2('25'$;2(+#(/2>$';02&/$$/$'%$':%6/('43'+./')%0/&,2('25'

1#P%1>1';024#4%"%+3<'

–  520'%$2"#+/)'$3$+/1$B'+./';024#4%"%+3'25'#'1#&02H$+#+/'%$':%6/('43'

/(+02;3<'%</<B'n'W'/P;'C'*Y?cD''

C&D'M%#(.#('!./(' L_'

•  N20'#'$3$+/1'&2>;"/)'8%+.'dJ-'&2()%,2($B''

•  N20'#'$3$+/1'&2>;"/)'8%+.'dT-'&2()%,2($B'

!

Pi "exp(#Gi /RT) = exp(#Hi /RT)exp(Si /R)

!

Pi "exp(#Ai /RT) = exp(#Ei /RT)exp(Si /R)

*+#,$,&#"'[/#(%(:'25'N0//'E(/0:%/$'

•  =%0/&+"3')/Q(/)'43'+./';024#4%"%+3'25'#'1#&02H$+#+/'

•  N>0+./0'0/"#+/)'+2'+./';02;/0,/$'25'1%&02$&2;%&'$+#+/$'

+.02>:.'+./';#0,,2('5>(&,2('

•  N20'/P#1;"/S''

C&D'M%#(.#('!./(' Lb'

!

S =""T

kBT lnQ( ) = kB lnQ+ kBT" lnQ"T

!

E = "d lnQd#

= kBT2 d lnQdT

!

A = E "TS

= kBT2 d lnQdT

"T(kB lnQ+ kBT# lnQ#T

)

= "kBT lnQ

O+./0'-./012)3(#1%&'J02;/0,/$'

•  !"#$$%&#"'+./012)3(#1%&$'0/"#,2($.%;$'&#('4/'>$/)'+2'

)/0%6/)'+./'$+#,$,&#"')/Q(%,2($'25'#""';02;/0,/$'

•  N20'/P#1;"/S'

C&D'M%#(.#('!./(' Lj'

!

P = "#A#V$

% &

'

( ) N ,T

= kBT# lnQ#V

$

% &

'

( ) N ,T

H = E + PVG = A + PV

Cv =#E#T$

% &

'

( ) N ,V

Cp =#H#T$

% &

'

( ) N ,P

!

S =""T

kBT lnQ( )!

E = "d lnQd#

!

A = "kBT lnQ

E(+.#";3'#()'E(+02;3'!21;/($#,2('

•  !q'W'!^'u'-!*'•  !2($%)/0'#('/P#1;"/'25';02+/%('52")%(:S'

$ $ $ $ $ $ $!^5't'e'''!-

5't'e'

f<  A28'+/1;/0#+>0/B'!q5'W'!^

5'u'-!*

5't'e'C52")%(:D'

C+./'5#620/)'$+#+/'%$'(2+'+./'120/'G0#()21I')/(#+>0/)'$+#+/oD''

L<  @+'52")%(:'+/1;/0#+>0/'-1B'!q

5'W'e'C;

5'W';

>'W'e<_D'

Z<  ^%:.'+/1;/0#+>0/B'!q5'W'!^

5'u'-!*

5'r'e'C>(52")%(:D'

C&D'M%#(.#('!./(' Lg'

Enth

alpy

native

denatured

Page 8: Classical and Sta,s,cal Thermodynamics

ER>%"%40%>1'!2($+#(+'

•  X/1/14/0'+.#+':%6/('#'0/#&,2(S''

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'+./'R>#(,+3S'U'W'v!wv=wYv@wvcw'%$'#'&2($+#(+'+.#+'%$'&2112("3'0/5/00/)'+2'#$'

#('G/R>%"%40%>1'&2($+#(+I<'c>+'8.3'#'&2($+#(+`''

C&D'M%#(.#('!./(' Lp'

•  .,))/S''•  N%0$+B'(//)$'+2')/Q(/'#'G$+#()#0)'$+#+/”'C&2112("3'LpgUB'f#+1B'f[D<'

