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The van der Waals' constant 'b' of a gas...

The van der Waals' constant 'b' of a gas is `4pixx 10^(-4)L//mol.` How near can the centeres of the two molecules approach each other? [Use :`N_(A)=6xx10^(23)`]

A

`10^(-7)` m

B

`10^(-10)` m

C

`5xx10^(-11)` m

D

`5xx10^(-9)` m

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The correct Answer is:
To solve the problem, we need to determine how near the centers of two gas molecules can approach each other, given the van der Waals constant 'b' and Avogadro's number. ### Step-by-Step Solution: 1. **Understand the van der Waals constant 'b':** The van der Waals constant 'b' is related to the volume occupied by one mole of gas molecules. It is given by the equation: \[ b = N_A \cdot \frac{4}{3} \pi R^3 \] where \( R \) is the radius of a gas molecule, and \( N_A \) is Avogadro's number. 2. **Substitute the given values:** We have: \[ b = 4 \pi \times 10^{-4} \, \text{L/mol} \] and \[ N_A = 6 \times 10^{23} \, \text{molecules/mol} \] 3. **Rearranging the equation for R:** Rearranging the equation for \( R \): \[ R^3 = \frac{3b}{4\pi N_A} \] Now substitute the values of \( b \) and \( N_A \): \[ R^3 = \frac{3 \times (4 \pi \times 10^{-4})}{4 \pi \times (6 \times 10^{23})} \] 4. **Simplifying the equation:** The \( 4\pi \) terms cancel out: \[ R^3 = \frac{3 \times 10^{-4}}{6 \times 10^{23}} = \frac{3}{6} \times 10^{-4} \times 10^{-23} = \frac{1}{2} \times 10^{-27} \] \[ R^3 = 0.5 \times 10^{-27} \] 5. **Calculating R:** Now, take the cube root: \[ R = \left(0.5 \times 10^{-27}\right)^{1/3} \] This can be calculated as: \[ R = \frac{1}{\sqrt[3]{2}} \times 10^{-9} \, \text{m} \approx 0.7937 \times 10^{-9} \, \text{m} \approx 7.937 \times 10^{-10} \, \text{m} \] 6. **Finding the distance between two molecules:** The distance between the centers of two molecules when they are just touching each other is: \[ d = 2R \approx 2 \times 7.937 \times 10^{-10} \, \text{m} \approx 1.5874 \times 10^{-9} \, \text{m} \approx 1.59 \times 10^{-9} \, \text{m} \] ### Final Answer: The centers of the two molecules can approach each other to a distance of approximately \( 1.59 \times 10^{-9} \, \text{m} \).

To solve the problem, we need to determine how near the centers of two gas molecules can approach each other, given the van der Waals constant 'b' and Avogadro's number. ### Step-by-Step Solution: 1. **Understand the van der Waals constant 'b':** The van der Waals constant 'b' is related to the volume occupied by one mole of gas molecules. It is given by the equation: \[ b = N_A \cdot \frac{4}{3} \pi R^3 ...
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van der Waal's equation for calculating the pressure of a non ideal gas is (P+(an^(2))/(V^(2)))(V-nb)=nRT van der Waal's suggested that the pressure exerted by an ideal gas , P_("ideal") , is related to the experiventally measured pressure, P_("ideal") by the equation P_("ideal")=underset("observed pressure")(underset(uarr)(P_("real")))+underset("currection term")(underset(uarr)((an^(2))/(V^(2)))) Constant 'a' is measure of intermolecular interaction between gaseous molecules that gives rise to nonideal behavior. It depends upon how frequently any two molecules approach each other closely. Another correction concerns the volume occupied by the gas molecules. In the ideal gas equation, V represents the volume of the container. However, each molecule does occupy a finite, although small, intrinsic volume, so the effective volume of the gas vecomes (V-nb), where n is the number of moles of the gas and b is a constant. The term nb represents the volume occupied by gas particles present in n moles of the gas . Having taken into account the corrections for pressure and volume, we can rewrite the ideal gas equation as follows : underset("corrected pressure")((P+(an^(2))/(V^(2))))underset("corrected volume")((V-nb))=nRT AT relatively high pressures, the van der Waals' equation of state reduces to

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