Here, MO = molar mass and M = mass of gas molecule,
Urms = \(\frac{\sqrt{3}RT}{M}\)
Urms ∝ \(\sqrt{\frac{1}{m}}\) ⇒ Urms ∝ \(\frac{1}{m^{\frac{1}{2}}}\)
⇒ Urms ∝ \(m^{-\frac{1}{2}}\)
Hence, the correct option is ‘C '.i.e. \(m^{-\frac{1}{2}}\)
Root mean square velocity(Urms) is the square root of the average square of velocity.
Urms = \(\frac{\sqrt{3}RT}{M}\), where R= gas constant, T= temperature, M= molar mass
Urms ∝ \(\sqrt{\frac{1}{m}}\) ⇒ Urms ∝ \(\sqrt{\frac{1}{m}}\)
⇒ Urms ∝ \(\frac{1}{m^{\frac{1}{2}}}\)
⇒ Urms ∝ \(m^{-\frac{1}{2}}\)
Hence, the correct option is ‘C '.i.e. \(m^{-\frac{1}{2}}\)
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: