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7/23/2019 Lecture 6 Liquids and Solids.pptx
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Liquids and SolidsChapter 11
1
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Liquids and Solids
2
~12 bar, assuming
gas is Ar, T=298K
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Gases vs. Liquids &
Solids
3
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Textbook Chapters to
Cover11.2 Solids, Liquids, and Gases: a Moleular
Co!parison
11.", 11.# $nter!oleular %ores11., 11.' (apori)ation, (apour *ressure,
Subli!ation and %usion
11.+ eatin- Curve or /ater
11.0 *hase ia-ra!s11. /ater: 3n 4xtraordinar5 Substane
11.11, 11.12 Cr5stalline Solids
4
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4xluded Textbook
Chapters11.1 Cli!bin- Gekos and $nter!oleular
%ores
11.16 Cr5stalline Solids: eter!inin- TheirStruture b5 789a5 Cr5stallo-raph5
11.1" Cr5stalline Solids: and Theor5
5
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;utline$nter!oleular %ores
*roperties o Liquids
*hase Chan-eseatin- Curves
*hase ia-ra!s
Cr5stalline Solids
6
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IntermolecularForces%ores o attration & repulsion
;perative in !oleular solids, liquids, and -ases
<as opposed to !etalli, ovalent, & ioni solids=
7
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%ores o attration &
repulsion%ores in non8!oleular solids: !etalli <e.-.
Cu=, ovalent <e.-. dia!ond=, and ioni <e.-.>aCl= bonds These ores are 16 ti!es stron-er than van der
/aals ores ?@ hi-h !p & bp.
%ores in !oleular speies: inter!oleular<aka van der /aals= oresA e.-.
2;, su-ar,
Baxdispersion ores <aka London ores=
dipole8dipole ores
h5dro-en bondin- 8
8
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ispersion %ores3lso alled London %ores
;perate in all !oleules
ue to eletron loud <e..=Collision distorts e.. → instantaneous
dipole
$nst. dipole indues sa!e on nearb5!oleule
9
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4et o Moleular Si)e
10
*olarisabilit5oB easil5 is eletron loud distortedD
More eletrons ? !ore polarisable
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4et o Shape4xposed surae inreases interation
11
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ipole8ipole
$nterationsetBeen !oleules Bith per!anent dipole
ipole results ro!
Enequal eletron sharin- <dierenteletrone-ativities=
3s5!!etr5 o !oleule
9elativel5 stron- inter!oleular ore
Stren-th depends on dipole !o!ent
12
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4xa!ple: 8ClCl is ver5 eletrone-ativeA is less so
Cl pulls eletrons toBards its end <ne-ative=
let Bith partial positive har-e end o one Cl attrated to Cl end o
another
13
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14
ipole8ipole $nterations
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ipole Mo!ent &
S5!!etr51,2-Dichlorobenzene 1,4-Dichlorobenzene
Dipole moment2.6 deb5e <=
Boiling point1,28C: 106.FC
Dipole moment6.66 <s5!!etr5=
Boiling point1+#FC
15
>o net dipole
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16
ipole Mo!ent & bp
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LC: oilin- *oints/hih list o o!pounds is in order
o dereasin- boilin- pointD
3. $2, Cl2, r2
. C'', C''Cl, C''Cl2
C. 3s<C"=", *<C"=", ><C"="
. C#, C2', C"0
17
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LC: oilin- *oints/hih list o o!pounds is in order
o dereasin- boilin- pointD
C. 3s<C"=", *<C"=", ><C"="
London ores operativeCo!pound Bith !ost eletrons Bill have
hi-hest b.p.
18
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5dro-en ondin-Moleules Bith bound
to >, ;, or %.
ato! is eletropositive.SuperH dipole8dipole
ore, unusuall5 stron-.
>ot to be onused Bith a
he!ial bond <i.e. aovalent bond=.
