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The rate of a particular chemical reaction \(A+B \rightarrow C\) is proportional to the concentrations of the reactants \(A\) and \(B\) : $$ \frac{d C(t)}{d t}=\alpha[A(0)-C(t)][B(0)-C(t)] $$ (a) Find \(C(t)\) for \(A(0) \neq B(0)\). (b) Find \(C(t)\) for \(A(0)=B(0)\). The initial condition is that \(C(0)=0\).

Short Answer

Expert verified
For \(A(0) \neq B(0)\), \( C(t)=\frac{A(0)B(0)}{(B(0)-A(0))e^{-\alpha (B(0)-A(0))t} + A(0)} \).\nFor \(A(0)=B(0)\), \(C(t) = \frac{A(0)^2\alpha t}{1+A(0)\alpha t}\).

Step by step solution

01

Express the Rate in Terms of Concentrations

The rate of the reaction is expressed as \( \frac{dC(t)}{dt} = \alpha [A(0) - C(t)][B(0) - C(t)] \), where \(C(t)\) is the concentration of product \(C\) at time \(t\), and \(A(0)\) and \(B(0)\) are the initial concentrations of reactants \(A\) and \(B\), respectively.
02

Separate the Variables

Rearrange the differential equation to separate variables: \[ \frac{dC}{[A(0) - C][B(0) - C]} = \alpha dt \]. Here, we need to integrate both sides with respect to their variables.
03

Integrate Both Sides

Integrate the left side with respect to \(C\) and the right side with respect to \(t\): \[ \int \frac{dC}{[A(0) - C][B(0) - C]} = \int \alpha \, dt \]. Use partial fraction decomposition for the left side to simplify the integral.
04

Solve the Integral for A(0) ≠ B(0)

Using partial fraction decomposition, the left side becomes: \[ \frac{1}{B(0) - A(0)} \left( \int \frac{1}{A(0) - C} \, dC - \int \frac{1}{B(0) - C} \, dC \right) = \alpha t + K \]. Solve these integrals to find \(C(t)\).
05

Apply Initial Condition for A(0) ≠ B(0)

Apply the initial condition \( C(0) = 0 \): Substitute \(t = 0\) and \(C = 0\) into the integrated equation to find the constant \(K\). Substitute back to find \(C(t)\).
06

Derive a Specific Solution for A(0) = B(0)

In the case of \(A(0) = B(0) = C_0\), the equation \( \frac{dC}{dt} = \alpha [C_0 - C]^2 \) simplifies the integration. Integrate as \( \int \frac{dC}{(C_0 - C)^2} = \int \alpha \, dt \) to find \(C(t)\).
07

Apply Initial Condition for A(0) = B(0)

Again, using \(C(0) = 0\), find the constant from the equation \( \int \frac{dC}{(C_0 - C)^2} = \alpha t + K \). Determine \(K\) and substitute back to obtain \(C(t)\).

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Key Concepts

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

Chemical Reaction Kinetics
Chemical reaction kinetics is the study of rates at which chemical processes occur. For a reaction like \(A + B \rightarrow C\), the rate often depends on the concentrations of the reactants. Here, the rate equation is given by \(\frac{dC(t)}{dt} = \alpha [A(0)-C(t)][B(0)-C(t)]\). This equation signifies that the speed of the product formation \( C(t) \) is proportional to the product of the concentrations of \(A\) and \(B\). Initially, both \(A\) and \(B\) are at their starting concentrations, \(A(0)\) and \(B(0)\), and as \(C\) is formed, these concentrations decrease.

To solve for \(C(t)\), we need to express the changing concentration in terms of time and initial conditions. Bio-chemists often study these equations to understand how quickly a reaction can reach completion, which is crucial in processes like drug production and metabolism control.

Learning chemical kinetics helps industrial chemists develop better catalysts, optimize temperature and pressure conditions, and improve yields in reactions.
Separation of Variables
Separation of variables is a mathematical technique used to solve differential equations. It is helpful when you can rearrange the equation to separate parts in terms of different variables. This is what was done with \(\frac{dC(t)}{dt} = \alpha [A(0)-C(t)][B(0)-C(t)]\), which was rearranged to \[\frac{dC}{[A(0) - C][B(0) - C]} = \alpha dt\].

Essentially, the goal is to isolate \(C\) on one side of the equation and \(t\) on the other, preparing both for integration. This helps find a functional relationship between \(C\) and \(t\) since it allows us to individually integrate each side to solve for \(C(t)\).
  • Isolate variables on each side of the equation.
  • Perform integration on both sides independently.
  • Apply initial or boundary conditions to solve for constants.
By practicing with exercises like these, students gain powerful tools to tackle various complex differential equations within science and engineering.
Partial Fraction Decomposition
Partial fraction decomposition is an algebraic technique used to simplify the integration of rational functions. When dealing with \(\int \frac{dC}{[A(0) - C][B(0) - C]}\), it helps express the integrand as a sum of simpler fractions. These can be integrated individually.

The decomposition involves expressing the original fraction as a sum of terms like \(\frac{1}{[A(0) - C]} - \frac{1}{[B(0) - C]}\). Mathematically this can be written as:
\[\frac{1}{(B(0) - A(0))} \left(\int \frac{1}{A(0) - C} dC - \int \frac{1}{B(0) - C} dC \right)\]

Each of these simpler terms is much easier to integrate. After partial fraction decomposition, you solve by integrating each part separately. It's especially useful when \(A(0) eq B(0)\), since direct integration without decomposition would be too cumbersome.
  • Break complex fractions into simpler terms.
  • Make integration more manageable.
  • Useful in solving many engineering problems.
With partial fraction decomposition, students learn how to handle seemingly daunting integrals efficiently, which is crucial for advanced calculus applications.

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Most popular questions from this chapter

Given that one solution of $$ R^{\prime \prime}+\frac{1}{r} R^{\prime}-\frac{m^{2}}{r^{2}} R=0 $$ is \(R=r^{m}\), show that Eq. (8.127) predicts a second solution \(R=r^{-m}\).

Develop a series solution selecting the parameter \(n\) to make your series a polynomial. Solve the Chebyshev equation $$ \left(1-x^{2}\right) T_{n}^{\prime \prime}-x T_{n}^{\prime}+n^{2} T_{n}=0 $$ by series substitution. What restrictions are imposed on \(n\) if you demand that the series solution converge for \(x=\pm 1 ?\)

Show that Legendre's equation has regular singularities at \(x=-1,1\), and \(\infty\).

Uniqueness theorem. The function \(y(x)\) satisfies a second-order, linear, homogeneous differential equation. At \(x=x_{0}, y(x)=y_{0}\), and \(d y / d x=y_{0}^{\prime} .\) Show that \(y(x)\) is unique in that no other solution of this differential equation passes through the points \(\left(x_{0}, y_{0}\right)\) with a slope of \(y_{0}^{\prime}\). Hint. Assume a second solution satisfying these conditions and compare the Taylor series expansions.

The differential equation for the population of a radioactive daughter element is $$ \frac{d N_{2}(t)}{d t}=\lambda_{1} \exp \left(-\lambda_{1} t\right)-\lambda_{2} N_{2}, $$ \(\lambda_{1} \exp \left(-\lambda_{1} t\right)\) being the rate of production resulting from the decay of the parent element, \(\lambda_{1}=0.10 \mathrm{~s}^{-1}, \lambda_{2}=0.08 \mathrm{~s}^{-1}\). Integrate this \(\mathrm{ODE}\) from \(t=0\) out to \(t=40 \mathrm{~s}\) for the initial condition \(N_{2}(0)=0\). Tabulate and plot \(N_{2}(t)\) vs \(t\).

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