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Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany Adsorption Calorimetry: Basics and Applications in Heterogeneous Catalysis Sabine Wrabetz Fritz-Haber-Institut of the Max Planck Society Department of Inorganic Chemistry, 14195 Berlin, Germany, [email protected] Beijing - November 11, 2010
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Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Adsorption Calorimetry:

Basics and Applications

in Heterogeneous Catalysis

Sabine WrabetzFritz-Haber-Institut of the Max Planck Society

Department of Inorganic Chemistry, 14195 Berlin, Germany,

[email protected]

Beijing - November 11, 2010

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

1. Introduction & motivation

2. Adsorptive microcalorimetric setup

3. Power balance of Tian-Calvet calorimeter &

Evolved adsorption heat &

Differential heats of adsorption

4. Volumetric-Barometric System

calibration & measurement of adsorbed amount

5. Obtained physical quantities & evaluation criteria of

the calorimetric results

6. Applications of microcalorimetry in heterogeneous

catalysis

Contents

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Introduction

Calor (Latin): heat, warmth

Metron (Greek): measure

Johan C. Wilcke (1732-1796)

Antoine L. Lavoisier (1743-1794)

and Marie P. Lavoisier

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Introduction

▒ direct method to determine number, strength and energy distribution of the adsorption sitesAdsorption Isothermal Micrcalorimetry

▒ allows measurement of the differential heats (ads. enthalpy) evolved when known amounts of gas probe molecules are adsorbed on the catalyst surface

▒ the evolved heat is related to the energy of the bonds formed between the adsorbed species and the adsorbent and hence to the nature of the bonds and to the chemical reactivity of the surface

▒ adsorption steps, surface reaction processes, and desorption steps

▒ the energetics of these surface physical-chemical events play an important role in the determination of the catalytic properties of the surface

▒ key to the effective use of adsorptive microcalorimetry is the careful choice ofprobe molecules and the adsorption temperature

▒ The data obtained are of substantial importance for comparing theoretical and experimental hypotheses about reaction pathways.

Analyzing of the catalytic data with respect to the surface processes occurring on the catalyst material during adsorptive microcalorimetry.

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

▒ careful choice of probe molecules and the adsorption temperature

▒ metal oxide catalysts provides acid/base properties

strong basic NH3 at RT

weak basic CO at 77 K

acidic CO2 at RT

Brønsted acid sites:

transfer of H+

from OH to

Adsorbate

Lewis acid sites:

coordination to an electron-

deficient metal atom

cusMen+

oxygen vacancy:

O2-

OH-metall cations

under

participation of

oxygen: MexO-y

Motivation: surface sites

▒ use of probe molecules such as educt, intermediate, product or moleculesclosely related to the reactants is an elegant method to study the surfacesites relevant for catalytic reaction Tadsorption < Treaction study of the pure ads. processesTadsorption = Treaction study of the surface chemical events during the reaction

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

1. Introduction & motivation

2. Adsorptive microcalorimetric setup

3. Power balance of Tian-Calvet calorimeter &

Evolved adsorption heat &

Differential heats of adsorption

4. Volumetric-Barometric System

calibration & measurement of adsorbed amount

5. Obtained physical quantities & evaluation criteria of

the calorimetric results

6. Applications of microcalorimetry in heterogeneous

catalysis

Contents

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Equipmentat the Fritz-Haber-Institute

Calorimeter

Sample cell Reference cell

Adsorptive

Microcalorimetry

Volumetric system(probe molecule dosing system)

Sample cell

Isolation

Electronics

Sample cell chamber

Heating

Heat flow

Calorimetric Element

Thermocouple

Body sample holderL = 70 mm

= 15 mm

catalyst

MS 70 Tian-Calvet calorimeterof SETARAM combined with acustom-designed high vacuumand gas dosing apparatus.Karge, H.G. etal., J. Phys. Chem. 98, 1994, 8053.

