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At STP the density of a gas X is three t...

At STP the density of a gas `X` is three times that of gas `Y` while molecule mass of gas Y is twice that of X. The ratio of pressures of X and Y will be:

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To find the ratio of pressures of gases X and Y, we can use the relationship between density, molecular mass, and pressure. Let's break down the solution step by step. ### Step 1: Understand the given information We have: - Density of gas X (Dx) = 3 * Density of gas Y (Dy) - Molecular mass of gas Y (MY) = 2 * Molecular mass of gas X (MX) ### Step 2: Write the formula for density The density of a gas can be expressed using the formula: \[ D = \frac{PM}{RT} \] Where: - \( D \) = Density - \( P \) = Pressure - \( M \) = Molecular mass - \( R \) = Universal gas constant - \( T \) = Temperature ### Step 3: Express the pressures of gases X and Y From the density formula, we can rearrange it to find pressure: \[ P = \frac{D \cdot RT}{M} \] ### Step 4: Set up the ratio of pressures The ratio of pressures of gas X (PX) to gas Y (PY) can be expressed as: \[ \frac{P_X}{P_Y} = \frac{D_X \cdot R \cdot T / M_X}{D_Y \cdot R \cdot T / M_Y} \] ### Step 5: Simplify the ratio Since \( R \) and \( T \) are constants and will cancel out, we have: \[ \frac{P_X}{P_Y} = \frac{D_X}{D_Y} \cdot \frac{M_Y}{M_X} \] ### Step 6: Substitute the known values Substituting the values we have: - \( D_X = 3D_Y \) - \( M_Y = 2M_X \) So, \[ \frac{P_X}{P_Y} = \frac{3D_Y}{D_Y} \cdot \frac{2M_X}{M_X} \] ### Step 7: Simplify further This simplifies to: \[ \frac{P_X}{P_Y} = 3 \cdot 2 = 6 \] ### Conclusion Thus, the ratio of pressures of gas X to gas Y is: \[ \frac{P_X}{P_Y} = 6:1 \]

To find the ratio of pressures of gases X and Y, we can use the relationship between density, molecular mass, and pressure. Let's break down the solution step by step. ### Step 1: Understand the given information We have: - Density of gas X (Dx) = 3 * Density of gas Y (Dy) - Molecular mass of gas Y (MY) = 2 * Molecular mass of gas X (MX) ### Step 2: Write the formula for density ...
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