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ME 475/675 Introduction to Combustion
Lecture 16 Chemical kinetics
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Announcements HW 6 Monday, Thank you for coming early to the midterm.
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Chapter 4 Chemical Kinetics
Describes rates at which: Reactants are consumed and products are produced, Thermal energy is produced (exothermal) or consumed (endothermal) βGlobalβ Combustion Reaction (molar based) 1 πΉ ππ’ππ +πππ₯ ππ₯ππππ§ππ βπππ(πππππ’ππ‘π ) On what does reaction rate depend? In general it: Increases with reactant molar concentrations and temperature Decreases with product molar concentrations Define Molar Concentration of species π, π (number density) π = π π π = π π π π = π π π π
π’ π = π π π
π’ π π π = π π
π’ π = π π π ππ πππ₯ π = π π Ο ππ πππ₯ Units: 1 πππππ π π π 100ππ ππππ π 1 πππππ π = ππππ π ππ Number of molecules n = N*NAV Avogadro's Number π π΄π =6.022β ππππππ’πππ πππππ Number of molecules in 12 kg of C12 π π΄ =6.022β ππππππ’πππ ππππ Number of molecules in 12 g of C12
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Global Rate Equations π πΉ ππ‘ =β π πΊ π πΉ π ππ₯ π βBlack Boxβ Approach
πΉ+πππ₯βπππ π πΉ ππ‘ =β π πΊ π πΉ π ππ₯ π π πΊ π = Global rate coefficient, strongly dependent on temperature T π,π= Reaction order of Oxidizer and Fuel π+π= Overall reaction order Different π πΊ π and π,π for different temperature and pressure ranges pp (Chapter 5) βBlack Boxβ Approach Based on measurements and correlations (empirical) Not based on βcausalityβ understanding individual reaction steps, which may involve intermediate species Overall global reaction may involve many intermediate reaction steps
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Multi-step Reaction Example Overall Reaction: 2 π» 2 + π 2 β2 π» 2 π (hydrogen combustion) H-H O-O H-O-H Many possible intermediate, elementary reactions steps Each step breaks one bond, and forms one bond π» 2 + π 2 βπ» π 2 +π» (π» π 2 = hydroperoxy radical) H-H O-O H-O-O H π»+ π 2 βππ»+π H O-O O-H O ππ»+ π» 2 β π» 2 π+π» O-H H-H H-O-H H π»+ π 2 +πβπ» π 2 +π (π= passive species, process termination step) H O-O H-O-O Free Radicals = reactive, short-lived molecules with unpaired electron Unpaired with proton, Charged, in this example: π» π 2 , π», ππ», π
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Bimolecular Reactions
Two molecules react, form two new molecules π΄+π΅βπΆ+π· For example: one step of multi-step reaction: π» 2 + π 2 βπ» π 2 +π» Rate for this elementary reaction π π΄ ππ‘ =β π πππππππ π΄ 1 π΅ 1 = π π΅ ππ‘ =β π πΆ ππ‘ =β π π· ππ‘ π π΅πππππ =ππ π , but is theoretically-based Units π πππππππ = π 3 ππππβπ Use collision theory to find π π΅πππππ During time π‘, an A particle, of diameter π, moving at speed π£, βsweepsβ volume π π π£π‘ If it is in a region of stationary B particles, also of diameter π, and number density π π΅ π , then the number of collisions per time is: π π΅ π π π 2 π£ ππππππ ππππ π‘πππ
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Collision Rate between all A and B particles
If all A and B particles are actually moving randomly (with a Maxwellian velocity distribution) with average speed π£ (which depends on temperature) Can be shown (CBS) that the rate at which a single moving particle A (diameter π π΄ ) collides with a field of randomly moving B ( π π΅ ) particles is ππππππ ππππ π ππ π π = 2 π π΅ π π π π΄π΅ 2 π£ π΄ 2 bigger than might be expected from last expression, due to motion Where π π΄π΅ = π π΄ + π π΅ 2 and CBS π£ π΄ = 8 π π΅ π π π π΄ Now consider many A particles, with number density π π΄ π The number of collisions between all Aβs and Bβs per volume and time is π π΄π΅ π = π π΄ π π π΅ π π π π΄π΅ π π΅ π ππ π π΄ = π π΄ π π΄π , π π΅ = π π΅ π π΄π ,and CBS π= π π΄ π π΅ π π΄ + π π΅
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Relation to reaction rate
β π π΄ ππ‘ = π π΄π΅ π ππππππππππ‘π¦ ππππππ πππ πππππ π‘π πππππ‘πππ ππππππ π΄ ππππππ’πππ π΄ = π π΄π΅ π π« 1 π π΄π π«=πβππ₯π β πΈ π΄ π
π’ π π= Steric factor (collision of geometry) < 1 ππ₯π β πΈ π΄ π
π’ π = Fraction of all collisions with energy greater than activation energy πΈ π΄ CBS β π π΄ ππ‘ = π π΄ π π΄π π π π΅ π π΄π π π π π΄π΅ π π΅ π ππ πβππ₯π β πΈ π΄ π
π’ π π π΄π β π π΄ ππ‘ =π π π΄π π π΄π΅ 2 π΄ π΅ 8π π π΅ π π ππ₯π β πΈ π΄ π
π’ π =π π π΄ π΅ π π =π π π΄π π π΄π΅ π π π΅ π π ππ₯π β πΈ π΄ π
π’ π but π and πΈ π΄ = ?
