
Given: The equation for the equilibrium constant \( K \) is related to the forward and backward rate constants \( k_f \) and \( k_b \) as:
\(\log K = \log \left( \frac{k_f}{k_b} \right)\)
Thus, we can express \( K \) as:
\(K = \frac{k_f}{k_b}\)
We are given that \( 6 = \log k_f - \log k_b \), and also that \( \log k_f = 9 \) at 500 K. Therefore, we can substitute these values into the equation:
\(6 = 9 - \log k_b\)
Solving for \( \log k_b \):
\(\log k_b = 3 \quad \text{at} \, 500K\)
The Arrhenius equation gives the rate constant \( k_b \) as:
\(k_b = A_b e^{\frac{-E_{ab}}{RT}}\)
Taking the natural logarithm of both sides:
\(\ln k_b = \ln A_b - \frac{E_{ab}}{RT}\)
Multiplying both sides by 2.303 to convert to base 10 logarithms:
\(2.303 \log k_b = 2.303 \log A_b - \frac{E_{ab}}{500R}\)
Now, we use the equation for the logarithmic difference of the rate constants at two temperatures \( T_1 = 500 K \) and \( T_2 = 250 K \):
\(\frac{E_a}{500R} = 2.303 \left( \log 10^{11} - 3 \right)\)
Simplifying this expression:
\(E_a = 2.303 \times R \times 500\)
Next, we calculate the logarithmic ratio of the rate constants at 250 K and 500 K:
\(\ln \left( \frac{k_{250K}}{k_{500K}} \right) = \frac{-2.303 \times R \times 500}{R} \left( \frac{1}{500} - \frac{1}{250} \right)\)
This simplifies to:
\(\log K_{250K} - 3 = -8\)
Solving for \( \log K_{250K} \), we get:
\(\log K_{250K} = -5\)
Taking the absolute value, we find:
\(| \log K_{250K} | = 5\)
The 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:
\[\boxed{5}\]
An amount of ice of mass \( 10^{-3} \) kg and temperature \( -10^\circ C \) is transformed to vapor of temperature \( 110^\circ C \) by applying heat. The total amount of work required for this conversion is,
(Take, specific heat of ice = 2100 J kg\(^{-1}\) K\(^{-1}\),
specific heat of water = 4180 J kg\(^{-1}\) K\(^{-1}\),
specific heat of steam = 1920 J kg\(^{-1}\) K\(^{-1}\),
Latent heat of ice = \( 3.35 \times 10^5 \) J kg\(^{-1}\),
Latent heat of steam = \( 2.25 \times 10^6 \) J kg\(^{-1}\))
Match List-I with List-II.
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hookeβs law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.
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.