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Consider the formation of double-stranded (DS) DNA from two complementary single strands (S and S') through the following mechanism involving an intermediate helix (IH): \\[ \begin{array}{l} \mathrm{S}+\mathrm{S}^{\prime} \frac{k_{1}}{\mathrm{k}_{-1}} \mathrm{IH} \\ \mathrm{IH} \stackrel{k_{2}}{\longrightarrow} \mathrm{DS} \end{array} \\] a. Derive the rate law expression for this reaction employing the preequilibrium approximation. b. What is the corresponding rate-law expression for the reaction employing the steady state approximation for the intermediate IH?

Short Answer

Expert verified
The rate law expressions for the given reaction after employing the preequilibrium approximation and the steady state approximation for the intermediate IH are as follows: a. Preequilibrium approximation: \[ \mathrm{rate}=k_{2}K[\mathrm{S}][\mathrm{S}^{\prime}] \] b. Steady state approximation: \[ \mathrm{rate}=k_{2}\left(\frac{k_{1}[\mathrm{S}][\mathrm{S}^{\prime}]}{k_{-1}+k_{2}}\right) \]

Step by step solution

01

Write the equilibrium expression

The reaction reaches a rapid equilibrium before the slow step, so we have: \[ \begin{array}{l} \mathrm{S}+\mathrm{S}^{\prime} \longleftrightarrow \mathrm{IH} \end{array} \] The reaction has an equilibrium constant K, which can be expressed as: \[ K=\frac{[\mathrm{IH}]}{[\mathrm{S}][\mathrm{S}^{\prime}]} \]
02

Write the rate law for the slow step

The slow step is the formation of DS from IH: \[ \mathrm{IH} \stackrel{k_{2}}{\longrightarrow} \mathrm{DS} \] The rate law for the slow step can be written as: \[ \mathrm{rate}=k_{2}[\mathrm{IH}] \]
03

Substitute the equilibrium expression into the rate law

To obtain the rate law in terms of the reactants' concentrations, substitute the equilibrium expression into the rate law: \[ \mathrm{rate}=k_{2}[\mathrm{IH}]=k_{2}K[\mathrm{S}][\mathrm{S}^{\prime}] \] This is the rate law expression for the reaction employing the preequilibrium approximation. #b. What is the corresponding rate-law expression for the reaction employing the steady state approximation for the intermediate IH?#
04

Write the rate of formation and consumption of IH

For the steady-state approximation, the rate of formation of IH is equal to its rate of consumption. The rate of formation of IH is given by: \[ \mathrm{Formation\:rate}=k_{1}[\mathrm{S}][\mathrm{S}^{\prime}] \] The rate of consumption of IH is given by: \[ \mathrm{Consumption\:rate}=k_{-1}[\mathrm{IH}]+k_{2}[\mathrm{IH}] \]
05

Use the steady state approximation

Set the formation rate equal to the consumption rate: \[ k_{1}[\mathrm{S}][\mathrm{S}^{\prime}]=k_{-1}[\mathrm{IH}]+k_{2}[\mathrm{IH}] \] Rearrange the equation to solve for [IH]: \[ [\mathrm{IH}]=\frac{k_{1}[\mathrm{S}][\mathrm{S}^{\prime}]}{k_{-1}+k_{2}} \]
06

Write the rate law for the steady-state case

The rate law for the steady-state case is the rate of formation of DS: \[ \mathrm{rate}=k_{2}[\mathrm{IH}] \] Substitute the expression for [IH] we obtained using the steady-state approximation: \[ \mathrm{rate}=k_{2}\left(\frac{k_{1}[\mathrm{S}][\mathrm{S}^{\prime}]}{k_{-1}+k_{2}}\right) \] This is the rate-law expression for the reaction employing the steady state approximation for the intermediate IH.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Preequilibrium Approximation
Understanding the preequilibrium approximation is vital when analyzing certain chemical reactions, including the formation of double-stranded DNA from single strands. The preequilibrium approximation assumes that the initial steps of a reaction reach an equilibrium much faster than the subsequent steps. This leads to a temporary steady state where the concentrations of the reactants and the intermediate product remain relatively constant.

