The Mayo-Lewis Copolymerization Model - rohan.sdsu.edu
Transcription
The Mayo-Lewis Copolymerization Model - rohan.sdsu.edu
Chemistry Old Models New Models The Mayo-Lewis Copolymerization Model Vadim Ponomarenko Department of Mathematics and Statistics San Diego State University CSRC Colloquium Series April 27, 2007 http://www-rohan.sdsu.edu/∼vadim/mayolewis.pdf Chemistry Old Models Outline Chemistry Old Models New Models New Models Chemistry Old Models Outline Chemistry Old Models New Models New Models Chemistry Old Models New Models Basics A polymer is a large molecule, built up from many small monomers. We study the building process. Consider the polymer as a long necklace. Note: Branching (non-linear polymers) is possible, but not today. Step Polymerization All monomers and (partial) polymers are simultaneously reactive. (attach two small necklaces) Chain Polymerization (our interest today) A small amount of reactive (partial) polymer absorbs monomers one at a time. (add one bead to a necklace) Chemistry Old Models New Models Basics A polymer is a large molecule, built up from many small monomers. We study the building process. Consider the polymer as a long necklace. Note: Branching (non-linear polymers) is possible, but not today. Step Polymerization All monomers and (partial) polymers are simultaneously reactive. (attach two small necklaces) Chain Polymerization (our interest today) A small amount of reactive (partial) polymer absorbs monomers one at a time. (add one bead to a necklace) Chemistry Old Models New Models Basics A polymer is a large molecule, built up from many small monomers. We study the building process. Consider the polymer as a long necklace. Note: Branching (non-linear polymers) is possible, but not today. Step Polymerization All monomers and (partial) polymers are simultaneously reactive. (attach two small necklaces) Chain Polymerization (our interest today) A small amount of reactive (partial) polymer absorbs monomers one at a time. (add one bead to a necklace) Chemistry Old Models New Models Basics A polymer is a large molecule, built up from many small monomers. We study the building process. Consider the polymer as a long necklace. Note: Branching (non-linear polymers) is possible, but not today. Step Polymerization All monomers and (partial) polymers are simultaneously reactive. (attach two small necklaces) Chain Polymerization (our interest today) A small amount of reactive (partial) polymer absorbs monomers one at a time. (add one bead to a necklace) Chemistry Old Models New Models Chain Polymerization These are classified into types, based on underlying reaction: Ionic (cationic/anionic). More complex, less common, not today. Radical Simple, common. A molecule with a free radical is highly reactive. It bonds with a monomer, which in turn gains a free radical. Chemistry Old Models New Models Chain Polymerization These are classified into types, based on underlying reaction: Ionic (cationic/anionic). More complex, less common, not today. Radical Simple, common. A molecule with a free radical is highly reactive. It bonds with a monomer, which in turn gains a free radical. Chemistry Old Models New Models Chain Polymerization These are classified into types, based on underlying reaction: Ionic (cationic/anionic). More complex, less common, not today. Radical Simple, common. A molecule with a free radical is highly reactive. It bonds with a monomer, which in turn gains a free radical. Chemistry Old Models New Models Radical Chain Polymerization Life Cycle Step 1: Radicals are born. (initiator radicals) Processes used: thermal, redox, photochemical, ionizing radiation, etc. Very small amount, compared to monomers. Step 2..1000: Radicals react with monomers. radical chain + monomer ⇒ longer radical chain Final Step: Radicals die. Two radical chains react with each other. Coupling: they become nonradical and merge Disproportionation: they become nonradical and don’t merge Chemistry Old Models New Models Radical Chain Polymerization Life Cycle Step 1: Radicals are born. (initiator radicals) Processes used: thermal, redox, photochemical, ionizing radiation, etc. Very small amount, compared to monomers. Step 2..1000: Radicals react with monomers. radical chain + monomer ⇒ longer radical chain Final Step: Radicals die. Two radical chains react with each other. Coupling: they become nonradical and merge Disproportionation: they become nonradical and don’t merge Chemistry Old Models New Models Radical Chain Polymerization Life Cycle Step 1: Radicals are born. (initiator radicals) Processes used: thermal, redox, photochemical, ionizing radiation, etc. Very small amount, compared to monomers. Step 2..1000: Radicals react with monomers. radical chain + monomer ⇒ longer radical chain Final Step: Radicals die. Two radical chains react with each other. Coupling: they become nonradical and merge Disproportionation: they become nonradical and don’t merge Chemistry Old Models New Models Radical Chain Polymerization Life Cycle Step 1: Radicals are born. (initiator radicals) Processes used: thermal, redox, photochemical, ionizing radiation, etc. Very small amount, compared to monomers. Step 2..1000: Radicals react with monomers. radical chain + monomer ⇒ longer radical chain Final Step: Radicals die. Two radical chains react with each other. Coupling: they become nonradical and merge Disproportionation: they become nonradical and don’t merge Chemistry Old Models New Models Radical Chain Polymerization Life Cycle Step 1: Radicals are born. (initiator radicals) Processes used: thermal, redox, photochemical, ionizing radiation, etc. Very small amount, compared to monomers. Step 2..1000: Radicals react with monomers. radical chain + monomer ⇒ longer radical chain Final Step: Radicals die. Two radical chains react with each other. Coupling: they become nonradical and merge Disproportionation: they become nonradical and don’t merge Chemistry Old Models New Models Radical Chain Polymerization Life Cycle Step 1: Radicals are born. (initiator radicals) Processes used: thermal, redox, photochemical, ionizing radiation, etc. Very small amount, compared to monomers. Step 2..1000: Radicals react with monomers. radical chain + monomer ⇒ longer radical chain Final Step: Radicals die. Two radical chains react with each other. Coupling: they become nonradical and merge Disproportionation: they become nonradical and don’t merge Chemistry Old Models New Models Radical Chain Polymerization Life Cycle Step 1: Radicals are born. (initiator radicals) Processes used: thermal, redox, photochemical, ionizing radiation, etc. Very small amount, compared to monomers. Step 2..1000: Radicals react with monomers. radical chain + monomer ⇒ longer radical chain Final Step: Radicals die. Two radical chains react with each other. Coupling: they become nonradical and merge Disproportionation: they become nonradical and don’t merge Chemistry Old Models New Models Radical Chain Polymerization Life Cycle Step 1: Radicals are born. (initiator