Calorimetric Element

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

The Calorimetric Element

The sample cell is placed into a

calorimeter element

The cell is surrounded by a thermopile

made of more than 400 conductive

thermocouples in series

Thermopile has 2 functions:

1. heat transfer

2. signal generation

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Heat and Heat Flow

The heat produced by the

adsorption/reaction of a dosed probe

molecule with the catalyst surface

is consumed by 2 processes

1. Increase of the temperature of the

sample cell

2. Once there is a temperature gradient

between cell and surrounding block,

heat flow through the thermopile

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Reference Cell

Setup according to

Tian and Calvet

The calorimetric block consists of

a sample cell and a reference

cell.

The reference cell compensate

external temperature fluctuations

and it provides a good stability of

the baseline.

Measurement of the temperature

difference Δ θ

Reference Sample

Cell Cell

The heat-flow detector gives a

signal “U” which is propotional to

the heat transferred per time unit.

Δ θ

N. C. Cardona-Martinez and J.A. Dumesic, Advances in Catalysis 38 150-243.

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Physisorption and Chemisorption

Physisorption Chemisorption

Type of interaction and

heat of adsorption

(negative enthalpy of

adsorption)

van der Waals forces

10 – 20 kJ/mol

noble gases, CH4, N2

Dipole-dipole

20 – 50 kJ/mol

water on oxides

chemical bonding,

electron transfer

80 – 500 kJ/mol

CO on metals

dissociative adsorption

(O2, H2 on Pt, H2O on

oxides)

Reversibility reversible reversible or irreversible

Speed fast can be slow

(e.g. activated

adsorption)

Coverage multilayers possible monolayer only

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Physisorption and Chemisorption

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

1. Introduction & motivation

2. Adsorptive microcalorimetric setup

3. Power balance of Tian-Calvet calorimeter &

Evolved adsorption heat &

Differential heats of adsorption

4. Volumetric-Barometric System

calibration & measurement of adsorbed amount

5. Obtained physical quantities & evaluation criteria of

the calorimetric results

6. Applications of microcalorimetry in heterogeneous

catalysis

Contents

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Power Balance of Tian-Calvet Calorimeter & Adsorption Heat Signal

The power P [W] necessary to heat the cell by d is

proportional to the heat capacity C [J/K] of the cell dt

dCP

The heat flow [power] is proportional to the

temperature gradient between cell and block and to

the thermal conductivity G [W/K]

GG blockcell )(

Gdt

dCPtotal

gU

Ug

G

dt

dU

g

CPtotal

Total thermal power of cell

The electrical signal is proportional to the temperature

difference; (proportionality factor g=f (number and type of the thermocouple))

The relation between power and electrical signal is then

G [W/K] is constant and if C [J/K] can be considered

constant, then C/G is a constant with units of time G

C

The Tian equation shows that the power is not proportional to

the temperature difference, the power is delayed with respect to

the signal U produced by the celldt

dUU

g

GPtotal

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Evolved Heat & Differential Heats of Adsorption

The integral under the curve is proportional to the evolved

heat

AfdtUg

GQ int

A: area under curve [Vs]

f: calibration factor [J/(Vs)]

The calorimeter can be calibrated

by using an Ohm resistance which

produces a certain amount of heat.

Q = U*I*t

f = (U*I*t) / Aohm resistance [Ws/Vs]

ATdiff nQq ,int )/(Differential heats of adsorption as a

function of coverage can be determined

If heat is released in the cell for a limited period of time,

e.g. through adsorption, then a electrical signal U with an

exponential decrease is obtained .

Calculation of Adsorbed Amount

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

1. Introduction & motivation

2. Adsorptive microcalorimetric setup

3. Power balance of Tian-Calvet calorimeter &

Evolved adsorption heat &

Differential heats of adsorption

4. Volumetric-Barometric System

calibration & measurement of adsorbed amount

5. Obtained physical quantities & evaluation criteria of

the calorimetric results

6. Applications of microcalorimetry in heterogeneous

catalysis

Contents

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Calibration of the volumetric system

Vcal = 31.8 ml

= 134.4 ml

Wall adsorption isotherm reflects number of molecules in thegas phase and on the inner walls.

