Activation energy for a chemical reaction

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Discussion Overview

The discussion revolves around the activation energy for a chemical reaction, specifically how the rate of the forward reaction depends on temperature and concentration. Participants explore the application of the Boltzmann distribution in this context, addressing both theoretical and practical aspects of reaction kinetics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents a model for the rate of a unimolecular reaction, suggesting that the rate can be expressed as r_f = k[A] exp(E*/(nRT)), but questions the assumption that E = E*.
  • Another participant challenges the use of the 1/n factor in the exponential and asks for clarification on the dimensions of activation energy.
  • It is noted that typical activation energies for chemical reactions range from 10-100 kcal/mol, and the Arrhenius equation is introduced as a way to express the temperature dependence of the rate constant.
  • A participant discusses the preexponential factor and its dependence on reaction specifics, suggesting that it can be derived from collision theory or experimental data.
  • One participant expresses a desire for a simpler relationship between reaction rate, temperature, and concentration, indicating that the current explanations are overly complex.
  • Another participant introduces the Lindemann theory for unimolecular reactions and discusses the Maxwell-Boltzmann distribution in the context of molecular kinetics.
  • There is a mention of the relationship between the Boltzmann distribution and activation energy, with some participants questioning the connection and the nature of the potential being discussed.

Areas of Agreement / Disagreement

Participants express differing views on the assumptions made regarding activation energy and the complexity of the equations involved. There is no consensus on the best approach to relate the Boltzmann distribution to the reaction rate, and the discussion remains unresolved with multiple competing perspectives.

Contextual Notes

Some participants highlight the need for clarification on the dimensions of activation energy and the assumptions underlying the use of the Boltzmann distribution in this context. The discussion reflects a range of familiarity with the underlying concepts and mathematical formulations.

Who May Find This Useful

This discussion may be useful for individuals interested in chemical kinetics, the application of statistical mechanics to chemical reactions, and those seeking to understand the relationship between temperature, concentration, and reaction rates.

vladimir69
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hi,
could some one please verify what i have done here or tell me where i went wrong.

suppose the activation energy for a chemical reaction is E*, i have to work out how the rate of the forward reaction depends on temperature T and concentration. (note: i am given the Boltzmann distribution
c(E)=c_{0} \exp(\frac{E}{nRT}) )
n = number of moles
R = gas constant
E = gravitational potential energy
c_{0} = initial concentration
c = c(E) = concentration

i made the following assumptions in my calculations
- the reaction is a unimolecular decomposition reaction ( ie A -> B + C )
- the reaction is first order
- and by analogy E=E* (not so sure about this assumption)

let the rate of the forward reaction for the reaction A -> B + C be
r_{f}
so
r_{f} = -\frac{d[A]}{dt}
=k[A] where k is the rate constant

therefore
r_{f} = kc_{0}\exp(\frac{E*}{nRT})

i also need to put some plausible values for E* and comment on the quantitative results - i am not sure how to go about this and not sure what plausible values for E* are

thanks for your time
 
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vladimir69 said:
hi,
could some one please verify what i have done here or tell me where i went wrong.
.....
- and by analogy E=E* (not so sure about this assumption)

let the rate of the forward reaction for the reaction A -> B + C be
r_{f}
so
r_{f} = -\frac{d[A]}{dt}
=k[A] where k is the rate constant

therefore
r_{f} = kc_{0}\exp(\frac{E*}{nRT})


Why E=E*?. And why do you put a 1/n in the exponential factor?
Which are the dimensions of your activation energy needed?. And, is the same "k" in both last equations?.
 
Hi,

Most of the chemical reactions have activation energies around 10-100 kcal/mol.

If you´re assuming that that´s a first order reaction the concentration dependence is set to: v=k*[A]^1

The temperature dependence is given by the Arrhenius expression:
k=C*exp(\frac{-E*}{RT})
where C is the preexponential factor, that is different for each reaction.

The preexponential factor can be calculated theoretically aplying models such as collision theory or activated complex theory. You can take it from experimental data too.

So you can write the total expression for the rate of the reaction like this:
v=C*exp(\frac{-E*}{RT})*[A]

The Boltzmann expression is used in collison theory to obtain the distribution of energy of the sample. It gives you (for each value of energy) the amount of particles that have that energy. So introducing kinetic energy (not gravitational) you can get the amount of molecules that are able to collide with enough energy to react.

Sorry if i´m not helpful for you
 
hey thanks for the replies
for clausius2, the 1/n comes from the ideal gas equation PV=nRT
n = number of moles
as opposed to the ideal gas equation PV=NkT where N is the number of molecules

and yes k is the same for each expression that uses k
 
altered-gravity said:
Hi,


The temperature dependence is given by the Arrhenius expression:
k=C*exp(\frac{-E*}{RT})
where C is the preexponential factor, that is different for each reaction.


So you can write the total expression for the rate of the reaction like this:
v=C*exp(\frac{-E*}{RT})*[A]


This is the correct formulation. You have not cleared up enough E* dimensions. And note you have equalled r_f two times with different expresions for k. I absolutely agree with altered_gravity.

Que pasa, :biggrin: De donde eres?. Ya no me acuerdo de nada de esto de la energía de activación.
 
clausius2 - i did use 2 different expressions for rf but just so captain obvious didnt come to the rescue i didnt include them. i don't think the expression which altered-gravity kindly provided did what i wanted: which was to get a relationship between rate and temperature and concentration from the Boltzmann distribution. of course i could just pluck the formula from one of my chemistry past exam papers but i think the point of the question was to show how the Boltzmann distribution can be applied to a variety of different situations. hope this makes things clearer for you
 
I´m sorry, i´ve forgotten everything about this subject, perhaps i´m not able to help you. Anyway let´s try, let me see...