radicals) Processes used: thermal, redox, photochemical, ionizing radiation, etc. Very small amount, compared to monomers. Step 2..1000: Radicals react with monomers. radical chain + monomer ⇒ longer radical chain Final Step: Radicals die. Two radical chains react with each other. Coupling: they become nonradical and merge Disproportionation: they become nonradical and don’t merge Chemistry Old Models New Models Steady-State for Radicals Radicals are created at a constant rate, and destroyed at a rate proportional to the square of their concentration. dx dt = a − bx 2 ; has solution x(t) = As t → ∞, x(t) → q q a b a b. In practice, ∞ is actually quite small. √ tanh((t + c) ab). Chemistry Old Models New Models Steady-State for Radicals Radicals are created at a constant rate, and destroyed at a rate proportional to the square of their concentration. dx dt = a − bx 2 ; has solution x(t) = As t → ∞, x(t) → q q a b a b. In practice, ∞ is actually quite small. √ tanh((t + c) ab). Chemistry Old Models New Models Steady-State for Radicals Radicals are created at a constant rate, and destroyed at a rate proportional to the square of their concentration. dx dt = a − bx 2 ; has solution x(t) = As t → ∞, x(t) → q q a b a b. In practice, ∞ is actually quite small. √ tanh((t + c) ab). Chemistry Old Models New Models Polymerization Summary Molecule Concentrations Molecule Monomers Radicals Polymers Initial high none none In Progress decreasing tiny increasing Final low none high We want to understand the rate at which this happens. ‘kinetics’ Only monomer concentrations are efficiently measured, through various spectroscopies (IR, UV, NMR). Chemistry Old Models New Models Polymerization Summary Molecule Concentrations Molecule Monomers Radicals Polymers Initial high none none In Progress decreasing tiny increasing Final low none high We want to understand the rate at which this happens. ‘kinetics’ Only monomer concentrations are efficiently measured, through various spectroscopies (IR, UV, NMR). Chemistry Old Models New Models Polymerization Summary Molecule Concentrations Molecule Monomers Radicals Polymers Initial high none none In Progress decreasing tiny increasing Final low none high We want to understand the rate at which this happens. ‘kinetics’ Only monomer concentrations are efficiently measured, through various spectroscopies (IR, UV, NMR). Chemistry Old Models Outline Chemistry Old Models New Models New Models Chemistry Old Models Single Monomer Polymerization With one type of polymer, the relevant DE is: dx dt = −k rx x is the monomer concentration r is the (constant) radical concentration k is the goal (rate constant) Too simple for chemists to screw up. Also, of limited interest. New Models Chemistry Old Models Single Monomer Polymerization With one type of polymer, the relevant DE is: dx dt = −k rx x is the monomer concentration r is the (constant) radical concentration k is the goal (rate constant) Too simple for chemists to screw up. Also, of limited interest. New Models Chemistry Old Models Single Monomer Polymerization With one type of polymer, the relevant DE is: dx dt = −k rx x is the monomer concentration r is the (constant) radical concentration k is the goal (rate constant) Too simple for chemists to screw up. Also, of limited interest. New Models Chemistry Old Models New Models Two-Monolymer Polymerization Terminal Model With two type of monomers, we divide radicals into rx , ry based on last monomer added. dx dt = −kxx rx x − kyx ry x dy dt = −kxy rx y − kyy ry y x, y are the monomer concentrations kxx , kyx , kxy , kyy are the goal (rate constants) rx + ry is the (constant) radical concentration Chemistry Old Models New Models Two-Monolymer Polymerization Terminal Model With two type of monomers, we divide radicals into rx , ry based on last monomer added. dx dt = −kxx rx x − kyx ry x dy dt = −kxy rx y − kyy ry y x, y are the monomer concentrations kxx , kyx , kxy , kyy are the goal (rate constants) rx + ry is the (constant) radical concentration Chemistry Old Models New Models The Value of Kinetics dx dt = −kxx rx x − kyx ry x dy dt = −kxy rx y − kyy ry y x, y are the monomer concentrations kxx , kyx , kxy , kyy are the goal (rate constants) rx + ry is the (constant) radical concentration kyx , kxy ∼ = 0 Block Copolymerization; homogeneous chains kxx , kyy ∼ = 0 Alternating Copolymerization kyx ∼ = kxy ∼ = kxx ∼ = kyy Random Copolymerization Chemistry Old Models New Models The Value of Kinetics dx dt = −kxx rx x − kyx ry x dy dt = −kxy rx y − kyy ry y x, y are the monomer concentrations kxx , kyx , kxy , kyy are the goal (rate constants) rx + ry is the (constant) radical concentration kyx , kxy ∼ = 0 Block Copolymerization; homogeneous chains kxx , kyy ∼ = 0 Alternating Copolymerization kyx ∼ = kxy ∼ = kxx ∼ = kyy Random Copolymerization Chemistry Old Models New Models The Value of Kinetics dx dt = −kxx rx x − kyx ry x dy dt = −kxy rx y − kyy ry y x, y are the monomer concentrations kxx , kyx , kxy , kyy are the goal (rate constants) rx + ry is the (constant) radical concentration kyx , kxy ∼ = 0 Block Copolymerization; homogeneous chains kxx , kyy ∼ = 0 Alternating Copolymerization kyx ∼ = kxy ∼ = kxx ∼ = kyy Random Copolymerization Chemistry Old Models New Models The Value of Kinetics dx dt = −kxx rx x − kyx ry x dy dt = −kxy rx y − kyy ry y x, y are the monomer concentrations kxx , kyx , kxy , kyy are the goal (rate constants) rx + ry is the (constant) radical concentration kyx , kxy ∼ = 0 Block Copolymerization; homogeneous chains kxx , kyy ∼ = 0 Alternating Copolymerization kyx ∼ = kxy ∼ = kxx ∼ = kyy Random Copolymerization Chemistry Old Models New Models Completing the Model dx dt = −kxx rx x − kyx ry x dy dt = −kxy rx y − kyy ry y x, y are the monomer concentrations kxx , kyx , kxy , kyy are the goal (rate constants) rx + ry is the (constant) radical concentration Additional DE: drx dt dr = − dty = kyx ry x − kxy rx y = 0 (Mayo, Lewis) BAD IDEA Chemistry Old Models New Models Completing the Model dx dt = −kxx rx x − kyx ry x dy dt = −kxy rx y − kyy ry y x, y are the monomer concentrations kxx , kyx , kxy , kyy are the goal (rate constants) rx + ry is the (constant) radical concentration Additional DE: drx dt dr = − dty = kyx ry x − kxy rx y = 0 (Mayo, Lewis) BAD IDEA Chemistry Old Models New Models Completing the Model dx dt = −kxx rx x − kyx ry x dy dt = −kxy rx y − kyy ry y x, y are the monomer concentrations kxx , kyx , kxy , kyy are the goal (rate constants) rx + ry is the (constant) radical concentration Additional DE: drx dt dr = − dty = kyx ry x − kxy rx y = 0 (Mayo, Lewis) BAD IDEA Chemistry Old Models New Models Completing the Model dx dt = −kxx rx x − kyx ry x dy dt = −kxy rx y − kyy ry y x, y are the monomer concentrations kxx , kyx , kxy , kyy are the goal (rate constants) rx + ry is the (constant) radical concentration Additional DE: drx dt dr = − dty = kyx ry x − kxy rx y = 0 (Mayo, Lewis) BAD IDEA Chemistry Old Models New Models Mayo Lewis Copolymerization Model Divide dx/dt by dy /dt, and