Cal

DosDosCal

DosCalCalDos V

pp

ppV

...)()()()( 4

,

3

,

2

,,,, iSCiSCiSCiSCigwSC pdpcpbpan

Amount of adsorbed molecules

Determination of the dosed amount

The number of molecules adsorbed

in the (i+1)th step is then

The total number of ads. molecules

in a given steps is

Volumetric-Barometric System

vacuum

probe molecule

sample cell + catalyst

pressure gauge dosing system

DOSING VOLUME VDos

CELL VOLUME

CALIBRATION

VOLUME Vcal

pressure gauge sample cell

vacuum

reference cell

T = constant

nads

p

p

RT

Vppn

DosaftDosbefDos

i

)( ,,

int,

1,,,,1int,1, igwSCigwSCiiads nnnn

1,,,1,, iadsitotadsitotads nnn

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

registered Raw Data

0 2 4 20 22 24 26 28 30 32 343

4

5

6

7

8

9

10

0.0

0.5

1.0

1.5

2.0

Pre

ss

ure

in

do

sin

g v

olu

me

/ h

Pa

Zeit / h

Pre

ss

ure

in

sa

mp

le c

ell

/ h

Pa

20 21 22 23 24 25 26 27 28 29 300.2

0.4

0.6

0.8

1.0

1.2

1.4

0.0

0.5

1.0

1.5

2.0

2.5

3.0

Th

erm

os

ign

al / V

Time / h

Eq

uil

ibri

um

pre

ss

ure

/ h

Pa

Raw data

equilibrium pressure

Raw data

equilibrium pressure and thermosignal (Qint.)

DOSING

VOLUME

CELL VOLUME

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

1. Introduction & motivation

2. Adsorptive microcalorimetric setup

3. Power balance of Tian-Calvet calorimeter &

Evolved adsorption heat &

Differential heats of adsorption

4. Volumetric-Barometric System

calibration & measurement of adsorbed amount

5. Obtained physical quantities & evaluation criteria of

the calorimetric results

6. Applications of microcalorimetry in heterogeneous

catalysis

Contents

Adsorption isotherm qdiff strength of surface sites qdiff = f (nads) distribution of surface sites

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

obtained results

Adsorption Isotherm

nads = f ( pequ.)

nads (total) : overall adsorbed amount under an equilibrium pressure of 95 mbar

nads (irrev.) : chemisorbed amount

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Adsorption Isotherm of propane on 10%V/SBA15 catalyst

active in oxidation of propane

0,00

0,02

0,04

0,06

0,08

0,10

0,12

0,14

0 10 20 30 40 50 60

equilibrium pressure [mbar]

am

ou

nt

of

ad

so

rbe

d p

rop

an

e [

mm

ol

/ g

]

T activation

Analysis

higher order Langmuir model,

Nads - coverage with certain equilibrium pressure

Nmono - monolayer coverage

p - equilibrium pressuren - adsorption order

K/A - adsorption equilibrium constant

R2 - correlation coefficient; goodness of fit

S - stoichiometry

Specific surface area propane = N mono * S * cross-section area propane,T * Avogadro constant

; R2

Freundlich model

The enthalpy of adsorption ΔaH (qdiff )

per site is constant with coverage Θ

The enthalpy of adsorption ΔaH (qdiff )

per site decreases with coverage Θ

10%V/SBA15

dehydration

temperature

Nmono

µmol *g-1

n R2

Spropanem2*g-1

BETSN2

m2*g-1

373 K 0.9 (2) 1.20 (2) 0.99983 226 (10) 329 (4)

573 K 1.3 (4) 1.22 (2) 0.99982 304 (10)

673 K 1.2 (3) 1.22 (2) 0.99905 290 (10)

R2=0.99983

R2=0.99853

R2=0.99973

higher order Langmuir

0 10 20 30 40 50 60

0.00

0.02

0.04

0.06

0.08

0.10

0.12

0.14 Higher order Langmuir model

1st order Langmuir model

Freundlich model

N / m

mo

l*g

px,i

/ mbar

n = 1 non-dissociative ads.