-./('520'#'$2">,2('8%+.'#'&2(&/(+0#,2('v@wB'

' ' ' 'q'W'qe'm'X-'"('Cv@wYv@weD'W'qe'm'X-'"('v@w'

•  -./0/520/B $ $ $ $!q'W'!qe'm'X-'"('Cv!wv=wYv@wvcwD'

•  @+'/R>%"%40%>1B'!q'W'e<'-.>$B'

' ' ' '!qe'm'X-'"('Cv!wv=wYv@wvcwD'W'e'

' ' ' '!qe'W'H'X-'"('U'

' ' ' 'U'W''v!wv=wYv@wvcw'W'/P;'C'H'!qeYX-D'

-./012&./1%$+03'

•  EP;/0%1/(+#"')/+/01%(#,2('25'+./'+./012)3(#1%&'

;#0#1/+/0$'$>&.'#$'!qB'!^'#()'!*<''

•  !q'&#('4/')%0/&+"3'&#"&>"#+/)'5021'U/R'

–  Ox/(')2(/'43'Qy(:'+2'#',+0#,2('&>06/'

–  X/R>%0/'&.22$%(:'#'1/#$>0#4"/'+.#+'0/$;2()$'+2'4%()%(:'20'C4%2HD

&./1%&#"'0/#&,2('

•  =/+/01%(#,2('25'!^'#()'!*'–  T#(a+'^29'X/"#,2($.%;'–  !#"20%1/+03'

–  -./203'#()'$%1>"#,2(S'(2+'0/"%#4"/'#+'R>#(,+#,6/'"/6/"'

C&D'M%#(.#('!./(' Ze'

T#(a+'^29'X/"#,2($.%;'

•  -./'&"#$$%&#"'#;;02#&.B'0/R>%0/'1>",;"/'1/#$>0/1/(+$'25'U/R'

#+')%9/0/(+'+/1;/0#+>0/$'#()'&/0+#%('#$$>1;,2($'

C&D'M%#(.#('!./(' Zf'

!

lnKeq = "#G0

RT= "

#H 0

RT+#S0

R

•  @$$>1%(:'+.#+'!^'#()'!*'#0/'+/1;/0#+>0/'

%()/;/()/(+'C2x/('#'

$+02(:'#$$>1;,2('%('

4%2&./1%&#"Y4%2;.3$%&#"'

;02&/$$/$'

•  'G$#5/0I'+2'&#"&>"#+/'!*WC!^H!qDYX'

!#"20%1/+03'

•  G+./'R>#(,+#,6/'1/#$>0/1/(+'25'./#+I'

•  =/;/()%(:'2('+./'$/+>;B'/%+./0'B6'20'B

;'

–  J024/'!E'C4214D'20'!^'C&2($+#(+';0/$$>0/D'

–  c%2&./1%&#"'$3$+/1$'2x/('0/R>%0/'+./'#4%"%+3'+2'

$+>)3'6/03'$1#""'62">1/$'C1%&20&#"20%1/+03D'

•  @'&#"20%1/+/0'1/#$>0/$'+./'./#+'%(+2'20'2>+'25'

+./'$#1;"/'

•  @')%9/0/(,#"'&#"20%1/+/0'1/#$>0/$'+./'./#+'25'

+./'$#1;"/'0/"#,6/'+2'#'0/5/0/(&/'

•  @')%9/0/(,#"'$&#((%(:'&#"20%1/+/0'C=*!D')2/$'

#""'+./'#426/'#()'./#+$'+./'$#1;"/'8%+.'#'

"%(/#0'+/1;/0#+>0/'0#1;'

C&D'M%#(.#('!./(' ZL'

•  @'K$2+./01#"'-%+0#,2('!#"20%1/+03'CK-!D'1/#$>0/$'+./'./#+'

#4$204/)'20'0/"/#$/)'43'#'C4%2D&./1%&#"'0/#&,2('

Page 9: Classical and Sta,s,cal Thermodynamics

=%9/0/(,#"'*&#((%(:'!#"20%1/+03'C=*!D'

•  -./')%9/0/(&/'%('./#+'z28'+2'+./'$#1;"/'#()'#'0/5/0/(&/'#+'+./'

$#1/'+/1;/0#+>0/B'%$'0/&20)/)'#$'#'5>(&,2('25'+/1;/0#+>0/<''

C&D'M%#(.#('!./(' ZZ'

@(#"3$%$'25'=*!'