use the assumption drx /dt = 0 dx dy kx = kxx kxy , ky = = x(kx x+y ) y (x+ky y ) kyy kyx , ‘copolymerization equation’ new rate constants kx measures the degree to which a radical ending in x preferentially bonds with x again. (still meaningful) Chemistry Old Models New Models Mayo Lewis Copolymerization Model Divide dx/dt by dy /dt, and use the assumption drx /dt = 0 dx dy kx = kxx kxy , ky = = x(kx x+y ) y (x+ky y ) kyy kyx , ‘copolymerization equation’ new rate constants kx measures the degree to which a radical ending in x preferentially bonds with x again. (still meaningful) Chemistry Old Models New Models Mayo Lewis Copolymerization Model Divide dx/dt by dy /dt, and use the assumption drx /dt = 0 dx dy kx = kxx kxy , ky = = x(kx x+y ) y (x+ky y ) kyy kyx , ‘copolymerization equation’ new rate constants kx measures the degree to which a radical ending in x preferentially bonds with x again. (still meaningful) Chemistry Old Models New Models Using The Copolymerization Equation dx dy = x(kx x+y ) y (x+ky y ) Basic use: Take multiple measurements of x, y throughout. dx at each paired measurement. With two such, Estimate dy can solve 2 × 2 linear system to find kx , ky . y x Advanced use: Change variables (e.g. to x+y , x+y ) and/or manipulate algebraically. Find kx , ky through regression. Many variations exist. Scat with racing stripes: Expand model to consider last two monomers added. Chemistry Old Models New Models Using The Copolymerization Equation dx dy = x(kx x+y ) y (x+ky y ) Basic use: Take multiple measurements of x, y throughout. dx at each paired measurement. With two such, Estimate dy can solve 2 × 2 linear system to find kx , ky . y x Advanced use: Change variables (e.g. to x+y , x+y ) and/or manipulate algebraically. Find kx , ky through regression. Many variations exist. Scat with racing stripes: Expand model to consider last two monomers added. Chemistry Old Models New Models Using The Copolymerization Equation dx dy = x(kx x+y ) y (x+ky y ) Basic use: Take multiple measurements of x, y throughout. dx at each paired measurement. With two such, Estimate dy can solve 2 × 2 linear system to find kx , ky . y x Advanced use: Change variables (e.g. to x+y , x+y ) and/or manipulate algebraically. Find kx , ky through regression. Many variations exist. Scat with racing stripes: Expand model to consider last two monomers added. Chemistry Old Models New Models Critiquing The Copolymerization Equation dx dy Critical Assumption: = drx dt x(kx x+y ) y (x+ky y ) = kyx ry x − kxy rx y = 0. Note that kyx , ry , kxy , rx are all constants. Hence some constant α independent of t. x y = α, for The model collapses; x and y must react exactly in their initial proportions. Hence all rate constants are equal (x, y indistinguishable) ‘random model’. Chemistry Old Models New Models Critiquing The Copolymerization Equation dx dy Critical Assumption: = drx dt x(kx x+y ) y (x+ky y ) = kyx ry x − kxy rx y = 0. Note that kyx , ry , kxy , rx are all constants. Hence some constant α independent of t. x y = α, for The model collapses; x and y must react exactly in their initial proportions. Hence all rate constants are equal (x, y indistinguishable) ‘random model’. Chemistry Old Models New Models Critiquing The Copolymerization Equation dx dy Critical Assumption: = drx dt x(kx x+y ) y (x+ky y ) = kyx ry x − kxy rx y = 0. Note that kyx , ry , kxy , rx are all constants. Hence some constant α independent of t. x y = α, for The model collapses; x and y must react exactly in