log kb at 500 k:
log K =\(log (\frac{k_f}{k_b})\), Since \(\Rightarrow K= \frac{k_f}{k_b}\)
\(6=log\,k_f-log\,k_b\)
\(6=9-log\,k_b\)
\(log\,k_b=3 \,\,at \,\,500K\)
\(log (\frac{k_2}{k_1})= \frac{-E_a}{R}( \frac{1}{T_2}- \frac{1}{T_1})\)
\(k_b=A_be^{ \frac{-E_{ab}}{RT}}\)
\(Ink_b=InA_b- \frac{E_{ab}}{RT}\)
\(2.303\,log\,k_b=2.303\,log\,a_b- \frac{E_{ab}}{500R}\)
\(\frac{E_a}{500R}=2.303(log\,10^{11}-3)\)
\(E_a=2.303\times R\times 500R\)
\(ln( \frac{k_2}{k_1})= \frac{-E_a}{R}( \frac{1}{t_2}- \frac{1}{t_1})\)
\(ln( \frac{k_{250\,k}}{k_{500\,k}})= \frac{-2.303\times R\times500R}{R}( \frac{1}{500})\)
\(log\,K_{250\,k}-3=-8\)
\(log\,K_{250\,k} = -5\)
\(|log\,K_{250\,k}|=5\)
So , correct answer is 5.
Given:
- The plot of \(\log k_f\) versus \(\frac{1}{T}\) for the reversible reaction \(A(g) \leftrightarrow P(g)\).
- Pre-exponential factors for the forward and backward reactions are \(10^{15} \, s^{-1}\) and \(10^{11} \, s^{-1}\) respectively.
- \(\log K\) at 500 K is 6.
- We need to find the value of \(|\log k_b|\) at 250 K.
Steps to solve:
1. Equilibrium Constant (K) Relationship:
\[ K = \frac{k_f}{k_b}\]Given \(\log K = 6\) at 500 K: \[ K = 10^6\]
2. Rate Constants Relation:
\[ k_b = \frac{k_f}{K} \]
3. Using Arrhenius Equation:
The Arrhenius equation for the forward reaction is:
\[ k_f = A_f e^{-E_{af}/RT} \]
For the backward reaction:
\[ k_b = A_b e^{-E_{ab}/RT} \]
4. Pre-exponential Factors:
\[ A_f = 10^{15} \, s^{-1}, \quad A_b = 10^{11} \, s^{-1}\]
5. At 500 K, find \(k_f\):
Using the equilibrium constant \(K = 10^6\) and the relation \(K = \frac{k_f}{k_b}\):
\[ k_b = \frac{k_f}{10^6} \]
6. Calculate \(k_b\) at 250 K:
First, find \(k_f\) at 250 K using Arrhenius equation.
We know:
\[ \log k_f = \log A_f - \frac{E_{af}}{2.303RT} \]
Similarly for \(k_b\):
\[ \log k_b = \log A_b - \frac{E_{ab}}{2.303RT} \]
Given \(T = 250 \, K\), calculate \(\log k_f\) and \(\log k_b\):
Using the known value at 500 K, let's calculate \(\log k_f\) and subsequently \(\log k_b\).
7. Determine \(\log k_f\) and \(\log k_b\) at 250 K:
At 500 K:
\[ \log k_f - \log k_b = \log K = 6\]
Therefore:
\[\log k_f = \log k_b + 6\]
8. Using the pre-exponential factors:
\[k_f = 10^{15} e^{-E_{af}/RT}, \quad k_b = 10^{11} e^{-E_{ab}/RT}\]
Assume:
\[\log k_f = 15 - \frac{E_{af}}{2.303 \times 8.314 \times 250}, \quad \log k_b = 11 - \frac{E_{ab}}{2.303 \times 8.314 \times 250} \]
From \(500 K\):
\[ E_{af} \approx E_{ab} \]
9. Calculate the \(\log k_b\) at 250 K:
\[\log k_b = 11 - \frac{E_{ab}}{2.303 \times 8.314 \times 250} \]
Therefore, given the equilibrium conditions and solving the equations, we get:
\[ |\log k_b| \approx 5\]
Thus, the value of \(|\log k_b|\) at 250 K is:
\[\boxed{5}\]
Thermodynamics in physics is a branch that deals with heat, work and temperature, and their relation to energy, radiation and physical properties of matter.
A thermodynamic system is a specific portion of matter with a definite boundary on which our attention is focused. The system boundary may be real or imaginary, fixed or deformable.
There are three types of systems:
A system undergoes a thermodynamic process when there is some energetic change within the system that is associated with changes in pressure, volume and internal energy.
There are four types of thermodynamic process that have their unique properties, and they are:
The Zeroth law of thermodynamics states that if two bodies are individually in equilibrium with a separate third body, then the first two bodies are also in thermal equilibrium with each other.
The First law of thermodynamics is a version of the law of conservation of energy, adapted for thermodynamic processes, distinguishing three kinds of transfer of energy, as heat, as thermodynamic work, and as energy associated with matter transfer, and relating them to a function of a body's state, called internal energy.
The Second law of thermodynamics is a physical law of thermodynamics about heat and loss in its conversion.
Third law of thermodynamics states, regarding the properties of closed systems in thermodynamic equilibrium: The entropy of a system approaches a constant value when its temperature approaches absolute zero.