CHAPTER 6 - TRANSPORT AND KINETICS 

 
B:  RAPID EQUILIBRIUM AND STEADY STATE 
ENZYME KINETICS - DERIVATIONS

BIOCHEMISTRY - DR. JAKUBOWSKI

03/19/2009

Learning Goals/Objectives for Chapter 6B:  After class and this reading, students will be able to

  • write appropriate chemical and differential equations for the rate of disappearance of reactants or appearance of products for 1st order, pseudo first order, second order, reversible first order reactions
  • draw and interpret graphs for integrated rate equations (showing reactant or product concentrations as a function of time) and initial rate equations (showing the initial velocity vo as a function of reactant ;
  • derive kinetic rate constants from data and graphs of integrated rate and initial rate equations;
  • write appropriate chemical, differential equations, and initial rate equations for the rate of disappearance of reactants or appearance of products for simple enzyme catalyzed reaction;
  • differentiate between rapid and steady state assumptions;
  • simplify the initial rate equation containing rate constants for an enzyme catalyzed reactions to one replacing the rate constants with kcat and KM, and give operational and mathematical definitions of those constants;

We will first explore the kinetics of non-catalyzed reactions as with did with our study of passive and facilitated diffusion.  Before we do that, a brief review of the two major types of kinetic equations that you studied in general chemistry is in order.:

As seen below for a first order reaction of reactant A forming P with rate constant k1, we can write equations that gives v as function of A:   v = d[A]/dt = -k1[A] or  v = d[P]/dt = k1[A].  From these equations comes two different types equations:

REVIEW OF ELEMENTARY REACTION KINETICS

First Order Reaction:  

 

where k1 is the first order rate constant.  For these reactions, the velocity of the reaction, v, is directly proportional to [A], or 

1a.  v = -d[A]/dt = +d[P]/dT = k1[A]. 

The negative sign in -d[A]/dt indicates that the concentration of A decreases.  The equation could also be written as:

1b. v = d[A]/dt = - k1[A]. 
For the rest of the reactions shown in this section, I will follow the convention of writing all velocities expressed as d[x]/dt as positive numbers.  A negative sign for a term on the right hand side of the differential equation (as in 1b) will indicate that the concentration dependency of that term will lead to an decrease  in [x] with time.  Likewise a positive sign for the term on the right hand side of the equation will indicate that concentration dependency of that term will lead to an increase in [x] with time. 

Using this nomenclature, the following differential equation can be written and solved to find [A] as a function of t.

 dA/A = -k1dt

Equation 2 is an example of an integrated rate equation.  The following graphs show plots of A vs t and lnA vs t for data from a first order process.   Note that the derivative of the graph of A vs t (dA/dt) is the velocity of the reaction.  The graph of lnA vs t is linear with a slope of -k1.  Note that the velocity of the reaction (slope of the A vs t curve) decreases with decreasing A, which is consistent with equation 1.  

Figure:  First Order Reaction:  A --> P


Another way of analyzing the kinetics of a reaction, in addition to following the concentration of a reactant or product as a function of time and fitting the data to an integrated rate equation, is to plot the initial velocity, vo, of the reaction as a function of concentration of reactants.  The initial velocity is the initial slope of a graph of the concentration of reactants or products as a function of time, taken over a range of times such that only a small fraction of A has reacted, so [A] is approximately constant = Ao.  From the first order graph of A vs t above,  the slope approaches 0 with increasing time as [A] approaches 0, which clearly indicates that the reaction velocity depends on A.  For a first order process, two equivalent equations, 1a and 1b, can be written.   

Equation 1a above is written showing the disappearance of A as v = -d[A]/dt = k1[A], while

Equation 1b above is written showing the appearance of A as v = d[A]/dt = -k1[A],

Both equations shows that v is directly proportional to A.  As [A] is doubled, the initial velocity is doubled. 

Initial velocity graphs used by biochemists usually show the initial velocity of product formation (not reactant decrease) as a function of reactant concentration.  Hence, as the concentration of product is increasing, the slopes of initial velocity are positive.   A graph of vo (= dP/dt) vs [A] for a first order process would have a positive slope and be interpreted as showing that the rate of appearance of P depends linearly on [A].


Second Order/Pseudo First Order Reactions

 

where k2 is the second order rate constant.  For the first of these irreversible reactions, the velocity of the reaction, v, is directly proportional to [A] and [B], or 

3.  v = d[A]/dt = d[B]/dt =-2d[P]/dT = -k2[A][B].  

We will consider two special cases of this reaction type:

4.  v = -(k2[B]) [A] = -k1' [A] 

where k1' is the pseudo first order rate constant  (= k2[B] ) for the reaction.  The reaction appears to be first order, depending only on [A].