n > 1 dissociative ads. ;

activated ads.

evaluation criteria

Analysis of the adsorption isotherm

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

obtained results

Differential heat versus the nads

Differential heat

Adsorbed volume

Enthalpy of condensation

strongLewis

acid sitesBrønstedacid sites

Homogeneous acid strength

Heterogeneousacid site

Interaction between adsorbed molecules

A. Auroux, Lecture Oct. 23,2009

Classical calorimetric curveDifferential heat

Adsorbed volume

Enthalpy of condensation

strongLewis

acid sitesBrønstedacid sites

Homogeneous acid strength

Heterogeneousacid site

Interaction between adsorbed molecules

A. Auroux, Lecture Oct. 23,2009

Differential heat

Adsorbed volume

Enthalpy of condensation

strongLewis

acid sitesBrønstedacid sites

Homogeneous acid strength

Heterogeneousacid site

Interaction between adsorbed molecules

A. Auroux, Lecture Oct. 23,2009

Classical calorimetric curve

Classical Calorimetric Curve

Initial differential heat

Slope: heterogeneously distributed andenergetically different adsorption

sites

Completionof monolayer

Plateau: homogeneously distributed andenergetically uniform adsorption sites

Amount of adsorbed propane on phase-pure MoVTeNb#6059 / mmol/g

Diffe

rential h

ea

t o

f a

dso

rbe

d

pro

pa

ne

/ k

J/m

ol

0.0 0.1 0.2 0.3 5 10 15 20 25 30

0

100

200

300

400

500

600

700

800

Dif

fere

nti

al

heat

of

ox

yg

en

ad

s. [

kJ/

mo

l]

amount of ads. oxygen [ mol/g]

Dif

fere

nti

al h

ea

t o

f a

ds

orb

ed

o

xyg

en

ato

m / k

J/m

ol

High diff. heats & heat oscillation :dynamic ads. processchemisorption-oxidation-reaction

Amount of ads. O2 on Pd/N-CNF at Treact. / µmol/g

most active

less active

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

q int (ads.) > q int (des.) partially irreversible ads.;activated ads. process

q int (ads.) < q int (des.) instability of the catalyst in the presence of probe molecule

q int (ads.) = q int (des.) reversible ads. process

+ qintegral (ads.) = 7892 mJ

- qintegral (des.)= 6560 mJ

Integral heat signal of

adsorption and desorptionstepwise adsorption of propane on MoVTeNb oxide at 313K

0 2000 4000 6000 8000 10000 12000 14000

0.430

0.435

0.440

0.445

0.450

0.455

0.460

SZ

the

rmo

sig

na

l / V

time / s

Background of the thermo signal

during the stepwise adsorptionstepwise n-butane ads. on sulf. ZrO2 at 313 K

Background deviates from the base-line

Adsorption process is accompanied by

secondary processes

e.g. during n-butane ads. a partial

isomerization of n-butane to isobutane

in the calorimeter cell was observed

Evaluation criteriaof the calorimetric experiment

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

0xxexpAyy 0

200 300 400 500 600 700 800 9000.2

0.4

0.6

0.8

1.0

Th

erm

osi

gn

al [

V]

Response time / 10.3 h

C

Shape of the integral heat signalO2 adsorption on 2%Pd/N-CNF473K at 353K=Treaction

0 10 20 30 40

0.30

0.35

0.40

Th

erm

osi

gn

al [

V]

Response time / 0.4 h

K(t)= 377 s

A

2 μmol/g oxygen

Evaluation criteriaof the calorimetric experiment

300 310 320 330 340 350 3600.2

0.4

0.6

0.8

1.0

Th

erm

osi

gn

al [

V]