their initial proportions. Hence all rate constants are equal (x, y indistinguishable) ‘random model’. Chemistry Old Models New Models Critiquing The Copolymerization Equation, II dx dy Critical Assumption: = drx dt x(kx x+y ) y (x+ky y ) = kyx ry x − kxy rx y = 0. Can we derive the equation from the starting DEs without the critical assumption? This has been done (e.g. probabilistic methods). It doesn’t help. The copolymerization equation is equivalent to the critical assumption. It cannot be saved. Chemistry Old Models New Models Critiquing The Copolymerization Equation, II dx dy Critical Assumption: = drx dt x(kx x+y ) y (x+ky y ) = kyx ry x − kxy rx y = 0. Can we derive the equation from the starting DEs without the critical assumption? This has been done (e.g. probabilistic methods). It doesn’t help. The copolymerization equation is equivalent to the critical assumption. It cannot be saved. Chemistry Old Models New Models Critiquing The Copolymerization Equation, II dx dy Critical Assumption: = drx dt x(kx x+y ) y (x+ky y ) = kyx ry x − kxy rx y = 0. Can we derive the equation from the starting DEs without the critical assumption? This has been done (e.g. probabilistic methods). It doesn’t help. The copolymerization equation is equivalent to the critical assumption. It cannot be saved. Chemistry Old Models New Models Critiquing The Copolymerization Equation, II dx dy Critical Assumption: = drx dt x(kx x+y ) y (x+ky y ) = kyx ry x − kxy rx y = 0. Can we derive the equation from the starting DEs without the critical assumption? This has been done (e.g. probabilistic methods). It doesn’t help. The copolymerization equation is equivalent to the critical assumption. It cannot be saved. Chemistry Old Models Outline Chemistry Old Models New Models New Models Chemistry Old Models New Models Decoupled Model Assume vastly more rx reactions. kxx rx x kyx ry x, kxy rx y kyy ry y dx dt ∼ = −kxx rx x −kxx rx x ≥ −kxy rx y ≥ 1 kx yx 1+ ≥ dx dy ∼ = kx yx dx dt dy dt dx dy dy dt ∼ = −kxy rx y ≥ −kxx rx x(1 + ) ≥ −kxy rx y (1 + ) ≥ kx yx (1 + ) Analytic solution: x(t) x(0) = y (t) y (0) kx Chemistry Old Models New Models Decoupled Model Assume vastly more rx reactions. kxx rx x kyx ry x, kxy rx y kyy ry y dx dt ∼ = −kxx rx x −kxx rx x ≥ −kxy rx y ≥ 1 kx yx 1+ ≥ dx dy ∼ = kx yx dx dt dy dt dx dy dy dt ∼ = −kxy rx y ≥ −kxx rx x(1 + ) ≥ −kxy rx y (1 + ) ≥ kx yx (1 + ) Analytic solution: x(t) x(0) = y (t) y (0) kx Chemistry Old Models New Models Decoupled Model Assume vastly more rx reactions. kxx rx x kyx ry x, kxy rx y kyy ry y dx dt ∼ = −kxx rx x −kxx rx x ≥ −kxy rx y ≥ 1 kx yx 1+ ≥ dx dy ∼ = kx yx dx dt dy dt dx dy dy dt ∼ = −kxy rx y ≥ −kxx rx x(1 + ) ≥ −kxy rx y (1 + ) ≥ kx yx (1 + ) Analytic solution: x(t) x(0) = y (t) y (0) kx Chemistry Old Models New Models Decoupled Model Assume vastly more rx reactions. kxx rx x kyx ry x, kxy rx y kyy ry y dx dt ∼ = −kxx rx x −kxx rx x ≥ −kxy rx y ≥ 1 kx yx 1+ ≥ dx dy ∼ = kx yx dx dt dy dt dx dy dy dt ∼ = −kxy rx y ≥ −kxx rx x(1 + ) ≥ −kxy rx y (1 + ) ≥ kx yx (1 + ) Analytic solution: x(t) x(0) = y (t) y (0) kx Chemistry Old Models New Models Decoupled Model Assume vastly more rx reactions. kxx rx x kyx ry x, kxy rx y kyy ry y dx dt ∼ = −kxx rx x −kxx rx x ≥ −kxy rx y ≥ 1 kx yx 1+ ≥ dx dy ∼ = kx yx dx dt dy dt dx dy dy dt ∼ = −kxy rx y ≥ −kxx rx x(1 + ) ≥ −kxy rx y (1 + ) ≥ kx yx (1 + ) Analytic solution: x(t) x(0) = y (t) y (0) kx Chemistry Old Models New Models Decoupled Model Assume vastly more rx reactions. kxx rx x kyx ry x, kxy