•  [2$+"3'520'12(%+20%(:'./#+'/9/&+$'#$$2&%#+/)'8%+.';.#$/'

+0#($%,2($'#()'&./1%&#"'0/#&,2($'#$'#'5>(&,2('25'

+/1;/0#+>0/'C$>&.'#$';02+/%('52")%(:D'

•  c#$%&';02;/0,/$'#0/S'

C&D'M%#(.#('!./(' Z\'

!

Cp = dqp /dT = dH /dT

"H # CpdTT1

T2

$•  *>4$+#(,#"'&21;"%&#,2($'

#0%$/')>0%(:'+./'+0#($%,2('

0#(:/'8./0/'#'1%P+>0/'25'

;2+/(,#""3'1#(3'C1%&02HD'

$+#+/$'1%:.+'&2(+0%4>+/'+2'

+./'24$/06/)'C;'#()'

)/&2(62">,2('4/&21/$'

.%:."3'(2(H+0%6%#"'

-82H*+#+/'@(#"3$%$'25'=*!'

C&D'M%#(.#('!./(' Z_'

Native

Denatured

Tm

!

"H 0(Tm ) # "H 0 $ (Cp %Ci)dTTi

T j

&

"S0(Tm ) = "H 0(Tm ) /Tm

•  -82H$+#+/'0/6/0$%4"/'+0#($%,2('#$$>1/)'

!

"H 0(T) = "H 0(Tm ) + "CpdTTm

T

#

"S0(T) = "S0(Tm ) + "Cp /T dTTm

T

#

"Cp = Ci $C j

Note: baseline correction often needed.

X/"#,2('+2'+./'6#(a+'^29'E(+.#";3'

•  Different assumptions involved in DSC analysis and van’t Hoff relationship. Nonetheless,

C&D'M%#(.#('!./(' Zb'

!

"HDSC0 (T) and "HvH

0 (T) can be related.•  Assuming a reversible two-state system, the (base-line corrected)

calorimetry enthalpy change,

!

"Hi0(Tx ) = [Cp (T) #Ci(T)]dT

Ti

Tx

$ = "Ci(T)dTTi

Tx

$

% fi "H % f i "CpdTTi

T j

$

"H j0(Tx ) % # f j CpdT

Ti

T j

$

K(T) =f jf i% #

"H j0(T)

"Hi0(T)

Ti

Tj

Tx

!

"HvH0 (T) = #RT 2 d lnK(T)

dT= #RT 2 "Ci(T)

"Hi0(T)

#"C j (T)"H j

0(T)

$

% & &

'

( ) )

!

Disagreement of "HDSC0 (T) and "HvH

0 (T) indicates non two - state behavior

Page 10: Classical and Sta,s,cal Thermodynamics

[#l20'*2>0&/$'25'E0020$'

•  !#"%40#,2('•  !2(+#1%(#,2('

•  *#1;"/';0/;#0#,2('u'.28'$#1;"/'%$'"2#)/)'%(+2'#';#('

–  d//)'+2'1%(%1%F/'+./01#"':0#)%/(+'

•  X/$%)>#"'$2"6/(+$'#()'12%$+>0/<'

•  -./01#"'"#:'

–  ^/#,(:Y!22"%(:'0#+/$'–  *#1;"/'1#$$'

•  J02&/$$%(:'/0020$'

C&D'M%#(.#('!./(' Zj'

K$2+./01#"'-%+0#,2('!#"20%1/+03'

•  [2$+"3'>$/)'520'