In the context of DNA formation, when single strands S and S' combine, they form an intermediate helix (IH) rapidly and then, more slowly, transition into a double-stranded DNA (DS). Because the formation of IH is fast and reversible, it is assumed to be at equilibrium. By equating the forward and reverse reaction rates at this stage, we derive an equilibrium constant, K, which relates the concentration of the intermediate to the concentration of the initial strands, expressed as \[K = \frac{[\mathrm{IH}]}{[\mathrm{S}][\mathrm{S}']}\].

Applying preequilibrium to the rate law for the reaction's slower step, the formation of DS, allows us to express the rate in terms of reactants' concentrations, leading to a simplified rate law for the overall process. This approximation is invaluable for understanding reaction dynamics and calculating rate laws for complex mechanisms where intermediate species are involved.
Steady State Approximation
The steady state approximation is another insightful approach used in chemical kinetics, particularly for reactions involving unstable intermediates. This method assumes that after a short initial period, the rate of formation of an intermediate species equals its rate of consumption, resulting in a steady (unchanged) concentration of the intermediate over time.

In the case of double-stranded DNA formation, the intermediary is the IH. The rates of both its formation and consumption are considered. By setting these rates equal to each other, \[k_{1}[\mathrm{S}][\mathrm{S}'] = k_{-1}[\mathrm{IH}] + k_{2}[\mathrm{IH}]\], the concentration of IH can be deduced. This allows for the expression of the rate law in terms of only the observable species—S and S'.

The steady state approximation simplifies the mathematics of complex reaction mechanisms by eliminating the need to consider time-dependent changes in the intermediate. It's particularly useful when dealing with reactions where intermediate species are difficult to detect or measure directly.
Rate Law Expression
Understanding the rate law expression is crucial for predicting how fast a reaction will occur under various conditions. A rate law expresses the rate of a reaction in terms of the concentration of its reactants, often raised to some power which corresponds to their reaction order.

In the formation of double-stranded DNA, the rate law can be derived using either the preequilibrium or steady state approximation. The preequilibrium approximation gives us a rate law that reflects the initial, fast equilibrium, resulting in a rate proportional to the product of the concentrations of the single strands S and S'. On the other hand, the steady state approximation leads to a more nuanced rate law that accounts for the formation and consumption of the intermediate, resulting in the formula \[\mathrm{rate} = k_{2}\left(\frac{k_{1}[\mathrm{S}][\mathrm{S}']}{k_{-1}+k_{2}}\right)\].

By employing the correct approximation and deriving the rate law, chemists can make accurate predictions about reaction rates, which is essential for process control and optimization in industrial applications and laboratory experiments.
Double-Stranded DNA Formation
Double-stranded DNA formation is a fundamental biological process that lies at the heart of genetics and molecular biology. It involves the pairing of two complementary single DNA strands to form the familiar double helix structure. This pairing is mediated by hydrogen bonds between the complementary bases on each strand.

The reaction mechanism for double-stranded DNA formation can be described by the association of single strands (S and S') to form an intermediate helix (IH), which then converts into the double-stranded DNA (DS). The application of kinetic approximations like preequilibrium and steady state helps us understand and model this critical biophysical process, providing insight into the rate at which genetic information is stabilized into its double-helical form.

Grasping the process of double-stranded DNA formation is critical not only for academic purposes but also for practical applications, such as DNA replication, repair, and the biotechnological processes that underpin modern molecular biology and genetic engineering.

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Most popular questions from this chapter

