First slide

laws

Question

Pressure exerted by a gas at constant temperature is

Easy

A

independent of density of the gas
B

inversely proportional of the density of the gas
C

directly proportional to the square of density of the gas
D

directly proportional to the density of the gas

Solution

$P = \frac{n R T}{V} = \frac{n M R T}{V M} (M = m o l e c u l a r m a s s) P = (\frac{m}{V}) \frac{R T}{M} = ρ \frac{R T}{M} (m = m a s s o f t h e g a s) P \infty ρ$

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