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Arrhenius Form For a limited temperature range Three parameter form:
π π =π΄ππ₯π β πΈ π΄ π
π’ π π΄= pre-exponential factor Three parameter form: π π =π΄ π π ππ₯π β πΈ π΄ π
π’ π π΄, π and πΈ π΄ values are tabulated pp 112 (Chapter 4)
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Other Elementary Reactions
Uni-molecular (isomerization or decomposition) π΄βπ΅ (change in structure) π΄βπ΅+πΆ (examples π 2 β2π; π» 2 β2π») Measurements show that At high pressures β π π΄ ππ‘ = π π’ππ π΄ (first order in pressure) At low pressures β π π΄ ππ‘ = π π’ππ π΄ π (Explain this later): π= other molecules with which A may collide Ter-molecular π΄+π΅+πβπΆ+π Recombination (π»+π»+πβ π» 2 +π; π»+ππ»+πβ π» 2 π+π) β π π΄ ππ‘ = π π‘ππ π΄ π΅ π Third order π= third body, caries energy away If A = B (i.e. π΄+π΄+πβπΆ+π), then β π π΄ ππ‘ = 2π π‘ππ π΄ π΄ π
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Multi-step Mechanism Reaction Rates
A sequence of reactions leading from Reactants to Products Example: hydrogen combustion (forward and reverse reactions) L steps, i = 1, 2,β¦ L N species, j = 1, 2,β¦ N R1: π» 2 + π 2 π πΉ1 , π π
1 π» π 2 +π» π=1 R2: π»+ π 2 π πΉ2 , π π
2 ππ» +π π=2 R3: ππ»+ π» 2 π πΉ3 , π π
3 π» 2 π+π» π=3 R4: H+ π 2 +π π πΉ4 , π π
4 π» π 2 +π π=4 Number of steps: L = 4 Number of Species (π= π» 2 , π 2 , π» π 2 ,π», ππ», π, π» 2 π,π): N = 8 8 time-dependent unknown molar concentrations: π π‘ Need 8 equations (constraints)
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Species net reaction rates
j = 1 π π 2 ππ‘ = π π
1 π» π 2 π» + π π
2 ππ» π + π πΉ3 ππ» π» 2 β π πΉ1 π» 2 π 2 β π πΉ2 π» π 2 β π πΉ4 π» π 2 π j = 2 π π» ππ‘ = π πΉ1 π» 2 π 2 + π π
2 ππ» π + π πΉ3 ππ» π» 2 + π π
4 π» π 2 π β π π
1 π»π 2 π» β π πΉ2 π» π 2 β π π
3 π» 2 π π» β π πΉ4 π» π 2 π j = 3, 4, β¦8 Book describes compact notation
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What happens at equilibrium?
A general reaction ππ΄+ππ΅ π π π π ππΆ+ππ· π π΄ ππ‘ =π β π π π΄ π π΅ π + π π πΆ π π· π At equilibrium π π΄ ππ‘ =0, so π π π΄ π π΅ π΅ = π π πΆ π π· π π π π π π π = πΎ πΆ π = πΆ π π· π π΄ π π΅ π πΎ πΆ π = Equilibrium Constant based on molar concentration
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End 2017
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Relationship between Rate Coefficients and Equilibrium Constant (Chapter 2)
ππ΄+ππ΅ π π π π ππΆ+ππ· πΎ π π = π πΆ π π π π π· π π π π π΄ π π π π π΅ π π π π = π π π
π’ π πΎ πΆ π = π πΉ π π π
π = πΆ π π· π π΄ π π΅ π = π πΆ π
π’ π π π π· π
π’ π π π π΄ π
π’ π π π π΅ π
π’ π π = π πΆ π π π π π· π π π π π΄ π π π π π΅ π π π π π π
π’ π π+πβ(π+π) π = π π π
π’ π πΎ πΆ π = πΎ π π π π π
π’ π π+πβ(π+π) Or πΎ π π = πΎ πΆ π π
π’ π π π π+πβ(π+π) Note: If π+π=π+π, then πΎ π π = πΎ πΆ π
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Example 4.2 (page 120, turn in next time)
In their survey of experimental determinations of rate constants for the H-H-O system, Nanson and Salimian [reference 10 in book] recommend the following rate coefficient for the reaction ππ+πβπ+ π 2 . π π =2.80β π 1.0 ππ₯π β20,820 π = ππ 3 ππππβπ Determine the rate coefficient at 2300 K for the reverse reaction, i.e. π+ π 2 βππ+π
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