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Question: What will be the ratio of the root mean square speeds of the molecules of an ideal gas at \[270K\] a...

What will be the ratio of the root mean square speeds of the molecules of an ideal gas at 270K270K and30K30K?

Explanation

Solution

In order to solve this question, we are going to firstly write the formula for the root mean square speeds of the molecules of a gas. After that, the speeds of the molecules are calculated at the two different temperatures as given in the question and then, the ratio is calculated by dividing.

Formula used:
The root mean square speed of the molecules is given as:
vrms=3RTm{v_{rms}} = \sqrt {\dfrac{{3RT}}{m}}
Where, TTis the temperature, mmis the mass of the molecules and RRis the Gas constant.

Complete step-by-step solution:
It is given in the question that the values of the two temperatures are as follows:
{T_1} = 270K \\\ {T_2} = 30K \\\
We know that the root mean square speed of the molecules is given as:
vrms=3RTm{v_{rms}} = \sqrt {\dfrac{{3RT}}{m}}
Where, TTis the temperature, mmis the mass of the molecules and RRis the Gas constant.
Putting the values of the temperatures and calculating the root mean square speeds of the molecules:
{v_{rms\left( 1 \right)}} = \sqrt {\dfrac{{3R \times 270}}{m}} \\\ {v_{rms\left( 2 \right)}} = \sqrt {\dfrac{{3R \times 30}}{m}} \\\
Dividing the above two root mean square speed equations in order to get the ratio of the two, we get
\dfrac{{{v_{rms\left( 1 \right)}}}}{{{v_{rms\left( 2 \right)}}}} = \dfrac{{\sqrt {\dfrac{{3R \times 270}}{m}} }}{{\sqrt {\dfrac{{3R \times 30}}{m}} }} \\\
\Rightarrow \dfrac{{{v_{rms\left( 1 \right)}}}}{{{v_{rms\left( 2 \right)}}}} = \sqrt {\dfrac{{270}}{{30}}} = \sqrt 9 = 3 \\\

Hence, the ratio of the root mean square speeds of the molecules of an ideal gas at 270K270K and30K30Kis3:13:1.

Note: It is important to note that the root-mean-square speed is the measure of the speed of particles in a gas, defined as the square root of the average velocity-squared of the molecules in a gas. The mass and the Gas constant values for a particular gas remain the same and only temperature is the variant.