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Question: If \( 2moles \) of an ideal monatomic gas at a temperature \( {T_0} \) is mixed with \( 4mole \) of ...

If 2moles2moles of an ideal monatomic gas at a temperature T0{T_0} is mixed with 4mole4mole of another ideal monatomic gas at a temperature 2T02{T_0} then the temperature of the mixture is:
(A) 53T0\dfrac{5}{3}{T_0}
(B) 32T0\dfrac{3}{2}{T_0}
(C) 43T0\dfrac{4}{3}{T_0}
(D) 54T0\dfrac{5}{4}{T_0}

Explanation

Solution

Use the energy conservation law and law of equipartition energy to solve the problem. Law of conservation of energy: E=E1+E2E = {E_1} + {E_2} where, E1{E_1} and E2{E_2} are the individual internal energies of the components of mixture respectively and EE is the internal energy of the total mixture.
Law of Equipartition of Energy: E=12fnRTE = \dfrac{1}{2}fnRT where ff is the degree of freedom, nn is the number of moles of the ideal gas, RR is the universal gas constant and TT is the absolute temperature .

Complete step by step solution:
From the given question we have the information about the number of moles of the ideal gases, their temperature and their type i.e., monoatomic gases. We are asked to calculate the temperature of the mixture of the two gases.
We know by conservation of energy that total internal energy of a system remains conserved. So, if E1{E_1} be the internal energy of the monatomic gas at temperature T0{T_0} , E2{E_2} be the internal energy of the monatomic gas at temperature 2T02{T_0} and EE be the internal energy of the total mixture then by law of conservation of energy we can write:
E=E1+E2E = {E_1} + {E_2} ............................... eqn(1)\to eqn(1)
The law of equipartition of energy states that for a system of particles at absolute temperature TT ,the average internal energy associated with each degree of freedom( ff ) is 12fnRT\dfrac{1}{2}fnRT where nn and RR have the same physical meanings as stated above.
Thus, substituting the value of internal energy in eqn(1)eqn(1) we can write:
12f(n1+n2)RT=12fn1RT1+12fn2RT2\dfrac{1}{2}f({n_1} + {n_2})RT = \dfrac{1}{2}f{n_1}R{T_1} + \dfrac{1}{2}f{n_2}R{T_2} eqn(2)\to eqn(2)
Where, n1=2mole{n_1} = 2mole ; n2=4mole{n_2} = 4mole ; T1=T0{T_1} = {T_0} ; T2=2T0{T_2} = 2{T_0} (from the given question)
Cancelling ff and RR on both sides as the degrees of freedom is equal for all monatomic gases and Universal gas constant is a constant term for all gases, we can rewrite eqn(2)eqn(2) as:
(n1+n2)T=n1T1+n2T2({n_1} + {n_2})T = {n_1}{T_1} + {n_2}{T_2}
Substituting the values, we have,
(2+4)T=2T0+4(2T0)\Rightarrow (2 + 4)T = 2{T_0} + 4(2{T_0})
T=106T0=53T0\Rightarrow T = \dfrac{{{\text{10}}}}{6}{T_0} = \dfrac{5}{3}{T_0}
Thus, option A is the correct answer to the question.

Note:
Degrees of freedom can be defined as the minimum number of coordinates required to specify the configuration of a dynamic system.
For a monatomic gas f=3f = 3 .