The following differential equation can be written and solved to find [A] as a function of t.

5.  v = d[A]/dt = +2d[P]/dT = -k2[A][A] = - k2[A]2 

6.  1/A = 1/Ao  +  k2t   

The following graphs show plots of A vs t and 1/A vs t for data from a second order process. 

Figure:  Second Order Reaction:  A + A --> P

Note that just from a plot of A vs t, it would be difficult to distinguish a first from second order reaction.  If the plots were superimposed, you would observe that at the same concentration of A (10 for example as in the linked plots), the vo of a first order reaction would be proportional to 10 but for a second order reaction to 102 or 100.  Therefore, the second order reaction is faster (assuming similarity in the relative magnitude of the rate constants) as indicated by the steeper negative slope of the curve.  However, at low A (0.1 example), the vo of a first order reaction would be proportional to 0.1 but for a second order reaction to 0.12 or 0.01.  Therefore, the second order reaction is slower. 


Reversible First Order Reactions

A differential equation can be written for this reaction:

7.   v = d[A]/dt = -k1[A] + k2[P]

This can be solved through integration to give the following equations:

Graphs of A and P vs t for this reaction at two different sets of values of k1 and k2 are shown below.

Figure:  Reversible First Order Reactions:  A <=> P

Xcel Spread Sheet:  Reversible First Order Reactions

Go to the following spread sheet and change the values of k1 and k2.  Note the changes in the graphs.  Remember that the dissociation constant, Kd, is related to the rate constants by the formula Kd = k2/k1.  Note that if the first order rate constants are equal , Kd = Keq =1 and the equilibrium concentrations of A and P are equal.


Consecutive First Order Reactions

For these reactions:

Graphs of A, B, and C vs t for these reaction at two different sets of values of k1 and k2 are shown below.

Figure:  Consecutive Irreversible First Order Reactions:  A --> B --> C

Xcel Spread Sheet:  Consecutive Reactions

Change the values of k1 and k2.  Note the changes in the graphs. 


  Reaction Appliets:

 


ENYZME-CATALYZED REACTION KINETICS

We have previously derived equations for the reversible binding of a ligand to a macromolecule. Next we derived equations for the receptor-mediated facilitated transport of a molecule through a semipermeable membrane. This latter case extended the former case by the addition of a physical transport step. Now, in what hopefully will seem like deja vu, we will derive almost identical equations for the chemical transformation of a ligand, commonly referred to as a substrate, by an enzyme. Two scenarios will be studied.

  1. Rapid Equilibrium Assumption - enzyme (macromolecule) and ligand (substrate) concentrations can be determined using the dissociation constant since E, S, and ES are in rapid equilibrium, as we previously used in our derivation of the equations for facilitated transport.
  2. Steady State Assumption (more general) -  enzyme and substrate concentrations are not those determined using the dissociation constant.

Enzyme kinetics experiments, as we will see in the next several Chapter, must be used to determine the detailed mechanism of the catalyzed reaction.  Using kinetics analyzes you can determine the order of binding/dissociation of substrates and products, the rate constants for individual steps, and clues as the to methods used by the enzyme in catalysis.

RAPID EQUILIBRIUM ASSUMPTION - HENRI-MICHAELIS-MENTEN EQUATION

Consider the following reaction mechanism for the enzyme-catalyzed conversion of substrate S into product P. (We will assume that the catalyzed rate is much greater than the noncatalyzed rate.)

 

As we did for the derivation of the equations for the facilitated transport reactions under rapid equilibrium conditions, this derivation is based on the assumption that the relative concentrations of S, E, and ES can be determined by the dissociation constant, Ks, for the interactions and the concentrations of each species during the early part of the reaction (i.e. under initial rate conditions). Assume also the S >> Eo.  Remember that under these conditions, S does not change much with time. Is this a valid assumption?  Examine the mechanism shown above.  S binds to E with a second order rate constant k1.  ES has two fates. It can dissociate with a first order rate constant k2 to S + E, or it can be converted to product with a first order rate constant of k3 to give P + E. If we assume that k2 >> k3 (i.e. that the complex falls apart much more quickly than S is converted to P), then the relative ratios of S, E, and ES can be described by Ks. Alternatively, you can think about it this way. If S binds to E, most of S will dissociate, and a small amount will be converted to P. If it does, then E is now free, and will quickly bind S and reequilibrate since the most likely fate of bound S is to dissociate, not be converted to P (since k3 << k2). This make sense also, if you consider that the physical step characterized by k2 is likely to be quicker than the chemical step, characterized by k3. Hence the following assumptions have been used:

Let's assume that for this system that the initial velocity will be measured. We would like to derive equations which show the initial velocity vo as a function of the initial substrate concentration, So , (assuming that P is negligible over the time course of measuring the initial velocity). Also assume that the v catalyzed >> vnoncatalyzed. In contrast to the first-order reaction of S to P in the absence of E, v is not proportional to So but rather to Sbound. as we described in class with facilitated diffusion (flux proportional to AR, not free A). Therefore,

vo a ES, or

Equation 1)   vo = v = const [ES] = k3 [ES]

where vo is the  initial velocity.   How can we calculate ES when we know S (which is equal to So) and Etot (which is Eo)? Let us assume that S is much greater than E, as is the likely biological case. We can calculate ES using the following equations and the same procedure we used for the derivation of the binding equation, which gives the equation below:

ES = (EoS)/(Ks + S)   (analogous to ML = (MoL)/(Kd + L) 

DERIVATION

Equation 5)    v = const [ES] = k3 [ES] = k3 EoS/(Ks + S) = VmS/(Ks + S).

This is the world famous Henri-Michaelis-Menten Equation

It should be clear to you from this equation that:

These are the same conditions we detailed for our understanding of the binding equation

ML = (MoL)/(Kd + L)


STEADY STATE ASSUMPTION

 

In this derivation, we will consider the following equations and all the rate constants, and will not arbitrarily assume that k2 >> k3. We  will still assume that S >> Eo and that Po = 0. An added assumption, however, is that dES/dt is approximately 0. Look at this assumption this way. When an excess of S is added to E, ES is formed. In the rapid equilibrium assumption, we assumed that it would fall back to E + S faster than it would go onto product. In this case, we will assume that it might go on to product either less or more quickly than it will fall back to E + S. In either case, a steady state concentration of ES arises within a few milliseconds, whose concentration does not change significantly during the initial part of the reaction under which the initial rates are measured. Therefore, dES/dt is about 0. In the rapid equilibrium derivation, we observed that v = k3ES.   We then solved for ES using Ks and mass balance of E. In the steady state assumption, the equation v = k3ES still holds, but know we will solve for ES using the steady state assumption that dES/dt =0.

Equation 1)    v = k3ES

Equation 6: (steady state) dES/dt = k1(E)(S) - k2(ES) -k3(ES) = 0

k1(E)(S) = (k2 + k3)(ES)

k1(Eo-ES)(S) = (k2 + k3)(ES)

k1(Eo)(S) - k1(ES)(S) = (k2 + k3)(ES)

k1(Eo)(S) = (k2 + k3)(ES) + k1(ES)(S)

  k1(Eo)(S) = ES (k2 + k3 + k1S)

Equation 9)   v = k3ES = [k3(Eo)(S)]/ [(k2 + k3)/k1 + S] = [k3(Eo)(S)]/(Km+ S)


ANALYSIS OF THE GENERAL MICHAELIS MENTEN EQUATION

This equation can be simplified and studied under different conditions. First notice that (k2 + k3)/k1 is a constant which is a function of relevant rate constants. This term is usually replaced by Km which is called the Michaelis constant. Likewise, when S approaches infinity (i.e. S >> Km, equation 5 becomes v = k3(Eo) which is also a constant, called Vm for maximal velocity. Substituting Vm and Km into equation 5 gives the simplified equation:

Equation 10)   v = Vm(S)/(Km+ S)

It is extremely important to note that Km in the general equation does not equal the Ks, the dissociation constant used in the rapid equilibrium assumption!    Km and Ks have the same units of molarity, however. A closer examination of Km shows that under the limiting case when k2 >> k3 (the rapid equilibrium assumption) then,

Equation 11)  Km = (k2 + k3)/k1 = k2/k1 = Kd = Ks.

If we examine Equations 9 and 10 under several different scenarios, we can better understand the equation and the kinetic parameters:

Notice that equations 9 and 10 are exactly analysis to the previous equations we derived:

Please notice that all these equations give hyperbolic dependencies of the y dependent variable (ML, Jo, and vo) on the ligand, solute, or substrate concentration, respectively.

