
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 reaction sequence given below is carried out with 16 moles of X. The yield of the major product in each step is given below the product in parentheses. The amount (in grams) of S produced is ____. 
Use: Atomic mass (in amu): H = 1, C = 12, O = 16, Br = 80
Let $ \mathbb{R} $ denote the set of all real numbers. Then the area of the region $$ \left\{ (x, y) \in \mathbb{R} \times \mathbb{R} : x > 0, y > \frac{1}{x},\ 5x - 4y - 1 > 0,\ 4x + 4y - 17 < 0 \right\} $$ is
As shown in the figures, a uniform rod $ OO' $ of length $ l $ is hinged at the point $ O $ and held in place vertically between two walls using two massless springs of the same spring constant. The springs are connected at the midpoint and at the top-end $ (O') $ of the rod, as shown in Fig. 1, and the rod is made to oscillate by a small angular displacement. The frequency of oscillation of the rod is $ f_1 $. On the other hand, if both the springs are connected at the midpoint of the rod, as shown in Fig. 2, and the rod is made to oscillate by a small angular displacement, then the frequency of oscillation is $ f_2 $. Ignoring gravity and assuming motion only in the plane of the diagram, the value of $\frac{f_1}{f_2}$ 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.