Question:

The plot of log π‘˜π‘“ versus \(\frac{1}{T}\) for a reversible reaction, A (g) β‡Œ P (g) is shown. 
plot of log π‘˜π‘“ versus 1/T for a reversible reaction
Pre-exponential factors for the forward and backward reactions are 1015s-1 and 1011s-1 respectively. If the value of log K for the reaction at 500 K is 6, the value of |log kb| at 250K is_________
[K = equilibrium constant of the reaction,
π‘˜π‘“ = rate constant of forward reaction,
π‘˜π‘ = rate constant of backward reaction]

Updated On: May 24, 2024
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Correct Answer: 5

Approach Solution - 1

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.
 

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Approach Solution -2

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:
\[\boxed{5}\]

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Thermodynamics in physics is a branch that deals with heat, work and temperature, and their relation to energy, radiation and physical properties of matter.

Important Terms

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  • Isolated System – An isolated system cannot exchange both energy and mass with its surroundings. The universe is considered an isolated system.
  • Closed System – Across the boundary of the closed system, the transfer of energy takes place but the transfer of mass doesn’t take place. Refrigerators and compression of gas in the piston-cylinder assembly are examples of closed systems.
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Thermodynamic Process

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:

  • Adiabatic Process – A process in which no heat transfer takes place.
  • Isochoric Process – A thermodynamic process taking place at constant volume is known as the isochoric process.
  • Isobaric Process – A process in which no change in pressure occurs.
  • Isothermal Process – A process in which no change in temperature occurs.

Laws of Thermodynamics

Zeroth Law of Thermodynamics

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.

First Law of Thermodynamics 

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Second Law of Thermodynamics 

The Second law of thermodynamics is a physical law of thermodynamics about heat and loss in its conversion.

Third Law of Thermodynamics

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.