19
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20
5dro-en ondin-
Covalent
bond
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21
5dro-en ondin-
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LC: Choose the liquid at
9T;ne o these o!pounds is aliquid at 9T and the other tBo are
-ases. /hih one is a liquidD /h5D
3.2C?;
.C"%
C.2;2
22
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LC: Choose the liquid at
9T;ne o these o!pounds is aliquid at 9T and the other tBo are
-ases. /hih one is a liquidD /h5D
C.2;2
3ll three have 1'810 e, i.e. si!ilar dispersionores. 3ll three have dipole !o!ents. ;nl52;2 has diretl5 bonded to an
eletrone-ative ato! <;=, i.e. h5dro-en
bondin-. 2;2 has the hi-hest bp. 23
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$on8ipole %ores;perate in ionic solution. <More to o!e in Ch
12.=
24
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4xa!ple/hih ores are operative in the olloBin-
substanesD oB do 5ou expet their b.p.Is too!pareD
Co!pound %ores:b.p.JFC
2;
C">2
>aCl
C"<C2=1#C"
Cl 25
8bondin-, London %ores
8bondin-, London %ores
$oni ondin-
London %ores
London %ores, dipole8dipole
London %ores
166
8'."
1#1"
1#
80
810"
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26
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Properties ofLiquids
27
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*roperties o LiquidsSel8stud5: visosit5, surae tension, apillar5
ation <K11.#=
(apour *ressure
28
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(apour *ressureVapour pressure is the equilibrium partial
pressure o the vapour in the spae above aliquid
29
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(.*. inreases Bith te!p
30
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(.*. inreases Bith te!p
31
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(.*. inreases Bith te!p3 liquid Bill boil Bhen its vapour pressure
is equal to at!ospheri pressure.
The nor!al bp o a liquid is thete!perature at Bhih its vapour pressure is1.61"2 bar <1 at!=.
Liquids Bith hi-h vapour pressure at roo!
te!perature have loB boilin- points.
32
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LC: oilin- /ater3 pot o Bater is plaed on a stove. eore itboils, bubbles or! at the botto! o the pot andrise to the top. /hat are the bubbles !ade oD
<3=eat
<=3ir
<C=;x5-en -as and h5dro-en -as
<=/ater vapour
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bp at 266 !
(.*. inreases Bith
te!p(.*. urve an beused to nd boilin-point at pressuresother than 1.61"2bar <1 at! ? +'6
Torr=.
34
3t!os.press. at266 !
<"2 torr=
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LC: (apour *ressure
The vapour pressure o aet5lene, C22,
stored in a pressuri)ed 5linder is about
6.62 bar at 16 and 2.6 bar at 266 ./hat is the !ost likel5 value or thevapour pressure at 1+ D
3. 6.62 bar
. 6." barC. 1.6 bar
. 1. bar
35
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LC: (apour *ressure
. 6." bar
9e!e!ber shape o urve.
36
6.62
Te!p <=
16 266
2.66
1.66
1+
( a p p
r e s s < b a r =
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Clausius8Clape5ron
4quation
4quation or the vapour pressure urve<T1,*1= and <T2,*2= are tBo vapour pressure
data
∆vap is the enthalp5 o vapourisation
9 is the -as onstant: 0."1# NJJ!ol>otes:
T is alBa5s in
∆
vap is in NJ!ol, so that units anel Bith 9
37
lnP2
P1
=∆Hvap
R
1
T1
− 1
T2
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Eses or Clausius8
Clape5ron*redit (.*. at T2, -iven:
4nthalp5 o vapourisation <∆vap=
(.*. <*1= at te!perature T1
*redit boilin- point <T2= at pressure *2, -iven:
∆vap
>or!al bp <T1
, *1
=
;btain ∆vap -iven tBo T,* data
e.-. nor!al boilin- point and one other
38
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4xa!ple/hat is the (.*. o Bater <in torr= at 6FC i it is10 torr at 2 FC <∆vap? ## kNJ!ol=D
3ns: rst, rearran-e C8C equation or *2
39
P2 = P1 exp
∆ H vap
R
1
T 1 −1
T 2
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4xa!pleOont>ext, onvert te!peratures to & ∆vap to
NJ!ol:
T1 ? 20
T2 ? "2" ∆ ? ## 666 NJ!ol
*1 ? 10 torr
Then plu- in the values and alulate
*2 ? +1 torr
>ote: T inreased b5 0P, but * inreasedb5 26PQ
40
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LC: Clausius8Clape5ron/hat is the bp o Bater at the Mexio Cit5airport <altitude 22"6 !A at!ospheri pressure? 00 torr=D
∆vap? #6.'0 kNJ!olA 9?0."1# N 81 !ol81A 1
at!?+'6 torr
3. 200.+
. "''.6
C. 2".'
. "06.'
