Two containers contain the same gas at different temperatures and pressures, as indicated in the figure. The small container has a volume of 1 L, and the large container has a volume of 2 L. The two containers are then connected to each other using a thin tube, and the pressure and temperature in both containers are allowed to equalize. If the final temperature is 300. K, what is the final pressure? Assume that the connecting tube has negligible volume and mass.

THINK
As the two containers are connected to each other using a thin tube of negligible volume, then the final volume is equal to the sum of the volumes of each container,
\(V_{f}=V_{1}+V_{2}\)
The final pressure of the system can be determined by using the ideal gas law.
SKETCH
The situation can be represented with a neat sketch as follows.
RESEARCH
Ideal gas law can be represented by
\(p V=n R T \ldots \ldots\) (1)
Here \(p\) is the pressure of the gas, \(V\) is the volume occupied by the gas, \(n\) is the number of moles of the gas, \(R\) is the universal gas constant, and \(T\) is the absolute temperature of the
gas.
SIMPLIFY
The number of moles of the gas in container 1 is say \(n_{1}\), and the number of moles of the gas in container 2 is say \(n_{2}\).
Then the total number of moles at equilibrium is given by
\(n_{f}=n_{1}+n_{2} \ldots \ldots\) (2)
From the ideal gas law, we have
\(n_{1}=\frac{p_{1} V_{1}}{R T_{1}}\)
\(n_{2}=\frac{p_{2} V_{2}}{R T_{2}}\)
\(n_{f}=\frac{p_{f} V_{f}}{R T_{f}}\)
On substituting the values of \(n_{1}, n_{2}\) and \(n_{f}\) in equation (2), the final pressure can be obtained as
\(\frac{p_{f} V_{f}}{R T_{f}}=\frac{p_{1} V_{1}}{R T_{1}}+\frac{p_{2} V_{2}}{R T_{2}}\)
\(p_{f}=\frac{T_{f}}{V_{f}}\left(\frac{p_{1} V_{1}}{T_{1}}+\frac{p_{2} V_{2}}{T_{2}}\right)\)
CALCULATE
Pressure in container \(1, \quad p_{1}=3.00 \times 10^{5} \mathrm{~Pa}\)
Volume in the container \(1, V_{1}=2.00 \mathrm{~L}\)
Temperature in container \(1, T_{1}=600 \mathrm{~K}\)
Pressure in container \(2, \quad p_{2}=2.00 \times 10^{5} \mathrm{~Pa}\)
Volume in the container \(2, V_{2}=1.00 \mathrm{~L}\)
Temperature in the container \(2, T_{2}=200 \mathrm{~K}\)
At equilibrium the final volume of the gas is \(V_{f}=V_{1}+V_{2}\)
\(=2.00 \mathrm{~L}+1.00 \mathrm{~L}\)
\(=3.00 \mathrm{~L}\)
Final temperature of the gas at equilibrium, \(T_{f}=300 \mathrm{~K}\)
Substituting all these values in equation (3), the final pressure of the gas at equilibrium is:
$$ \begin{aligned} p_{f} &=\left(\frac{300 \mathrm{~K}}{3.00 \mathrm{~L}}\right)\left(\frac{\left(3.00 \times 10^{5} \mathrm{~Pa}\right)(2.00 \mathrm{~L})}{600 \mathrm{~K}}+\frac{\left(2.00 \times 10^{5} \mathrm{~Pa}\right)(1.00 \mathrm{~L})}{200 \mathrm{~K}}\right) \\ &=100(1000+1000) \mathrm{Pa} \\ &=200 \times 10^{3} \mathrm{~Pa} \\ &=200 \mathrm{kPa} \end{aligned} $$