The hydrogen-bromine reaction corresponds to the production of \(\operatorname{HBr}(g)\) from \(\mathrm{H}_{2}(g)\) and \(\mathrm{Br}_{2}(g)\) as follows: \(\mathrm{H}_{2}(g)+\operatorname{Br}_{2}(g) \rightleftharpoons 2 \mathrm{HBr}(g) .\) This reaction is famous for its complex rate law, determined by Bodenstein and Lind in 1906: \\[ \frac{d[\mathrm{HBr}]}{d t}=\frac{k\left[\mathrm{H}_{2}\right]\left[\mathrm{Br}_{2}\right]^{1 / 2}}{1+\frac{m[\mathrm{HBr}]}{\left[\mathrm{Br}_{2}\right]}} \\] where \(k\) and \(m\) are constants. It took 13 years for a likely mechanism of this reaction to be proposed, and this feat was accomplished simultaneously by Christiansen, Herzfeld, and Polyani. The mechanism is as follows: \\[ \begin{array}{l} \operatorname{Br}_{2}(g) \stackrel{k_{1}}{\sum_{k_{-1}}} 2 \operatorname{Br} \cdot(g) \\ \text { Br' }(g)+\mathrm{H}_{2}(g) \stackrel{k_{2}}{\longrightarrow} \operatorname{HBr}(g)+\mathrm{H} \cdot(g) \\ \text { H\cdot }(g)+\operatorname{Br}_{2}(g) \stackrel{k_{3}}{\longrightarrow} \operatorname{HBr}(g)+\operatorname{Br} \cdot(g) \\ \operatorname{HBr}(g)+\mathrm{H} \cdot(g) \stackrel{k_{4}}{\longrightarrow} \mathrm{H}_{2}(g)+\operatorname{Br} \cdot(g) \end{array} \\] Construct the rate law expression for the hydrogen-bromine reaction by performing the following steps: a. Write down the differential rate expression for \([\mathrm{HBr}]\) b. Write down the differential rate expressions for \([\mathrm{Br} \cdot]\) and [H']. c. Because \(\mathrm{Br} \cdot(g)\) and \(\mathrm{H} \cdot(g)\) are reaction intermediates, apply the steady-state approximation to the result of part (b). d. Add the two equations from part (c) to determine [Br'] in terms of \(\left[\mathrm{Br}_{2}\right]\) e. Substitute the expression for \([\mathrm{Br} \cdot]\) back into the equation for \([\mathrm{H} \cdot]\) derived in part \((\mathrm{c})\) and solve for \([\mathrm{H} \cdot]\) f. Substitute the expressions for \([\mathrm{Br} \cdot]\) and \([\mathrm{H} \cdot]\) determined in part (e) into the differential rate expression for \([\mathrm{HBr}]\) to derive the rate law expression for the reaction.

In the unimolecular isomerization of cyclobutane to butylene, the following values for \(k_{u n i}\) as a function of pressure were measured at \(350 \mathrm{K}\) \\[ \begin{array}{lcccc} \boldsymbol{P}_{\mathbf{0}}(\mathbf{T o r r}) & 110 & 210 & 390 & 760 \\ \boldsymbol{k}_{\boldsymbol{u n i}}\left(\mathbf{s}^{-1}\right) & 9.58 & 10.3 & 10.8 & 11.1 \end{array} \\] Assuming that the Lindemann mechanism accurately describes this reaction, determine \(k_{1}\) and the ratio \(k_{-1} / k_{2}\)

Protein tyrosine phosphatases (PTPases) are a general class of enzymes that are involved in a variety of disease processes including diabetes and obesity. In a study by Z.-Y. Zhang and coworkers [J. Medicinal Chemistry 43 \((2000): 146]\) computational techniques were used to identify potential competitive inhibitors of a specific PTPase known as PTP1B. The structure of one of the identified potential competitive inhibitors is shown here: The reaction rate was determined in the presence and absence of inhibitor \(I\) and revealed the following initial reaction rates as a function of substrate concentration: $$\begin{array}{ccc} & \mathbf{R}_{0}\left(\boldsymbol{\mu} \mathbf{M} \mathbf{~} \mathbf{s}^{-\mathbf{1}}\right) \\ {[\mathbf{S}](\boldsymbol{\mu} \mathbf{M})} & \mathbf{R}_{0}\left(\boldsymbol{\mu} \mathbf{M} \mathbf{~} \mathbf{s}^{-1}\right),[\boldsymbol{I}]=\mathbf{0} & {\left[\begin{array}{cc} \boldsymbol{I} & =\mathbf{2 0 0} \boldsymbol{\mu} \mathbf{M} \end{array}\right]} \\ \hline 0.299 & 0.071 & 0.018 \\ 0.500 & 0.100 & 0.030 \\ 0.820 & 0.143 & 0.042 \\ 1.22 & 0.250 & 0.070 \\ 1.75 & 0.286 & 0.105 \\ 2.85 & 0.333 & 0.159 \\ 5.00 & 0.400 & 0.200 \\ 5.88 & 0.500 & 0.250 \end{array}$$ a. Determine \(K_{m}\) and \(R_{\max }\) for PTP1B. b. Demonstrate that the inhibition is competitive, and determine \(K_{i}\)