41
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LC: Clausius8Clape5ron. "''.6 <onl5 reasonable ansBer=
9earran-e C8C equation or 1JT1
9eall that T2,*2 is nor!al bp
42
21
2
vap1 T
1
P
PlnH
R
T
1 +∆
=
373.15
1
588
760ln
40680
8.3145
T
1
1
+=
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Phase Chanes! Phase Diarams
43
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*hase Chan-es
44
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4nthalpies o Transition
45
∆Hvap° -∆Hvap°
∆Hfus°-∆Hfus°
∆Hsub° -∆Hsub°
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46
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eatin- Curves
47
q = mCs,steam
∆T
q = n∆vapH°
q = n∆fusH°q = mCs,liq∆T
q = mCs,ice∆T
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*hase ia-ra!s
48
• Line segments (AC, AD, AB)
represent certain T & P at
which the substance is in
equilibrium between two
states.• Triple point (A) represents the
unique T and P at which solid,
liquid, and gaseous states are in
equilibrium.• Critical point (B) represents
the T & P above which a
supercritical fluid exists.
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*hase ia-ra!s
49
Liquid will
not form
beyond this
temperature
(crit. temp.)
1 atm
bpmp
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Critial Te!perature and *ressureCritical temperature:
above this te!perature, liquid state Bill notor!
Critical pressure: pressure required to lique5 -as at ritial
te!perature
3bove ritial T & *, Ruid is superritialH
50
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Superritial en)ene
51
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2; and C;2
52
Negative Slope (atypical) Positive Slope (typical)
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Solids" Propertiesand #ondin
53
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;rder in Solids TBo t5pes
Crystalline: ato!s in
ordered !atrixe.-. quart)
solids have aets, leave alon- Bell denedplanes
Amorphous: short8ran-e ordersolids !elt over ran-e o te!peratures
properties depend on preparation
54
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55
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Moleular Solidsvan der /aals interations
e.-. 3r<s=, 2;<s=, C'12;'<s=
loB bp & !peletrial insulators
soluble in solvents o si!ilar polarit5
56
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Moleular Solids
Boiling point depends onnu!ber o eletrons, as expeted
Melting point depends onstren-th o inter!oleular ores
eien5 o pakin- <!oleular shape=
57
CH3Benzene:
mp = 5˚C
bp = 80˚C
Toluene:
mp = -95˚C
bp = 111˚C
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$oni Solidse.-. >aCl <s=, CsCl <s=, nS <s=, Ca%2 <s=
ondin-: eletrostati attration betBeen ions
ard, brittle
i-h !p & bpbp & !p depend on surface charge density o
ions
!p o M-; ? 202°CA !p o >aCl ? 061°C4letrial and ther!al insulators
So!e are soluble in polar solvents
58
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Metalli Solidse.-. %e<s=, >a<s=
ondin-: Metal ions in a seaH o valeneeletrons
Sot, dutile, !alleable
(ariable !p & bpMo !p 2'2" °CA >a !p 0 °CA - !p 8" °C
Man5 are soluble in <reat Bith= aids4letrial and ther!al ondutors
59
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>etBork Covalent Solidse.-. C<dia!ond=, C<-raphite=, SiC<s=
Covalent bondin-: ato!s share eletrons
(er5 hard & brittle(er5 hi-h bp & !p
$nsulators or se!iondutorsC<-raphite= is ondutor
$nsoluble in solvents
60
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>etBork Covalent Solids
61
Van der Waals
Forces
Covalent bonds
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LC: !eltin- points/hih solid has the loBest !eltin- point andBh5D
3. >aCl<s=
. C<s, dia!ond=
C. C"1'#<s=
62
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LC: !eltin- points/hih solid has the loBest !eltin- point andBh5D
3. >aCl<s=
. C<s, dia!ond=
