molecular and supramolecular understanding of
TRANSCRIPT
2II Jornadas Nacionais de Caracterização de Materiais
Energy balances.
Chemical reactions
Physical processes
Materials Characterization
Biophysics/Biochemistry
Engineering
to measure and follow heat changes in processesCalorimetry:
3II Jornadas Nacionais de Caracterização de Materiais
But Heat , q... Is not possible to measure directly
e.g. Heat flux ...versus... Time
to measure and follow heat changes in processesCalorimetry:
4II Jornadas Nacionais de Caracterização de Materiais
e.g. Heat flux ...versus... Time
T heatT
time
time
5II Jornadas Nacionais de Caracterização de Materiais
Seems to be a old-fashioned subject !!
Low-tech apparatus / methodology!!
to measure and follow heat changes in processesCalorimetry:
6II Jornadas Nacionais de Caracterização de Materiais
to measure and follow heat changes in processesCalorimetry:
DEPENDS:
Size of the Sample / Process
How strong is the heat change
What heat change we want to measure
Which process we want to follow
RESOLUTION/ACCURACY measurement
• isoperibolic (static and dynamic)
• heat exchanging (isothermal and temperature scanning)
• adiabatic (static and dynamic)
To measure lots of HEAT.... (e.g Chemical Reaction..combustion)
Temperature homogeneity
Lots of heat involved
MOTOR
Local
T control
Heating
cooling
Precise
T control
T measurement>Isoperibol Calorimeter
8
Adiabatic TEMPERATURE CHANGECombustion calorimeter
Local
T control
Region
T change
High heat capacityReasonable time constant
Fixe
d T
emp
erat
ure
dT/dt = u + k(TJ - T)
T(t) = T - (T - Ti)exp{- k(t – ti)}
T(t) = Ai + Bi t + Ci t2 + Di t3
ISOPERIBOLLong time to reach the temperatureStationary and uniform temperature
T
Tf
(tx)Te
mp
erat
ure
, T
t
c
t
b
tx
main period
T i
(tx)
(a)
A
BTf
(tc)
T i
(tb)
Example ..Combustion bomb
9
Local
T control
Region
T change
High heat capacityReasonable time constant
Fixe
d T
emp
erat
ure
T
T (tx)f
T' (t’x)f
Tem
per
atu
re,
T
tcTime, ttb tx t’x
Polynomial
Exponential
main period
(b)
T (tc)
dT/dt = u + k(TJ - T)
T(t) = T - (T - Ti)exp{- k(t – ti)}
T(t) = Ai + Bi t + Ci t2 + Di t3
ISOPERIBOLLong time to reach the temperatureStationary and uniform temperature
Combustion calorimeter
10
Local
T control
Region
T change
High heat capacityReasonable time constant
Fixe
d T
emp
erat
ure
Heat/energy content of :
Materials
Food
Fuels
Chemicals
Typical Comercial Combustion calorimeter
11
DSCSmal samples and low HEAT change involved
Differential Calorimetry / Microcalorimetry
temperature flutuation of the furnace
Strategy to cancel :
heat capacity of the cell/container
Differential Scanning Calorimetry / Microcalorimetry
temperature flutuation of the furnace
Strategy to cancel :
heat capacity of the cell/container
Sample temperature correction
Scanning > Temperature scan rate
DSCSmal samples and low HEAT change involved
Amostra e referência
instalados no mesmo
forno
Termopares
Amostra Referência
Amostras e referência em
Fornos independentes
Sensor de fluxo e aquecedor
Amostra Referência
DSCSmal samples and low HEAT change involved
Heat Flow DSC Power compensationDSC
16II Jornadas Nacionais de Caracterização de Materiais
Differential Scanning Calorimetry / Microcalorimetry
Scanning > Temperature scan rate
Ionic liquid
Thermal & Phase Behavior ….
CnC1im [PF6]
Differential Scanning Calorimetry
Thermal Behavior
CAL ...n=6
19
Differential Calorimetry / Microcalorimetry
Scanning > Temperature scan rate
Flash Differential Scanning Calorimetry (Flash DSC)
20
Differential Calorimetry / Microcalorimetry
Scanning > Temperature scan rate (cooling)
Flash Differential Scanning Calorimetry (Flash DSC)
21
Differential Calorimetry / Microcalorimetry
Scanning > Temperature scan rate (cooling)
Flash Differential Scanning Calorimetry (Flash DSC)
Low-tech ???
Quite high-tech!!
22
Calvet Microcalorimetry drop methodDirect determination of vaporization enthalpies
Capilary tubes: 20 – 30 mgSample: 3 – 5 mg ∆g
cr/lHo
m (T=298.15 K) = ∆g, Tcr/l, 298.15 KHo
m —∆T298.15 KHo
m(g)
“Drop methodology”
Tf K
TiK
<T> = 298.15 K
24
Time/ s
0 500 1000 1500 2000 2500 3000
Hea
t fl
ow
/ m
W
-12
-10
-8
-6
-4
-2
0
2
Flu
xo
tér
mic
o /
mW
Tempo / s
Sample Reference
Initial Temperature
Calorimeter
Temperature
Vacuum
~ 100 seconds
Calvet Microcalorimetry drop method
)(0g
l THm
T
.p dT)l(C
15298
0
m
g,
298.15 l, HT
T
p dTgC15.298
)(
K)(298.150
m
g
lH
IL (l, T = 298.15 K) IL (g, T =298.15 K)
IL (l, T ) IL (g, T )
)(0g
l THm
T
.p dT)l(C
15298
0
m
g,
298.15 l, HT
T
p dTgC15.298
)(
K)(298.150
m
g
lH
IL (l, T = 298.15 K) IL (g, T =298.15 K)
IL (l, T ) IL (g, T )
Calvet Microcalorimetry drop method
26
Calvet Microcalorimetry drop methodDirect determination of vaporization enthalpies
“Drop methodology”
TiK
<T> = 298.15 KJACS… Ionic liquids: First direct determination of their cohesive energy
Tf K
29
Drop Differential Microcalorimetry
“Drop methodology”
293.15 K
303.15 K
<T> = 298.15 K
Calorimeter (Tf)293.15 K
Furnace (Ti)303.15 K
Very accurate Heat capacity measurements
Bloco Calorimétrico (Tf)
Oven (Ti)exo
Drop Differential Microcalorimetry
Is proportinal to theArea
Cp
Very accurate Heat capacity measurements
High-Precision Heat Capacity Drop Calorimeter
N
2 4 6 8 10 12 14 16 18 20
Co
p /V
/
J·K
-1·c
m-3
1.86
1.88
1.90
1.92
1.94
1.96
1.98
2.00
2.02
Heat Capacities of Ionic Liquids – Cp /V= f(N), T=298.15 K
Heat Capacity ..Data
CAL ...n=6
Alkyl Side Chain Length effect
CAL ...N=2x6 =12
So
lva
tio
n
AlcoholsIonic Liquids
DifferentialHeat Flux Signal
R S
ITC Isothermal Titration Calorimetry ,
Solvation of alcohols in Ionic Liquids
MOLECULAR PROBES
What solvation says about the Nanostructuration in ILs?
Solvation of alcohols in Ionic Liquids (ITC)
[CN-1C1im][NTf2]
Alkyl side chain length (N = 3 – 13)
AlcoholsTrend Shift .. C6C1imNTf2
MOLECULAR PROBES