Home
Class 12
CHEMISTRY
The density of air 380K and 722 mm of Hg...

The density of air 380K and 722 mm of Hg is lg/`cm^3`. If air is cooled to 100K and 1 atm the final density is :

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem of finding the final density of air when it is cooled from 380 K and 722 mm of Hg to 100 K and 1 atm, we can use the ideal gas law and the relationship between density, pressure, and temperature. Here’s a step-by-step breakdown of the solution: ### Step 1: Convert Initial Pressure to Atmospheres The initial pressure \( P_1 \) is given as 722 mm of Hg. We need to convert this to atmospheres (atm) using the conversion factor \( 1 \text{ atm} = 760 \text{ mm of Hg} \). \[ P_1 = \frac{722 \text{ mm of Hg}}{760 \text{ mm of Hg/atm}} = 0.95 \text{ atm} \] **Hint:** Remember that to convert mm of Hg to atm, you divide by 760. ### Step 2: Identify Given Values We have the following values: - Initial Temperature \( T_1 = 380 \text{ K} \) - Initial Density \( d_1 = 1 \text{ g/cm}^3 \) - Final Temperature \( T_2 = 100 \text{ K} \) - Final Pressure \( P_2 = 1 \text{ atm} \) ### Step 3: Use the Ideal Gas Law Relationship According to the ideal gas law, the relationship between pressure, density, and temperature can be expressed as: \[ \frac{P_1}{d_1 T_1} = \frac{P_2}{d_2 T_2} \] Where: - \( d_2 \) is the final density we need to find. ### Step 4: Rearrange the Equation to Solve for \( d_2 \) Rearranging the equation gives us: \[ d_2 = \frac{P_2 \cdot d_1 \cdot T_2}{P_1 \cdot T_1} \] ### Step 5: Substitute the Known Values Now, we can substitute the known values into the equation: \[ d_2 = \frac{(1 \text{ atm}) \cdot (1 \text{ g/cm}^3) \cdot (100 \text{ K})}{(0.95 \text{ atm}) \cdot (380 \text{ K})} \] ### Step 6: Calculate \( d_2 \) Calculating the numerator and denominator: \[ d_2 = \frac{100}{0.95 \cdot 380} \] Calculating the denominator: \[ 0.95 \cdot 380 = 361 \] Now substituting back: \[ d_2 = \frac{100}{361} \approx 0.277 \text{ g/cm}^3 \] ### Step 7: Final Calculation Now, we can simplify this to find the final density: \[ d_2 \approx 0.277 \text{ g/cm}^3 \] ### Conclusion The final density of air when cooled to 100 K and 1 atm is approximately \( 0.277 \text{ g/cm}^3 \). ---
Promotional Banner

Similar Questions

Explore conceptually related problems

A flask containing air at 107^(@)C and 722 mm of Hg is cooled to 100 K and 760 mm of Hg. If density in the initial condition 1g//cm^(3) , then what is the final density (g//cm^(3)) ?

When the air cools, its density :

The density of a gas is 1.964 g dm^(-3) at 273 K and 76 cm Hg . The gas is

The temperature and pressure at Simla are 15.0^(@)C and 72.0cm of mercury and at Kalka these are 35.0^(@)C and 76.0 cm of mercury. Find the ratio of air density at Kalka to the air density at Simla.

A rain drop with radus 1.5 mm falls from a cloud at a height 1200 m from ground . The density of water is 1000 kg//m^(3) and density of air is 1.2 kg//m^(3) . Assume the drop was spherical throughout the fall and there is no air drag. The impact speed of the drop will be :

Air contained in a cylinder at 20.0^(@)C is compressed froma n initial pressure of 1.00 atm, and volume of 700 cm^(3) to a volume of 70.0cm^(3) . If the final pressure is 15.0 atm then what is the final temperature?

The HF_(2)^(Θ) ion solid state and in liquid HF but not in the dilute aqueous solution At 300 K and 1.00 atm, the density of HF is 3.17 gL^(-1) We conclude that there is a .

The relative density of a material is found by weighing the body first in air and then in water . If the weight in air is ( 10.0 +- 0.1) gf and the weight in water is ( 5.0 +- 0.1) gf , then the maximum permissible percentage error in relative density is

The density of a gas is 1.964 g/ dm^(-3) at 273 K and 76 cm Hg. Calculate the molecular weight of the gas.

Density of air (in g/L) at 307°C and 2 atm pressure is (Average molar mass of air is 29 g mol-1)