rx y kyy ry y dx dt ∼ = −kxx rx x −kxx rx x ≥ −kxy rx y ≥ 1 kx yx 1+ ≥ dx dy ∼ = kx yx dx dt dy dt dx dy dy dt ∼ = −kxy rx y ≥ −kxx rx x(1 + ) ≥ −kxy rx y (1 + ) ≥ kx yx (1 + ) Analytic solution: x(t) x(0) = y (t) y (0) kx Chemistry Old Models New Models Weaknesses of Decoupled Model dx dy ∼ = kx yx We assumed kxx rx x kyx ry x, kxy rx y kyy ry y . We may force rx ry by x(0) y (0), hopefully. However, what if kxx kyx , or kxy kyy ? The error is difficult to determine, and yet has a large effect on the outcome interval. Need to have x(0) y (0). Chemistry Old Models New Models Weaknesses of Decoupled Model dx dy ∼ = kx yx We assumed kxx rx x kyx ry x, kxy rx y kyy ry y . We may force rx ry by x(0) y (0), hopefully. However, what if kxx kyx , or kxy kyy ? The error is difficult to determine, and yet has a large effect on the outcome interval. Need to have x(0) y (0). Chemistry Old Models New Models Weaknesses of Decoupled Model dx dy ∼ = kx yx We assumed kxx rx x kyx ry x, kxy rx y kyy ry y . We may force rx ry by x(0) y (0), hopefully. However, what if kxx kyx , or kxy kyy ? The error is difficult to determine, and yet has a large effect on the outcome interval. Need to have x(0) y (0). Chemistry Old Models New Models Weaknesses of Decoupled Model dx dy ∼ = kx yx We assumed kxx rx x kyx ry x, kxy rx y kyy ry y . We may force rx ry by x(0) y (0), hopefully. However, what if kxx kyx , or kxy kyy ? The error is difficult to determine, and yet has a large effect on the outcome interval. Need to have x(0) y (0). Chemistry Old Models New Models Partially Decoupled Model Assume extreme relative concentrations of x, y and rx , ry : r x y , rx ry . More precisely, yx , ryx ∈ [0, ]. dx dt dy dt drx dt r A∼ = −kxx r B∼ = −kxy C∼ =0 = rx x(−kxx − kyx ryx ) = Arx x = rx y (−kxy − kyy ryx ) = Brx y r = rx x(−kxy yx + kyx ryx ) = Crx x −kxx ≥ A ≥ (−kxx − kyx ) −kxy ≥ B ≥ (−kxy − kyy ) kyx ≥ C ≥ −kxy A/B ∼ = kx Chemistry Old Models New Models Partially Decoupled Model Assume extreme relative concentrations of x, y and rx , ry : r x y , rx ry . More precisely, yx , ryx ∈ [0, ]. dx dt dy dt drx dt r A∼ = −kxx r B∼ = −kxy C∼ =0 = rx x(−kxx − kyx ryx ) = Arx x = rx y (−kxy − kyy ryx ) = Brx y r = rx x(−kxy yx + kyx ryx ) = Crx x −kxx ≥ A ≥ (−kxx − kyx ) −kxy ≥ B ≥ (−kxy − kyy ) kyx ≥ C ≥ −kxy A/B ∼ = kx Chemistry Old Models New Models Partially Decoupled Model Assume extreme relative concentrations of x, y and rx , ry : r x y , rx ry . More precisely, yx , ryx ∈ [0, ]. dx dt dy dt drx dt r A∼ = −kxx r B∼ = −kxy C∼ =0 = rx x(−kxx − kyx ryx ) = Arx x = rx y (−kxy − kyy ryx ) = Brx y r = rx x(−kxy yx + kyx ryx ) = Crx x −kxx ≥ A ≥ (−kxx − kyx ) −kxy ≥ B ≥ (−kxy − kyy ) kyx ≥ C ≥ −kxy A/B ∼ = kx Chemistry Old Models New Models Partially Decoupled Model Assume extreme relative concentrations of x, y and rx , ry : r x y , rx ry . More precisely, yx , ryx ∈ [0, ]. dx dt dy dt drx dt r A∼ = −kxx r B∼ = −kxy C∼ =0 = rx x(−kxx − kyx ryx ) = Arx x = rx y (−kxy − kyy ryx ) = Brx y r = rx x(−kxy yx + kyx ryx ) = Crx x −kxx ≥ A ≥ (−kxx − kyx ) −kxy ≥ B ≥ (−kxy − kyy ) kyx ≥ C ≥ −kxy A/B ∼ = kx Chemistry Old Models New Models Partially Decoupled Model, II The system dx dt = Arx x, dy dt = Brx y , drx dt = Crx x, has an analytic solution. x(t) = x(0) 1−αAe1−αA x(t)(1−αA)Ct B/A y (t) = y (0) 1−αAe1−αA x(t)(1−αA)Ct rx (t) = αx(0)C −αA+e1−αA −x(t)(1−αA)Ct x(t) x(0) = y (t) y (0) A/B x(t) x(0) = y (t) y (0) kx Chemistry Old Models New Models Partially Decoupled Model, II The system dx dt = Arx x, dy