The Kermack-McKendrick model was developed to explain the rapid rise and fall in the number of infected people during epidemics. This model involves the interaction of susceptible (S), infected (I), and recovered (R) people through the following mechanism: \\[ \begin{array}{l} \mathrm{S}+\mathrm{I} \stackrel{k_{1}}{\longrightarrow} \mathrm{I}+\mathrm{I} \\\ \mathrm{I} \stackrel{k_{2}}{\longrightarrow} \mathrm{R} \end{array} \\] a. Write down the differential rate expressions for \(S,\) I, and \(R\) b. The key quantity in this mechanism is called the epidemiological threshold defined as the ratio of \([\mathrm{S}] k_{1} / k_{2}\). When this ratio is greater than 1 the epidemic will spread; however, when the threshold is less than 1 the epidemic will die out. Based on the mechanism, explain why this behavior is observed.

A central issue in the design of aircraft is improving the lift of aircraft wings. To assist in the design of more efficient wings, wind-tunnel tests are performed in which the pressures at various parts of the wing are measured generally using only a few localized pressure sensors. Recently, pressure- sensitive paints have been developed to provide a more detailed view of wing pressure. In these paints, a luminescent molecule is dispersed into an oxygen- permeable paint and the aircraft wing is painted. The wing is placed into an airfoil, and luminescence from the paint is measured. The variation in \(\mathrm{O}_{2}\) pressure is measured by monitoring the luminescence intensity, with lower intensity demonstrating areas of higher \(\mathrm{O}_{2}\) pressure due to quenching. a. The use of platinum octaethylporphyrin (PtOEP) as an oxygen sensor in pressure-sensitive paints was described by Gouterman and coworkers [Review of Scientific Instruments \(61(1990): 3340] .\) In this work, the following relationship between luminescence intensity and pressure was derived: \(I_{0} / I=A+B\left(P / P_{0}\right),\) where \(I_{0}\) is the fluorescence intensity at ambient pressure \(P_{0},\) and \(I\) is the fluorescence intensity at an arbitrary pressure \(P .\) Determine coefficients \(A\) and \(B\) in the preceding expression using the Stern-Volmer equation: \(k_{\text {total}}=1 / \tau_{l}=k_{l}+k_{q}[Q] .\) In this equation \(\tau_{l}\) is the luminescence lifetime, \(k_{l}\) is the luminescent rate constant, and \(k_{q}\) is the quenching rate constant. In addition, the luminescent intensity ratio is equal to the ratio of luminescence quantum yields at ambient pressure \(\Phi_{0}\) and an arbitrary pressure \(\Phi:\) \\[ \Phi_{0} / \Phi=I_{0} / I \\] b. Using the following calibration data of the intensity ratio versus pressure observed for PtOEP, determine \(A\) and \(B\) : $$\begin{array}{cccc} I_{0} / I & P / P_{0} & I_{0} / I & P / P_{0} \\ \hline 1.0 & 1.0 & 0.65 & 0.46 \\ 0.9 & 0.86 & 0.61 & 0.40 \\ 0.87 & 0.80 & 0.55 & 0.34 \\ 0.83 & 0.75 & 0.50 & 0.28 \\ 0.77 & 0.65 & 0.46 & 0.20 \\ 0.70 & 0.53 & 0.35 & 0.10 \end{array}$$ c. \(A t\) an ambient pressure of 1 atm, \(I_{0}=50,000\) (arbitrary units \()\) and 40,000 at the front and back of the wing. The wind tunnel is turned on to a speed of Mach \(0.36,\) and the measured luminescence intensity is 65,000 and 45,000 at the respective locations. What is the pressure differential between the front and back of the wing?

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