Question:

The plot of log π‘˜π‘“ versus 1T\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(kfkb)log (\frac{k_f}{k_b}), Since β‡’K=kfkb\Rightarrow K= \frac{k_f}{k_b}
6=log kfβˆ’log kb6=log\,k_f-log\,k_b
6=9βˆ’log kb6=9-log\,k_b
log kb=3  at  500Klog\,k_b=3 \,\,at \,\,500K
log(k2k1)=βˆ’EaR(1T2βˆ’1T1)log (\frac{k_2}{k_1})= \frac{-E_a}{R}( \frac{1}{T_2}- \frac{1}{T_1})
kb=Abeβˆ’EabRTk_b=A_be^{ \frac{-E_{ab}}{RT}}
Inkb=InAbβˆ’EabRTInk_b=InA_b- \frac{E_{ab}}{RT}
2.303 log kb=2.303 log abβˆ’Eab500R2.303\,log\,k_b=2.303\,log\,a_b- \frac{E_{ab}}{500R}
Ea500R=2.303(log 1011βˆ’3)\frac{E_a}{500R}=2.303(log\,10^{11}-3)
Ea=2.303Γ—RΓ—500RE_a=2.303\times R\times 500R
ln(k2k1)=βˆ’EaR(1t2βˆ’1t1)ln( \frac{k_2}{k_1})= \frac{-E_a}{R}( \frac{1}{t_2}- \frac{1}{t_1})
ln(k250 kk500 k)=βˆ’2.303Γ—RΓ—500RR(1500)ln( \frac{k_{250\,k}}{k_{500\,k}})= \frac{-2.303\times R\times500R}{R}( \frac{1}{500})
log K250 kβˆ’3=βˆ’8log\,K_{250\,k}-3=-8
log K250 k=βˆ’5log\,K_{250\,k} = -5
∣log K250 k∣=5|log\,K_{250\,k}|=5
So , correct answer is 5.
 

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Approach Solution -2

Given:
- The plot of log⁑kf\log k_f versus 1T\frac{1}{T} for the reversible reaction A(g)↔P(g)A(g) \leftrightarrow P(g).
- Pre-exponential factors for the forward and backward reactions are 1015 sβˆ’110^{15} \, s^{-1} and 1011 sβˆ’110^{11} \, s^{-1} respectively.
- log⁑K\log K at 500 K is 6.
- We need to find the value of ∣log⁑kb∣|\log k_b| at 250 K.

Steps to solve:

1. Equilibrium Constant (K) Relationship:
  K=kfkb K = \frac{k_f}{k_b}Given log⁑K=6\log K = 6 at 500 K: K=106 K = 10^6

2. Rate Constants Relation:
   kb=kfK  k_b = \frac{k_f}{K}

3. Using Arrhenius Equation:
  The Arrhenius equation for the forward reaction is:
   kf=Afeβˆ’Eaf/RT   k_f = A_f e^{-E_{af}/RT}  
  For the backward reaction:
   kb=Abeβˆ’Eab/RT  k_b = A_b e^{-E_{ab}/RT}

4. Pre-exponential Factors:
  Af=1015 sβˆ’1,Ab=1011 sβˆ’1 A_f = 10^{15} \, s^{-1}, \quad A_b = 10^{11} \, s^{-1}

5. At 500 K, find kfk_f:
  Using the equilibrium constant K=106K = 10^6 and the relation K=kfkbK = \frac{k_f}{k_b}:
  kb=kf106  k_b = \frac{k_f}{10^6}  

6. Calculate kbk_b at 250 K:
  First, find kfk_f at 250 K using Arrhenius equation.

  We know:
   log⁑kf=log⁑Afβˆ’Eaf2.303RT   \log k_f = \log A_f - \frac{E_{af}}{2.303RT}  

  Similarly for kbk_b:
   log⁑kb=log⁑Abβˆ’Eab2.303RT  \log k_b = \log A_b - \frac{E_{ab}}{2.303RT}

  Given T=250 KT = 250 \, K, calculate log⁑kf\log k_f and log⁑kb\log k_b:
  Using the known value at 500 K, let's calculate log⁑kf\log k_f and subsequently log⁑kb\log k_b.

7. Determine log⁑kf\log k_f and log⁑kb\log k_b at 250 K:

  At 500 K:
  log⁑kfβˆ’log⁑kb=log⁑K=6 \log k_f - \log k_b = \log K = 6
  Therefore:
  log⁑kf=log⁑kb+6\log k_f = \log k_b + 6

8. Using the pre-exponential factors:
  kf=1015eβˆ’Eaf/RT,kb=1011eβˆ’Eab/RTk_f = 10^{15} e^{-E_{af}/RT}, \quad k_b = 10^{11} e^{-E_{ab}/RT}

  Assume:
  log⁑kf=15βˆ’Eaf2.303Γ—8.314Γ—250,log⁑kb=11βˆ’Eab2.303Γ—8.314Γ—250 \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 500K500 K:
  Eafβ‰ˆEab E_{af} \approx E_{ab}

9. Calculate the log⁑kb\log k_b at 250 K:

  log⁑kb=11βˆ’Eab2.303Γ—8.314Γ—250\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⁑kbβˆ£β‰ˆ5 |\log k_b| \approx 5

Thus, the value of ∣log⁑kb∣|\log k_b| at 250 K is:
5\boxed{5}

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Thermodynamics

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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.
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Laws of Thermodynamics

Zeroth Law of Thermodynamics

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Second Law of Thermodynamics 

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Third Law of Thermodynamics

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