We are given the following information:
We need to find the number of moles of $N_2$ from air dissolved in 10 moles of water.
Step 1: Calculate the partial pressure of $N_2$ in the air.
According to Dalton's law of partial pressures, the partial pressure of a gas in a mixture is the product of its mole fraction and the total pressure.
$P_{N_2} = y_{N_2} \times P_{total}$
$P_{N_2} = 0.8 \times 5$ atm
$P_{N_2} = 4$ atm
Step 2: Apply Henry's law to find the mole fraction of $N_2$ dissolved in water.
Henry's law relates the partial pressure of a gas above a liquid to the mole fraction of the gas dissolved in the liquid:
$P_{N_2} = K_H \times x_{N_2}$
Where $x_{N_2}$ is the mole fraction of $N_2$ dissolved in water.
Rearranging the formula to solve for $x_{N_2}$:
$x_{N_2} = \frac{P_{N_2}}{K_H}$
$x_{N_2} = \frac{4 \text{ atm}}{1.0 \times 10^5 \text{ atm}}$
$x_{N_2} = 4 \times 10^{-5}$
Step 3: Calculate the number of moles of $N_2$ dissolved in water.
The mole fraction of $N_2$ in the solution is defined as:
$x_{N_2} = \frac{n_{N_2}}{n_{N_2} + n_{water}}$
Where $n_{N_2}$ is the number of moles of dissolved $N_2$ and $n_{water}$ is the number of moles of water.
Since the solubility of $N_2$ in water is very low (indicated by the small mole fraction $x_{N_2} = 4 \times 10^{-5}$), the number of moles of dissolved $N_2$ ($n_{N_2}$) is much smaller than the number of moles of water ($n_{water}$). Therefore, we can approximate the denominator:
$n_{N_2} + n_{water} \approx n_{water}$
So, the mole fraction expression simplifies to:
$x_{N_2} \approx \frac{n_{N_2}}{n_{water}}$
Now, we can solve for $n_{N_2}$:
$n_{N_2} \approx x_{N_2} \times n_{water}$
$n_{N_2} \approx (4 \times 10^{-5}) \times (10 \text{ moles})$
$n_{N_2} \approx 40 \times 10^{-5}$ moles
$n_{N_2} \approx 4.0 \times 10^1 \times 10^{-5}$ moles
$n_{N_2} \approx 4.0 \times 10^{-4}$ moles
The final answer is \(4.0 \times 10^{-4}\).
1. Calculate the partial pressure of N2 in the air:
According to Dalton's Law of Partial Pressures, the partial pressure of a gas in a mixture is its mole fraction multiplied by the total pressure.
PN2 = Mole fraction of N2 × Total pressure
PN2 = 0.8 × 5 atm = 4.0 atm
2. Apply Henry's Law to find the mole fraction of N2 dissolved in water:
Henry's Law states: Pgas = KH × Xgas(dissolved)
Where:
- Pgas is the partial pressure of the gas above the solution (PN2 = 4.0 atm).
- KH is Henry's law constant (1.0 × 105 atm).
- Xgas(dissolved) is the mole fraction of the gas dissolved in the liquid (XN2(dissolved)).
Rearranging the formula to solve for XN2(dissolved):
XN2(dissolved) = PN2 / KH
XN2(dissolved) = 4.0 atm / (1.0 × 105 atm) = 4.0 × 10-5
3. Calculate the number of moles of N2 dissolved:
The mole fraction of N2 dissolved is defined as:
XN2(dissolved) = nN2 / (nN2 + nwater)
Where:
- nN2 is the number of moles of N2 dissolved.
- nwater is the number of moles of water (given as 10 moles).
So, 4.0 × 10-5 = nN2 / (nN2 + 10)
Since the solubility of N2 is very low (indicated by the small mole fraction), the number of moles of dissolved N2 (nN2) will be much smaller than the number of moles of water (nwater). Therefore, we can approximate the denominator: (nN2 + nwater) ≈ nwater.
XN2(dissolved) ≈ nN2 / nwater
nN2 ≈ XN2(dissolved) × nwater
nN2 ≈ (4.0 × 10-5) × (10 moles)
nN2 ≈ 40 × 10-5 moles
nN2 ≈ 4.0 × 10-4 moles
Therefore, the number of moles of N2 from air dissolved in 10 moles of water is 4.0 × 10-4.
Final Answer: The final answer is $4.0 \times 10^{-4}$.
Among the following, identify the compound that is not an isomer of hexane:
In an experiment to determine the figure of merit of a galvanometer by half deflection method, a student constructed the following circuit. He applied a resistance of \( 520 \, \Omega \) in \( R \). When \( K_1 \) is closed and \( K_2 \) is open, the deflection observed in the galvanometer is 20 div. When \( K_1 \) is also closed and a resistance of \( 90 \, \Omega \) is removed in \( S \), the deflection becomes 13 div. The resistance of galvanometer is nearly:
A block of certain mass is placed on a rough floor. The coefficients of static and kinetic friction between the block and the floor are 0.4 and 0.25 respectively. A constant horizontal force \( F = 20 \, \text{N} \) acts on it so that the velocity of the block varies with time according to the following graph. The mass of the block is nearly (Take \( g = 10 \, \text{m/s}^2 \)):