dt = Brx y , drx dt = Crx x, has an analytic solution. x(t) = x(0) 1−αAe1−αA x(t)(1−αA)Ct B/A y (t) = y (0) 1−αAe1−αA x(t)(1−αA)Ct rx (t) = αx(0)C −αA+e1−αA −x(t)(1−αA)Ct x(t) x(0) = y (t) y (0) A/B x(t) x(0) = y (t) y (0) kx Chemistry Old Models New Models Partially Decoupled Model, II The system dx dt = Arx x, dy dt = Brx y , drx dt = Crx x, has an analytic solution. x(t) = x(0) 1−αAe1−αA x(t)(1−αA)Ct B/A y (t) = y (0) 1−αAe1−αA x(t)(1−αA)Ct rx (t) = αx(0)C −αA+e1−αA −x(t)(1−αA)Ct x(t) x(0) = y (t) y (0) A/B x(t) x(0) = y (t) y (0) kx Chemistry Old Models Partially Decoupled Model, III More precisely, x(t) x(0) = y (t) y (0) A/B −kxx ≥ A ≥ (−kxx − kyx ) −kxy ≥ B ≥ (−kxy − kyy ) Error Range: A B − k? ≤ kx ≤ kx = kxx kxy , ky = A B (1 + ky k? ) kyy kyx , k? = kyx kxy New Models Chemistry Old Models Partially Decoupled Model, III More precisely, x(t) x(0) = y (t) y (0) A/B −kxx ≥ A ≥ (−kxx − kyx ) −kxy ≥ B ≥ (−kxy − kyy ) Error Range: A B − k? ≤ kx ≤ kx = kxx kxy , ky = A B (1 + ky k? ) kyy kyx , k? = kyx kxy New Models Chemistry Old Models Weaknesses of Partially Decoupled Model x(t) x(0) A B − k? ≤ kx ≤ ∼ = A B (1 y (t) y (0) kx + ky k? ) Error range depends on ky , k? . Can estimate ky through dual experiment, but k? is a mystery. Sensitive to measurement error for x(0), y (0). Need to have x y , rx ry . New Models Chemistry Old Models Weaknesses of Partially Decoupled Model x(t) x(0) A B − k? ≤ kx ≤ ∼ = A B (1 y (t) y (0) kx + ky k? ) Error range depends on ky , k? . Can estimate ky through dual experiment, but k? is a mystery. Sensitive to measurement error for x(0), y (0). Need to have x y , rx ry . New Models Chemistry Old Models Weaknesses of Partially Decoupled Model x(t) x(0) A B − k? ≤ kx ≤ ∼ = A B (1 y (t) y (0) kx + ky k? ) Error range depends on ky , k? . Can estimate ky through dual experiment, but k? is a mystery. Sensitive to measurement error for x(0), y (0). Need to have x y , rx ry . New Models Chemistry Old Models Weaknesses of Partially Decoupled Model x(t) x(0) A B − k? ≤ kx ≤ ∼ = A B (1 y (t) y (0) kx + ky k? ) Error range depends on ky , k? . Can estimate ky through dual experiment, but k? is a mystery. Sensitive to measurement error for x(0), y (0). Need to have x y , rx ry . New Models Chemistry Old Models Future Work • Solutions without restricting relative concentrations. (analytic? approximate? numerical?) • Extend previous models to 3 types of monomers. • Detailed analysis of Mayo-Lewis model. (can we save the old data?) • Propagate mathematical knowledge through chemistry community. New Models Chemistry Old Models Future Work • Solutions without restricting relative concentrations. (analytic? approximate? numerical?) • Extend previous models to 3 types of monomers. • Detailed analysis of Mayo-Lewis model. (can we save the old data?) • Propagate mathematical knowledge through chemistry community. New Models Chemistry Old Models Future Work • Solutions without restricting relative concentrations. (analytic? approximate? numerical?) • Extend previous models to 3 types of monomers. • Detailed analysis of Mayo-Lewis model. (can we save the old data?) • Propagate mathematical knowledge through chemistry community. New Models Chemistry Old Models Future Work • Solutions without restricting relative concentrations. (analytic? approximate? numerical?) • Extend previous models to 3 types of monomers. • Detailed analysis of Mayo-Lewis model. (can we save the old data?) • Propagate mathematical knowledge through chemistry community. New Models