Response time / 0.7 h

K(t)= 998 s

B

14 μmol/g oxygen 0.039 μmol/g oxygen

quasi pure dissociative

oxygen chemisorption

on Pdnads.↑

oxygen chemisorption

combined by

secondary processes

Determination of the time constant of the integral heat signal

8.8 104 8.85 104 8.9 104 8.95 104 9 104 9.05 104 9.1 104

Time (s)

1.24

1.26

1.28

1.3

1.32

1.34

1.36

Sig

nal T

herm

ocolu

mns (

V)

R=1kΩ →27.45 mJ

→ (calorimeter+cell) ~265 s

8000 9000 1 104 1.1 104 1.2 104 1.3 104 1.4 104

Time (s)

0.52

0.54

0.56

0.58

0.6

0.62

Sig

nal T

herm

ocolu

mns (

V)

gamma Al2O3, Methanol-Ads, 40grd, 3. Ads.-Step

(A+B*exp(-(x-C)/D),A=0.5438~,B=0.0249~,C=9237.80~,D=722.458~))

5.9 µmol/g propylene

adsorbed on MoVTeNb

at 313 K

= 287 s ~ cal+cell

pure ads. process

4.8 µmol/g

methanol adsorbed

on Al2O3 at 313 K

= 722 s > cal+cell

ads. + reaction

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

1. Introduction & motivation

2. Adsorptive microcalorimetric setup

3. Power balance of Tian-Calvet calorimeter &

Evolved adsorption heat &

Differential heats of adsorption

4. Volumetric-Barometric System

calibration & measurement of adsorbed amount

5. Obtained physical quantities & evaluation criteria of

the calorimetric results

6. Applications of microcalorimetry in heterogeneous

catalysis

Contents

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Applications

Probe

molecule

Catalyst / Activation / Catalytic activity T adsorption

[K]

q initial+

[kJ/mol]

n-butane 0.5wt%Pt/H-Mordenite / H2 reduced at 648 K /less active 313 350

n-butane 0.5wt%Pt/H-Mordenite / dehydr. at 723 K / active 313 42

n-butane 3.5wt% VOx-Al2O3 / H2 reduced at 773 K /active 313 63

n-butane Θ Al2O3 / H2 reduced at 773 K /non-active 313 35

propane 10 wt% VxOy-SBA15 / dehydrated at 373 K / active

573 K

637K

313 45

80

160

propane 3 wt% VxOy-SBA15 / dehydrated at 373 K / active 313 45

propane SBA15 / dehydrated at 373 K / non-active 313 32

propane hydrothermal synth. – M1 /dehydr. at 423 K /active, 58* 313 71

propane precipitation – M1 /dehydrated at 423 K /active , 43* 313 56

propane SHWVT ** – M1 / dehydrated at 423 K / active, 5* 313 64

CO2

CNFox functionalized by NH3 at 873 K

673 K

473 K

313

150

50

90

CO2 Fe-CNT / dehydrated at 373 K

FeIO-XT 24PS-CT / dehydrated at 373 K

313 272

191

O2

2wt%Pd#/N-CNT873K/ dehydrated at 353 K

2wt%Pd#/N-CNT473K/ dehydrated at 353 K

2wt%Pd/CNT/ H2 reduction at 423 K

353

353

313

500-700

500

175

O2 *** precipitation – M1 / H2 activated at 653 K

precipitation – M1 / propane activated at 653 K

473 218

257

O2 *** 8wt%VxOy-SBA15 / dehydrated at 673 K 473 248

Selected calorimetric measurements on supported metal oxide and mixed metal oxides .

+ We have adopted the calorimetric sign criterion (positive energetic quantity for an exothermic process).* partial oxidation of propane (POP); Selectivity to acrylic acid [mol-%]** superheated-water vapor treatment (SHWVT)*** cooperation with Instituto de Quimica Fisica “Rocasolano", CSIC, Madrid (Spain)# CNFox functionalized by NH3 at 873K or 473K, Pd catalysts are obtained via sol-immobilization on the CNFs

in which Na2PdCl4, NaBH4 and polyvinylalcohol (PVA) were used . Hence, Pd particles are partially covered by PVA.## Vapor Growth Commercial Carbon Nanofiber; oxygen-containing nanocarbon was obtained by treating with HNO3 at 373 K.