>()/0$+#()%(:'%(+/0H

12"/&>"#0'%(+/0#&,2($'

•  K(&0/1/(+#"'#))%,2('26/0'

,1/'25'#'"%:#()'C20'#'

4%()%(:';#0+(/0D'%(+2'#'

$2">,2('25'#';02+/%('C20'

#(2+./0';#0+(/0DB'>(,"'(2'

/P&/$$'./#+'1/#$>0#4"/'C(2'

120/'50//';02+/%(D'

•  [/#$>0/'+./'./#+'0/R>%0/)'

+2'1#%(+#%('+./'

+/1;/0#+>0/'

C&D'M%#(.#('!./(' Zg'

@(#"3$%$'25'K-!'

•  [>&.'$%1;"/0'&21;#0/)'+2'=*!'

C&D'M%#(.#('!./(' Zp'

!

q = "H 0(T)nPL = "H 0(T)V[PL]

= "H 0(T)V[PT ]Ka[L]1+ Ka[L]

!

[PL] = [PT ]Ka[L]1+ Ka[L]

P + L PL

!

qi = "H 0(T)V[PT ]Ka[L]i1+ Ka[L]i

#Ka[L]i#11+ Ka[L]i#1

$

% &

'

( )

=/Q(/'#'0#,2'D'W'vA-wYvJ

-wB'Qy(:'25'B

%'6$'X'8%""'3%/")'42+.'U

#'

#()'!^eC-D<''N0//'/(/0:3'#()'/(+02;3'&.#(:/$'+./('52""28<'!

[L]i = 0.5([LT ]" [PT ]± ([LT ]" [PT ]"1/Ka )2 " 4[LT ])

C&D'M%#(.#('!./(' \e'

EMBO reports 8, 1, 63–69 (2007)

the yeast exosome

Page 11: Classical and Sta,s,cal Thermodynamics

A%1%+#,2($'25'K-!'

•  =%{&>"+'520'$+>)3%(:'6/03'$+02(:'4%()/0$'

–  E#&.'%(&0/1/(+#"'25'"%:#()'4/&21/$'&21;"/+/"3'42>()'>(,"';02+/%('%$'

5>""3'&2($>1/)i'(2'+0#($%,2('+2'Q+o'

–  |;;/0'"%1%+'U#']'fep'[Hf'

–  [%:.+'4/'26/0&21/'43'$2H&#""/)')%$;"#&/1/(+',+0#,2('

C&D'M%#(.#('!./(' \f'

Ka ~ 106 M-1 Ka ~ 1012 M-1

=%$;"#&/1/(+'K-!'

C&D'M%#(.#('!./(' \L'

Nature Protocols 1, - 186 - 191 (2006)

Weak inhibitor strong inhibitor (Ka ~ 1012 M-1)

!#"20%1/+03'520'=0>:'=/$%:('

•  c2+.'=*!'#()'K-!'#0/';28/05>"'+22"$'520'24+#%(%(:'+./012)3(#1%&')#+#'&0%,&#"'520')0>:')/$%:('

•  ^28/6/0B'42+.'#0/',1/H&2($>1%(:'#()'"#420%2>$'#()'$;/&%#"'

)/$%:($'#0/'(/&/$$#03'520'+./'(//)'25'.%:.H+.02>:.;>+''

–  /<:<B'-./012N">20-['+/&.(2"2:3S'"/$$'R>#(,+#,6/''

•  n./+./0'4%()%(:'%$'/(+.#";3'20'/(+02;3')0%6/('&#(';026%)/'

%1;20+#(+'%($%:.+$'520'"/#)'2;,1%F#,2('C#()'$>&.'%(52'&#('(2+'

4/'24+#%(/)'5021'$+0>&+>0#"')#+#D'

•  X/;"#&/1/(+'K-!'520',:.+'4%()/0$'

C&D'M%#(.#('!./(' \Z'

Ref: “Calorimetry and Thermodynamics in Drug Design” by J. B. Chaires, Annu. Rev. Biophys. 2008. 37:135–51 .