Java Applet:  Michaelis-Menten Plots


EQUATION FOR MORE COMPLICATED REACTION

Not all reactions can be characterized so simply as a simple substrate interacting with an enzyme to form an ES complex, which then turns over to form product. Sometimes, intermediates form. For example, a substrate S might interact with E to form a complex, which then is cleaved to products P and Q. Q is released from the enzyme, but P might stay covalently attached. This happens often in the hydrolytic cleavage of a peptide bond by a protease, when an activated nucleophile like Ser reacts with the sessile peptide bond in a nucleophilic substitution reaction, releasing the amine end of the former peptide bond as the leaving group, while the carboxy end of the peptide bond remains bonded to the Ser as an Ser-acyl intermediate. Water then enters and cleaves the acyl intermediate, freeing the carboxyl end of the original peptide bond. This is shown in the written reaction below:

 

To simplify the derivation of the kinetic equation, let's assume that E, S, and ES are in rapid equilibrium defined by the dissociation constant, Ks. Assume Q has a visible absorbance, so it is easy to monitor.  Assume from the steady state assumption that:

d[E-P]/dt = k2[ES] - k3[E-P] = 0  (assuming k3 is a pseudo first order rate constant and [H2O] doesn't change.

The velocity depends on which step is rate limiting.  If k3<<k2, then the k3 step is rate-limiting.   Then

  v = k3[E-P]

 

  If k2<<k3, then the k2 step is rate-limiting.  Then

  v = k2[ES]

For a homework assignment, you derived the following kinetic equation for this reaction, assuming  v = k2[ES].

You can verify that you get the same equation if you assume that v = k3[E-P].  (Also, kcat will be defined below.)

This equation looks quite complicated, especially if you substitute for Ks, k-1/k1. All the kinetic constants can be expressed as functions of the individual rate constants. However this equation can be simplified by realizing the following:

Substituting these into equation 7 gives:

Equation 13)   v = Vm(S)/(Km+ S)

This again is the general form of the Michaelis-Menten equation

Note in the first bulleted item above that for this reaction, Vm = [(k2k3)/(k2 + k3)]Eo

This is more complicated than our earlier definition of Vm = k3Eo. They are similar in that the term Eo is multiplied by a constant which is itself a function of rate constant(s). The rate constants are generally lumped together into a generic constant called kcat. For the simple reaction kcat = k3 but for the more complicated reaction with a covalent intermdiate which we just deived, kcat = (k2k3)/(k2 + k3). For all reactions,

Equation 14)   Vm = kcatEo.


Figure:  Summary of vo vs S equations - Meanings of Km, kcat and Vm.

eXPERIMENTAL DETERMINATION OF Vm AND Km 

How can  Vm and  Km  be determined from experimental data? 

a.  From initial rate data:  The most common way is to determine initial rates, v0, from experimental values of P or S as a function of time.  Hyperbolic graphs of v0 vs [S] can be fit be fit or transformed as we explored with the different mathematical transformations of the hyperbolic binding equation to determine Kd.  These included:

The double-reciprocal plot is commonly used to analyze initial velocity vs substrate concentration data.  When used for such purposes, the graphs are referred to as Lineweaver-Burk plots, where plots of 1/v vs 1/S are straight lines with slope m = KM/Vmax, and y intercept b = 1/Vmax.  These plots can not be analyzed using linear regression, however, since that method assumes constant error in the y axis (in this case 1/v) data.  A weighted linear regression or even better, a nonlinear fit to a hyperbolic equation should be used.  The Mathcad template below shows such a nonlinear fit.  In the laboratory, we will use a series of programs developed by W. W. Cleland specifically designed to analyze initial rate data of enzyme catalyzed reactions.  A rearrangement of the corresponding Scatchard equations in the Eadie-Hofstee plot is also commonly used.

Mathcad 8 - Nonlinear Hyperbolic Fit.  Vm and Km.

Common Error in Biochemistry Textbooks:  The Shape of the Hyperbola

b.  From integrated rate equations:  KM and Vm can be extracted from progress curves of A or P as a function of t at one single A0 concentration by deriving an integrated rate equation for A or P as a function of t, as we did in equation 2 which shows the integrated rate equation for the conversion of A --> P in the absence of enzyme.  In that case, A=Aoe-k1t or P = A0(1-e-k1t).  The derivation of the relevant equations are shown below.

A graph of P/t vs [ln (1-P/A0)]/t  from equation 19 gives a straight line with a slope of Km and a y intercept of Vm.   A plot of  P vs t is shown below.   Note that the calculated values of Vm and Km are derived from only one substrate concentration, and the values may be affected by product inhibition

Compare this graph to that of P vs t for the non-enzyme catalyzed first order conversion of A -->  where A=A0e-k1t or P = A0(1-e-k1t)

Figure:  Enzyme Kinetics Progress Curve

TEnzyme Kinetics:  Interactive Java Applet - Change E, S, P, kcat, Km, Hill Coefficient

anicheck.gif (1995 bytes)Moodle Online Quiz (PASSWORD PROTECTED):   ENZYME KINETICS1

anicheck.gif (1995 bytes)Moodle Online Quiz (PASSWORD PROTECTED):   ENZYME KINETICS 2

 

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