The adiabatic exponent γ for a mixture of gases can be calculated using the mole fraction of each gas and their respective γ values.
Given Values: Moles of monoatomic gas n1 = 3, with γ1 = \( \frac{5}{3} \). Moles of diatomic gas n2 = 2, with γ2 = \( \frac{7}{5} \).
Calculating Total Moles: Total moles n = n1 + n2 = 3 + 2 = 5.
Using the Formula for γ of the Mixture: The formula for the adiabatic exponent of the mixture γmixture is given by:
\[ \gamma_{\text{mixture}} = \frac{n_1 \gamma_1 + n_2 \gamma_2}{n_1 + n_2} \]
Substituting the Values:
\[ \gamma_{\text{mixture}} = \frac{3 \times \frac{5}{3} + 2 \times \frac{7}{5}}{5} = \frac{5 + 14}{5} = \frac{25 + 14}{25} = \frac{39}{25} = 1.56 \]
Final Calculation: The average adiabatic exponent simplifies to:
\[ \gamma_{\text{mixture}} = \frac{29}{19} \approx 1.52 \]
The problem asks to find the value of the adiabatic exponent \( \gamma \) for a mixture of a monoatomic gas and a diatomic gas, given their respective number of moles and adiabatic exponents.
For a mixture of non-reacting ideal gases, the molar specific heat at constant volume (\( C_{v, \text{mix}} \)) and the molar specific heat at constant pressure (\( C_{p, \text{mix}} \)) are the weighted averages of the individual molar specific heats, weighted by the number of moles.
\[ C_{v, \text{mix}} = \frac{n_1 C_{v,1} + n_2 C_{v,2}}{n_1 + n_2} \] \[ C_{p, \text{mix}} = \frac{n_1 C_{p,1} + n_2 C_{p,2}}{n_1 + n_2} \]The adiabatic exponent for the mixture (\( \gamma_{\text{mix}} \)) is the ratio of these two values:
\[ \gamma_{\text{mix}} = \frac{C_{p, \text{mix}}}{C_{v, \text{mix}}} = \frac{n_1 C_{p,1} + n_2 C_{p,2}}{n_1 C_{v,1} + n_2 C_{v,2}} \]The molar specific heats for a gas are related to its adiabatic exponent \( \gamma \) by the following formulas, where \( R \) is the universal gas constant:
\[ C_v = \frac{R}{\gamma - 1} \quad \text{and} \quad C_p = \frac{\gamma R}{\gamma - 1} \]Step 1: List the given information for each gas.
For the monoatomic gas (Gas 1):
For the diatomic gas (Gas 2):
Step 2: Calculate the molar specific heats (\( C_v \) and \( C_p \)) for the monoatomic gas.
\[ C_{v,1} = \frac{R}{\gamma_1 - 1} = \frac{R}{\frac{5}{3} - 1} = \frac{R}{\frac{2}{3}} = \frac{3}{2}R \] \[ C_{p,1} = \frac{\gamma_1 R}{\gamma_1 - 1} = \frac{\frac{5}{3} R}{\frac{2}{3}} = \frac{5}{2}R \]Step 3: Calculate the molar specific heats (\( C_v \) and \( C_p \)) for the diatomic gas.
\[ C_{v,2} = \frac{R}{\gamma_2 - 1} = \frac{R}{\frac{7}{5} - 1} = \frac{R}{\frac{2}{5}} = \frac{5}{2}R \] \[ C_{p,2} = \frac{\gamma_2 R}{\gamma_2 - 1} = \frac{\frac{7}{5} R}{\frac{2}{5}} = \frac{7}{2}R \]Step 4: Calculate the numerator and denominator for the \( \gamma_{\text{mix}} \) formula.
The numerator is \( n_1 C_{p,1} + n_2 C_{p,2} \):
\[ n_1 C_{p,1} + n_2 C_{p,2} = 3 \left( \frac{5}{2}R \right) + 2 \left( \frac{7}{2}R \right) = \frac{15}{2}R + \frac{14}{2}R = \frac{29}{2}R \]The denominator is \( n_1 C_{v,1} + n_2 C_{v,2} \):
\[ n_1 C_{v,1} + n_2 C_{v,2} = 3 \left( \frac{3}{2}R \right) + 2 \left( \frac{5}{2}R \right) = \frac{9}{2}R + \frac{10}{2}R = \frac{19}{2}R \]Now, we can find the adiabatic exponent for the mixture by dividing the numerator by the denominator.
\[ \gamma_{\text{mix}} = \frac{n_1 C_{p,1} + n_2 C_{p,2}}{n_1 C_{v,1} + n_2 C_{v,2}} = \frac{\frac{29}{2}R}{\frac{19}{2}R} \]Canceling the common terms \( \frac{R}{2} \), we get:
\[ \gamma_{\text{mix}} = \frac{29}{19} \]The value of the adiabatic exponent \( \gamma \) for the mixture is \( \frac{29}{19} = 1.52 \).
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)