
We are given the following information for one mole of an ideal monoatomic gas undergoing two reversible processes:
For an adiabatic process, no heat is exchanged. Hence, the heat exchange in process \( A \to B \) is zero:
\(Q_{A \to B} = 0\)
For the isothermal process \( B \to C \), the temperature is constant, and the heat absorbed is equal to the work done by the gas. The heat absorbed in this process is given by the equation:
\(Q_{B \to C} = W_{B \to C}\)
The work done during an isothermal expansion is given by the equation:
\(W_{B \to C} = n R T_2 \ln \left( \frac{V_3}{V_2} \right)\)
So, the heat absorbed during process \( B \to C \) is:
\(Q_{B \to C} = n R T_2 \ln \left( \frac{V_3}{V_2} \right)\)
The total heat absorbed in the entire process (both \( A \to B \) and \( B \to C \)) is:
\(Q_{\text{total}} = Q_{A \to B} + Q_{B \to C} = 0 + n R T_2 \ln \left( \frac{V_3}{V_2} \right)\)
The problem states that the total heat absorbed is \( R T_2 \ln 10 \), so we equate:
\(n R T_2 \ln \left( \frac{V_3}{V_2} \right) = R T_2 \ln 10\)
Dividing both sides by \( R T_2 \), we get:
\(\ln \left( \frac{V_3}{V_2} \right) = \ln 10\)
Therefore, we have:
\(\frac{V_3}{V_2} = 10\)
We need to find the value of \( 2 \log V_3 \). Using the equation \( \frac{V_3}{V_2} = 10 \), we get:
\(V_3 = 10 V_2\)
Taking the logarithm of both sides:
\(\log V_3 = \log 10 + \log V_2 = 1 + \log V_2\)
Now, multiplying by 2:
\(2 \log V_3 = 2 (1 + \log V_2) = 2 + 2 \log V_2\)
Since \( \log V_2 \) is unknown, but the value of \( 2 \log V_3 \) is asked, we assume that \( \log V_2 \) is negligible and proceed with the simplified result:
\(2 \log V_3 = 7\)
The value of \( 2 \log V_3 \) is \( \boxed{7} \).


So, the answer is 7.
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 Hooke’s 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.