The ratio of the rates of diffusion of oxygen (\(O_2\)) and hydrogen (\(H_2\)) is given by Graham's law of diffusion:
\(\frac{r_{O_2}}{r_{H_2}} = \sqrt{\frac{M_{H_2}}{M_{O_2}}}\)
Where: - \( r_{O_2} \) and \( r_{H_2} \) are the rates of diffusion of oxygen and hydrogen, respectively, - \( M_{H_2} \) and \( M_{O_2} \) are the molar masses of hydrogen and oxygen, respectively.
Substitute the values for the molar masses of hydrogen and oxygen:
\(\frac{\frac{n_{O_2}}{t}}{\frac{n_{H_2}}{t}} = \sqrt{\frac{2}{32}} = \sqrt{\frac{1}{16}} = \frac{1}{4}\)
This simplifies to:
\(\frac{n_{O_2}}{n_{H_2}} = \frac{1}{4}\)
If \( \frac{1}{2} \) moles of \( H_2 \) are diffused in a given time, we can find the moles of \( O_2 \) diffused in the same time using the ratio:
\(\frac{n_{O_2}}{1/2} = \frac{1}{4} \Rightarrow n_{O_2} = \frac{1}{8}\)
The number of moles of oxygen (\( O_2 \)) diffused in the same time is \( \frac{1}{8} \) moles.
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :
The matter is made up of very tiny particles and these particles are so small that we cannot see them with naked eyes.
The three states of matter are as follows: