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Question: Solve Arrhenius equation and find expression for \({T_2}\) ....

Solve Arrhenius equation and find expression for T2{T_2} .

Explanation

Solution

Temperature and rate constant relation having pre-exponential factor. Use Arrhenius equation step by step by taking initial conditions of a reaction a s temperature T1{T_1} and it’s rate constant k1{k_1} and for final condition temperature T2{T_2} take rate constant k2{k_2} . Solve step by step and find the value of T2{T_2} in terms of other quantities.

Complete step by step answer:
We know that Arrhenius equation is k=Aexp(EaRT)k = A\,\exp (\dfrac{{ - {E_a}}}{{RT}})
Where, kk is the rate constant for given reaction
AA is the pre-exponential factor
Ea{E_a} is the activation energy
RR is the universal gas constant
TT is absolute temperature
We know that as given by the collision theory, that when reactant molecules collide having a certain amount of energy they will convert into a product. That specific amount of energy is termed as threshold energy. Some molecules if we take an example of reaction A+BCA + \,B \to \,C where the two reactants must collide to form a product. They must contain threshold energy, it means they should have a minimum amount of energy for converting into product. If reactant molecules don't have that minimum energy they are supplied extra energy from outside in terms of heat. This extra energy supplied to reactant molecules is called activation energy.
It was seen that on increasing the temperature, rate constant gets doubled it means double the number of reactants collide and changes into product. There is a Maxwell distribution curve which graphically explains the doubled area of a fraction of molecules.
Arrhenius gave an equation after his name called Arrhenius equation which symbolises the relation between temperature and rate constant. In the equation as we see above, the factor EaRT\dfrac{{ - {E_a}}}{{RT}} , this factor represents the fraction of molecules.
Now let’s start solving equation for T2{T_2}
We have Arrhenius equation as-k=Aexp(EaRT)k = A\,\exp (\dfrac{{ - {E_a}}}{{RT}})
If we take logarithm on both side, we get this equation, lnk=lnAEaRT\ln \,k = \,\ln A - \,\dfrac{{{E_a}}}{{RT}}
Now as we have to find value for T2{T_2} it means there must be T1{T_1} also,
Let’s take rate constants be k1{k_1}\, and k2{k_2}\, for temperature T1{T_1} and T2{T_2} , then the above equations for two rate constants become as lnk1=lnAEaRT1\ln \,{k_1} = \,\ln A - \,\dfrac{{{E_a}}}{{R{T_1}}} and lnk2=lnAEaRT2\ln \,{k_2} = \,\ln A - \,\dfrac{{{E_a}}}{{R{T_2}}}
Subtracting these equations we get, lnk2lnk1=EaRT1EaRT2\ln \,{k_2} - \ln {k_1} = \,\,\dfrac{{{E_a}}}{{R{T_1}}} - \dfrac{{{E_a}}}{{R{T_2}}}
In the next step if we take EaR\dfrac{{{E_a}}}{R} common it will changes like this,
lnk2lnk1=EaR(1T11T2)\ln \,{k_2} - \ln {k_1} = \,\,\dfrac{{{E_a}}}{R}(\dfrac{1}{{{T_1}}} - \dfrac{1}{{{T_2}}})
ln(k2k1)=EaR[1T11T2]\ln \,\left( {\dfrac{{{k_2}}}{{{k_1}}}} \right) = \,\,\dfrac{{{E_a}}}{R}\left[ {\dfrac{1}{{{T_1}}} - \dfrac{1}{{{T_2}}}} \right]
On multiplying in the brackets we get, ln(k2k1)=EaR×1T1EaR×1T2\ln \,\left( {\dfrac{{{k_2}}}{{{k_1}}}} \right) = \,\,\dfrac{{{E_a}}}{R} \times \dfrac{1}{{{T_1}}} - \dfrac{{{E_a}}}{R} \times \dfrac{1}{{{T_2}}}

This is the value of T2{T_2} . If we put the value of all terms in the right hand side, we can easily calculate the value of T2{T_2} .

Note: Arrhenius equation gives relation between temperature of a reaction and rate constant, so take temperature and rate constant for initial and final stages of a reaction, final stage may be any temperature you want. While solving the equation for two conditions, the open bracket wisely multiplies the coefficient with inner terms. In most cases mistakes happen in the calculation part.