An ideal diatomic gas is made up of molecules that do not vibrate. Its volume compressed by a factor of 32,without any exchange of heat. If the initial and final pressures are P1 and P2,respectively,the ratio P1:P2,is:
7:5
128:1
1:32
32:1
3:08
The correct answer is (B): \(128:1\)
To determine the ratio of the initial pressure \(P_1\) to the final pressure \(P_2\) for an ideal diatomic gas (which does not vibrate) undergoing adiabatic compression, we need to use the adiabatic condition for an ideal gas.
For an ideal diatomic gas, which has 5 degrees of freedom (3 translational + 2 rotational), the adiabatic index (γ) is:
\[ \gamma = \frac{7}{5} = 1.4 \]
The adiabatic relation for pressure and volume is given by:
\[ P_1 V_1^\gamma = P_2 V_2^\gamma \]
Here, \( V_1 \) is the initial volume and \( V_2 \) is the final volume. The problem states that the volume is compressed by a factor of 32, so:
\[ V_2 = \frac{V_1}{32} \]
Using the adiabatic condition, we have:
\[ P_1 V_1^\gamma = P_2 V_2^\gamma \]
\[ P_1 V_1^\gamma = P_2 \left( \frac{V_1}{32} \right)^\gamma \]
\[ P_1 V_1^\gamma = P_2 \frac{V_1^\gamma}{32^\gamma} \]
\[ P_1 = P_2 \frac{1}{32^\gamma} \]
\[ \frac{P_1}{P_2} = 32^\gamma \]
Substitute \(\gamma = 1.4\) into the equation:
\[ \frac{P_1}{P_2} = 32^{1.4} \]
Now we calculate \( 32^{1.4} \):
\[ 32 = 2^5 \]
\[ 32^{1.4} = (2^5)^{1.4} = 2^{5 \cdot 1.4} = 2^7 = 128 \]
Therefore, the ratio \( P_1 : P_2 \) is:
\[ P_1 : P_2 = 128 \]
So, the final answer is:
\[ P_1 : P_2 = 128 : 1 \]
Thus The correct answer is Option (B): \(128:1\)
List-I | List-II | ||
(A) | Isothermal process | (I) | No heat exchange |
(B) | Isochoric process | (II) | Carried out at constant temperature |
(C) | Isobaric process | (III) | Carried out at constant volume |
(D) | Adiabatic process | (IV) | Carried out at constant pressure |
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.