C. C"1'#<s=
C"1'# is a !oleular solid held to-ether b5 van
der /aals <inter!oleular= ores.>aClJdia!ond is held to-ether b5
ioniJovalent bonds, respetivel5, ten ti!es63
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Cr$stal Structure
in Solids
64
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Cr5stal Struture TBo parts to a r5stal
Lattice9epeatin- "8 pattern o points in spae
Theoretial
BasisChe!ial unit <ato!, !oleule, et.=
;ne basis unit at eah lattie point
65
C t l L tti d E it
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Cr5stal Lattie and Enit
CellLattie o!prised o repeatin- units alledunit ells
66
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Cubi Enit Cells
67
e.-. poloniu!*o<s=
e.-. alpha ironα8%e<s=
e.-. platinu!*t<s=
> b t it
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>u!ber o ato!s per unit
ell
68
8×1 / 8 = 1 atom 8×1 / 8 + 1 = 2 atoms 8×1 / 8 + 6×1 / 2= 4 atoms
Si!ple Cubi od5 Centred Cubi %ae Centred Cubi
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LC: %ind the %or!ula%ro! the unit ell, beloB, Bhat is the or!ula o
the oxide o niobiu!D
A. NbO
B. NbO2
C. Nb2O3
D. Nb2O
69
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%ind the %or!ula3. >b;12 O atoms shown
4ah has U insideell
Thereore, " ; ato!s6 Nb atoms shown
4ah has V insideell
Thereore, " >bato!s
Formula: Nb3O3
S!allest ratio: >b;
70
S tili ti i bi
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Spae utilisation in ubi
ells
71
Si!ple Cubi<1 ato!=
od5 Centred Cubi<2 ato!s=
%ae Centred Cubi<# ato!s=
# r 2 r# r
a
%&'2r()&*r) <#r=2 ?a2Wa2Wa2
a ? r√<1'J"=% &
<#r=2 ? a2Wa2
a ? r√0
% & r)
'*()2
S tili ti i bi
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Spae utilisation in ubi
ellsoB !uh spae taken up b5 ato!sD
3to! volu!e ? <#J"=πr"
Si!ple ubi:1 ato! per ell: <#J"=πr"J<0r"= ? πJ' ? 2./0
od58entred ubi:
2 ato!s per ell: 2×<#J"=πr"J<r"<1'J"="J2= ? +*.0
%ae8entered ubi: do the alulation5ourselQ
72
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LC: spae utilisationoB !uh spae istaken up b5 ato!s<as a perenta-e= in a
ae8entred ubiD
73 73
%ae Centred Cubi
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LC: spae utilisationoB !uh spae istaken up b5 ato!s ina ae8entred ubiD
# ato!s per ell:
#×<#J"=πr" J<r"<0="J2=
? /.0
74 74
%ae Centred Cubi
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M5 Super *oBer$ 5ou ould have an5 super poBer, BhatBould it beD
75
Packing the most amount
of stuff into the smallest
amount of space/time!
Close packing maximizes
atomic interactions and
minimizes the volume
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LC: %ind the densit5(anadiu! <(= r5stallises in a b struture and
has an ato!i radius o 1"1 p!. eter!ine thedensit5 i the ed-e len-th o the b unit ell is
#rJ√" and the ato!i !ass is 6.# -J!ol. <>3 ? '.622×162" !ol81=
3. ".6' -J!"
. '.11 -J!"
C. 2.++ -J!"
. 12.2 -J!"
4. 0.#' -J!"
76
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LC: %ind the densit5. '.11 -J!"
.Enit ell vol. ? X#×<1"1×16816 !=J√"Y" ?2.+'0×1682" !"
.2 ato!sJell: 2J<'.622×162" !ol81= ?"."21×1682# !ol
.
densit5: <"."21×1682# !ol=<6.# -J!ol=J<2.++×1682" !"=
.densit5: '.11 -J!"
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Su!!ar5Solids and liquids lassied b5 ores oattration
*roperties o substane result ro! ores o
attration!.p., b.p., ondutivit5, visosit5, et.
*hase han-e data su!!arised b5 heatingcurves & phase diagrams
Cr5stal struture o solids lassied b5 crystallattice and the basis
Moleular or!ula an be ound ro! the unit
ell 78
Su--ested Ch 11
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Su--ested Ch 11
4xerises9evieB questions 28#.
*roble!s b5 Topi, Cu!ulative *roble!s,Challen-e *roble!s: #, ", , , '1, '",
'+, ', +", ++, +, 0", 0, 0+, 0, 1, +, ,161, 16, 16+, 111, 11", 12, 1#1, 1, 1'1.
>ote: ansBers to all odd8nu!bered proble!sare ound in 3ppendix $$$.