The method was broadly

employed in several projects of

our department and yielded a

surprising spread of energetic

data for the same molecule on

different surfaces .

In addition, we observed

significant differences of the

energetic data for the same

molecule on slightly modified

surfaces.

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

0.0 0.1 0.2 0.3 0.4 0.5

0.000

0.005

0.010

0.015

0.020

0.025

0.030

0.035

am

ou

nt

of

ad

so

rbe

d C

O

/ m

mo

l*g

euilibrium pressure of CO / mbar

Model: higher order Langmuir model

qdiff = 200kJ/mol = constant versus nads

R2

= 0.88731

Nmono = 0.02631 (1st

run) - 0.00583(2nd

run)

K = 1662.35201 --> irreversibility

n = 1.15679

CO adsorption on Pt/Al2O3 at 40°C

Differential heat of adsorbed CO Adsorption isotherm of CO

n ads. (irreversible)

= 20.4 µmol/g

Pt-CO = 1:1 = 206 kJ/mol Pt2-CO = 94 kJ/mol[

J.Therm. Anal. Cal., 82, (2005) 105

Saturation

concentration

Saturation concentration

SCO = Nmono * S * cross-section-area CO,T * Avogadro constant

SCO = 20.4*10-6mol/g * 1* 16.2*10-20m * 6.022*1023mol-1 = 1.99 m2/g

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

n-butane (educt) adsorption on Pt/H-Mordenite catalyst at 40°C

Aim: structure-activity relationship study of Pt/HM for n-butane isomerization

0 1 2 30

100

200

1600

1800

2000

Time on stream [h]

Ra

te o

f is

om

eri

sa

tio

n [

mo

l/g

.h]

fully H2-reduced Pt/HMcatalyst activated in H2 at 350 oC for 2 h

n-butane isomerisation15 kPa n-butane in H2 at 300 oC

not completely H2-reduced Pt/HMcatalyst activated in H2 at 300 oC for 1 h

0.0 0.1 0.2 0.3 0.4 0.5

40

60

80

300

400

D

iff.

he

at

of

ad

so

rbe

d n

-bu

tan

e [

kJ

/mo

l]Equilibrium pressure of n-butane [mmol/g]

2300 2200 2100 2000 1900 1800

Wavenumber / cm-1

Pt0

Al3+

oct.

Ptx-CO

Ptx+

0.0 0.1 0.2 0.3 0.4 0.5

40

60

80

300

400

D

iff.

he

at

of

ad

so

rbe

d n

-bu

tan

e [

kJ

/mo

l]Equilibrium pressure of n-butane [mmol/g]

2300 2200 2100 2000 1900 1800

Wavenumber / cm-1

Pt0

Al3+

oct.

Ptx-CO

Ptx+

Differential heat of ads. n-butane at 40 C

IR spectra of ads. CO at RT

at 0.7 mbar

200 mol/g

450 mol/g

The active states of Pt/HM are characterized by:

a small amount of strong Lewis acid sites (Al3+oct., extraframework alumina)

well dispersed metallic platinum particles (1-3 nm)

higher number of n-butane adsorption sites

weak interaction of the surface acid sites with n-butane.The weaker interaction with the alkane is apparently favorable for the catalytic performance; perhaps because of facile product desorption.

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

20

30

40

50

60

70

80

0.00 0.01 0.01 0.02 0.02 0.03 0.03 0.04 0.04

Dif

fere

nti

al h

eat

[k

J/m

ol]

Amount of neo-pentane or iso-butane sorbed [mmol/g]

Fe/sulf.ZrO2 is active in isomerization of n-butane to isobutane at low temp. (100°C)

The scattering of the diff.

heats for iso-butane at low

coverage indicates the

presence of exothermic and

endothermic processes during

the adsorption.

Question: Does iso-butane (product) reacts with surface species

of Fe/sulf. ZrO2 at low temperature ?

Differential heat of adsorbed iso-butane & neo-pentane at 40 C

3

3

3CH

CH

CH

CH

ads. + reaction

Answer: Yes, iso-butane (product) reacts with surface species of

Fe/sulf. ZrO2 at low temperature.

pure ads.

The neo-pentane heat profile

follow the classical calorimetric

heat profile - heat decreases

with increasing the coverage

3

3

3

CH

C CH

CH3

CH

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

pure-phase MoVTeNb catalyst active indirect oxidation of propane to acrylic acid (aa)

Sabine Wrabetz, Yury V. Kolen’ko, Jutta Kröhnert, Lenard Csepei, Olaf Timpe, Wei Zhang, Annette Trunschke, and Robert Schlögl,

Characterization of MoVTeNb catalyst in their as prepared and active state by adsorption microcalorimetry and -FTIR spectroscopy ; in preparation 2010.

Aim: study of the post-reaction state of the surface “used catalyst” in

comparison with the prepared state of the surface “fresh catalyst”

Differential heat of propane adsorption at 40°C

phase-pure M1, Saa = 53%Spropane=11.4m2/g

oxidized M1, Saa = 37%Spropane=10.3m2/g

MoV oxide, Saa = 1.8%

Spropane=13.4m2/g

Saa → homogeneity → strength of interaction between educt and surface sites → density of propane ads. sites energetically uniform ( which is apparently favorable for catalytic performance;

ads. sites perhaps because of facile intermediate desorption)

the prepared state of the surface is different from the post-reaction state of the surface

dynamic surface during reaction

Amount of propane adsorption / mmol/m2

80

70

60

50

40

30

20

10Diffe

rential heat

/

kJ/m

ol

0 0.001 0.002 0.003 0.004 0.005 0 0.001 0.002 0.003 0.004 0.005 0 0.001 0.002 0.003 0.004 0.005

Amount of propane adsorption / mmol/m2Amount of propane adsorption / mmol/m2

MoV

Mo

Nb

Te

O

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

quasi in-situ microcalorimetry

Aim: Study of the educt and product interaction with the surface of sulf. ZrO2

if the surface at the state of highest activity in the n-butane isomerization

n-butane &

iso-butane ads.

at 313 K

after degassing at 378K

0 20 40 60 80 100 120 140

0

5

10

15

20

25

30

35

40

45

Rate

of

Isom

erization (

mol h

-1 g

-1)

Time on Stream (min)

n-butane isomerisation at 378Kin the flow-type calorimetric sample cell

0

10

20

30

40

50

60

70

80

0,000 0,005 0,010 0,015 0,020 0,025D

iffe

ren

tia

l h

ea

t [k

J/m

ol]

Amount of adsorbed n-butane & iso-butane [mmol/g]

K n-butane= kads./kdesorp. = 0.162

K iso-butane= kads. /kdesorp. = 0.011

The state of maximum activity of sulf. ZrO2 is characterized by:

A stronger interaction with n-butane (~70kJ/mol, educt) than with iso-butane (~45kJ/mol, product).

The weak interaction with iso-butane and the equilibrium constant (Kiso-butane=0.011) indicate

an increasing easiness of desorption of iso-butane from the surface sites.

stoppedat

TOS=120min

Differential heat at 40 C

Wrabetz, Sabine; Yang, Xiaobo; Tzolova-Müller, Genka; Schlögl, Robert; Jentoft, Friederike C., J. of Catalysis 269 /2 (2010) 351 - 359.

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

CNF surface chemistry plays a crucial

role in Metal/CNF interaction

Fe/N-CNF873K is the best catalyst in

electrocatalytic conversion of CO2 .