Maxwell_Boltzmann distributions of energy (or velocity) are used in molecular kietics models as they give you info about molecular average energy. Let´s try with collision model, it´s the simplest (but not good)

You proposed an unimolecular reaction A->B+C. Lindemann theory proposes this mechanism for unimolecular reactions:

A+M \rightleftharpoons A* + M
A* \rightarrow B+C

Theese are two reaction steps with three different reaction rates. Let´s propose a bimolecular reaction:

A+A->B

Here is the Maxwell-Boltzmann velocity distribution:
f(v)=4\pi(\frac{m}{2 \pi k T})^\frac{3}{2} v^2 exp(\frac{-m v^2}{2kT})

where m is the mass of the molecule
v is the velocity

So the average velocity is:
\sqrt{\frac{8kT}{\pi m_A}}

From this expression you can deduce the rate of collisions between two systems (A and A in this case). If you want to know how to deduce it, post it. This is the rate:

Z=\sqrt{2} \pi (d_A)^2 (\frac{8 k T}{\pi \mu_A})^\frac{1}{2}*[A]^2

d_A is the effective collisional diameter of the molecule
[A] is the concentration
\mu_A is the reduced mass of the system A - A

This is not the rate of reaction still, only collisions upon an energy E* make reaction. So you use the Maxwell-Boltzmann energy distribution (supposed that all the energy is kinetic):

\frac{n(E>E*)}{n_0}=exp(\frac{-E*}{RT})

n(E>E*) is the number of molecules with equal or more kinetic energy than E*

You multiply by this exponential factor and you get the rate of the reaction:

v=\sqrt{2} \pi (d_A)^2 (\frac{8 k T}{\pi \mu_A})^\frac{1}{2}*[A]^2*exp(\frac{-E*}{RT})

So the preexponential factor of the Arrhenius expression is:
C=\sqrt{2} \pi (d_A)^2 (\frac{8 k T}{\pi \mu_A})^\frac{1}{2}*exp(\frac{-E*}{RT})

You´d say: ¿why does preexponential factor depend on temperature? That dependence is very little as it is divided by the reduced mass and multiplied by Boltzmann constant.

Sorry if there are mistakes in expression (I´m new using laTex)
 
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Clausius2 said:
Que pasa, :biggrin: De donde eres?. Ya no me acuerdo de nada de esto de la energía de activación.

De Vitoria
Un saludo!
 
holy moley
that was a mouth full, let me say though i do appreciate your efforts.
i don't think the answer needs to be that complicated, i just need something similar to my first post - not a heap of equations i have never seen before and will probably never see again (hopefully)
so if it all possible
-few simplifiying assumptions
-from Boltzmann equation and *simple* relationships like rf=-d[A]/dt and rf=k[A] say
-out pops our relationship between reaction rate, temperature and concentration
hopefully you can see what i am trying to get at

thanks again for your time,
vladimir
 
  • #10
oopss! :blushing:
Sure you´re right. Forget it, today is not my day!

Well, at least I reviewed my old notes (very old!) Je Je! :biggrin:
 
  • #11
Hi Vladimir. Sorry for not being you very helpful. Anyway, why do you think it will exist a relation between the potential E coming from Boltzmann dist. and Activation Energy?. If I've not read wrong your last post, E is something like an electric potential, isn't it?.
 
  • #12
Clausius2 said:
Hi Vladimir. Sorry for not being you very helpful. Anyway, why do you think it will exist a relation between the potential E coming from Boltzmann dist. and Activation Energy?. If I've not read wrong your last post, E is something like an electric potential, isn't it?.

i am currently working on "similarities" in physics, in particular, applications of the Boltzmann distribution to a variety of situations, one of which being the rate of a chemistry reaction. my understanding has it that the Boltzmann distribution can be applied to very many systems in equilibria of different kinds
 
  • #13
problem

@altered-gravity

if one computes the integral from E to infinity using the Boltzmann equation on gets what you wrote:

\frac{n(E>E*)}{n_0}=exp(\frac{-E*}{RT})

however, if one takes (which i think in this case one has to) the maxwell-boltzmann distribution given by:

C * sqrt(E) * exp(-E/kt)

the integral from E to infinity is much more messy.

any thoughts on how one still gets exp(-E/kt) as the fraction of molecules having enough energy to react?
 
  • #14
(I don't think altered gravity is likely to respond)

Doing, the integral, I'm able to recover the correct exponential form under suitable conditions, but I have a troublesome prefactor:

f(E>E_a)=\frac{\int _{E_a}^{\infty} \sqrt{E}exp(-E_a/kT)dE}{\int _0^{\infty} \sqrt{E}exp(-E_a/kT)dE} = 2\sqrt{\frac{E_a}{\pi kT}}e^{-E_a/kT} + 1 - erf \left( \sqrt {\frac{E_a}{kT}} \right)

For Ea > 2kT, 1 - erf \left( \sqrt {(E_a/kT)} \right) < 0.05.

So if kT is not big enough to be comparable to Ea, these extra terms can be thrown away, leaving

f \approx 2\sqrt{(E_a/\pi kT)}exp(-E_a/kT).
 
Last edited:

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