Pd/N-CNF873K is the best catalyst in

oxidation of benzyl alcohol to

benzaldehyde

Microcalorimetric titration of basic sites on N-CNFs by CO2 adsorption at 40°C

Different oxygen and nitrogen species in CNFs

Oxidation of VGCNF by HNO3 at 373K for 2h and

amination using NH3 at 473/673/873 K.

0 2 4 6 8

20

40

60

80

100

120

140

160

a)

0 2 4 6

b)

0 2 4 6

c)

0 1 2 3

d)

partially irreversible

adsorbed

Differential heat of adsorbed CO2

N-CNF873K N-CNF473K N-CNF673K VGCNF

Arrigo, Rosa; Haevecker, Michael; Wrabetz, Sabine; Blume, Raoul; Lerch, Martin; McGregor, James; Parrott, Edward; Zeitler, J; Gladden,

Lynn; Knop-Gericke, Axel; Schlogl, Robert; Su, Dangsheng, Journal of the American Chemical Society 132/28 (2010) 9616 - 9630.

depending on the Tamination the N-CNF

surface provides energetically different

basic sites which are heterogeneously

distributed

Amount of adsorbed CO2 [ mol/g]

Diffe

rential h

ea

t o

f a

dso

rbe

d C

O2

[kJ/m

ol]

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Conclusion

very sensitive and hence a selective surface characterization methodbut very time consuming ( ~1 week for 1 experiment)

The nature of the reactive surface sites can be studied by

measuring the thermal effects during the reaction.

The knowledge about the energetics of the surface chemical

events helps better to understand the catalytic properties of the

surface and hence the catalytic reaction characteristics.

Microcalorimetry alone or combined with to other techniques, is applied

for the characterization of catalysts, supports and adsorbents, and to

the study of catalytic reactions (adsorption-desorption phenomena).

The calorimetric data obtained are of substantial importance for comparing

theoretical and experimental hypotheses about reaction pathways.

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

A. Auroux “Thermal Methods: Calorimetry, Differential Thermal Analysis, and

Thermogravimetry” in “Catalyst characterization: physical techniques for solid

materials”, Eds. B. Imelik, J.C. Vedrine, Plenum Pr., New York 1994

E. Calvet, H. Prat, H.A. Skinner “Recent progress in microcalorimetry”,

Pergamon Pr., Oxford1963

B. E. Handy, S.B. Sharma, B.E. Spiewak and J.A. Dumesic, “A Tian-Calvet

heat-flux microcalorimeter for measurement of differential heats of adsorption”,

Meas. Sci. Technol. 4 (1993) 1350-1356.

N. C. Cardona-Martinez and J.A. Dumesic, “Application of Adsorption

Microcalorimetry to the Study of heterogeneous Catalysis”, Advances in

Catalysis 38 150-243.

Z. Knor, “Static Volumetric Methods for Determination of Adsorbed Amount of

Gases on Clean Solid Surface”, Catalysis Reviews 1 (1) (1968) 257-313.

S. Černý and V. Ponec, „ Determination of Heat of Adsorption on Clean Solid

Surfaces”, Catalysis Reviews 2 (1) (1969) 249-322.

Literature

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Acknowledgement of financial support

Thanks the European Union for finacial support of the project

“Integrated Design of Nanostructured Catalytic Materials for a

Sustainable Development” .

Financial support for “Brückenschläge zwischen idealen und realen

Systemen in der Heterogenen Katalyse“ through DFG priority

program 1091 (JE 267/1-3) is gratefully acknowledged.

The SFB-project “Struktur, Dynamik und Reaktivität von

Übergangsmetalloxid- Aggregaten“ was sponsered by DFG.

Author thanks the DFG for providing an Emmy Noether

fellowship to the project leader “propane oxidation over

V/SBA15” Prof. C. Hess

The project “Pt-doped H-mordenite is used as a solid acid

catalyst for the isomerization of light alkanes” was financially

supported by BMBF grant 03C0307E.

Sabine Wrabetz, Electronic Structure and Adsorption / Metals, Dept. AC, Fritz Haber Institute of the MPG, Berlin, Germany

Thank you for your attention !


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