
For gaseous state, if most probable speed is denoted by ${C^*}$, average speed by \[\overline C \] and root mean square speed by C, then for large number of molecules the ratio of these speeds are:
a- ${C^*}$: $\overline C $ : C = 1.128 : 1.225 : 1
b- ${C^*}$: $\overline C $ : C = 1 : 1.128 : 1.225
c- ${C^*}$: $\overline C $ : C = 1 :1.125 : 1.128
d- ${C^*}$: $\overline C $ : C = 1.125 : 1.128 : 1
Answer
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Hint: The given three representations of velocity are related to each other by following formula:
${C^*}$: $\overline C $ : C = $\sqrt {\dfrac{{2RT}}{M}} $ : $\sqrt {\dfrac{{8RT}}{{\pi M}}} $: $\sqrt {\dfrac{{3RT}}{M}} $
Complete answer:
Kinetic Molecular Theory explains the macroscopic properties of gases and can be used to calculate the different kinds of gaseous speeds. Measuring the velocities of particles at a given time results in a large distribution of values; some particles may move very slowly, others very quickly, and because they are constantly moving in different directions, the velocity could equal zero.
-Most probable speed (${C^*}$): The most probable speed is the speed most likely to be possessed by any molecule of the same mass m in the gaseous system and corresponds to the maximum value. And it is given by the following formula:
C*= $\sqrt {\dfrac{{2RT}}{M}} $
-Average speed (\[\overline C \]): Movement of gaseous molecules is in random speeds and in random directions. The Maxwell-Boltzmann Distribution describes the average speeds of collection gaseous particles at a given temperature. And it is given by:
\[\overline C \]=$\sqrt {\dfrac{{8RT}}{{\pi M}}} $
-Root mean square speed (C or ${C_{rms}}$): As the name represents roots of mean of squares of the velocities is known as the root-mean-square (RMS) velocity, and it is represented as follows:
C or ${C_{rms}}$=$\sqrt {\dfrac{{3RT}}{M}} $
On comparing these three velocities:
${C^*}$: $\overline C $ : C = $\sqrt {\dfrac{{2RT}}{M}} $ : $\sqrt {\dfrac{{8RT}}{{\pi M}}} $: $\sqrt {\dfrac{{3RT}}{M}} $
=$\sqrt 2 :\sqrt {\dfrac{8}{\pi }} :\sqrt 3 $
=1 : 1.128 : 1.225
So, the correct option is (B) 1: 1.128: 1.225 .
Note:
Most probable speed, average speed, and root mean square speed are related to each other by the formula stated above.Their relation can be expressed as a graph as shown below:
${C^*}$: $\overline C $ : C = $\sqrt {\dfrac{{2RT}}{M}} $ : $\sqrt {\dfrac{{8RT}}{{\pi M}}} $: $\sqrt {\dfrac{{3RT}}{M}} $
Complete answer:
Kinetic Molecular Theory explains the macroscopic properties of gases and can be used to calculate the different kinds of gaseous speeds. Measuring the velocities of particles at a given time results in a large distribution of values; some particles may move very slowly, others very quickly, and because they are constantly moving in different directions, the velocity could equal zero.
-Most probable speed (${C^*}$): The most probable speed is the speed most likely to be possessed by any molecule of the same mass m in the gaseous system and corresponds to the maximum value. And it is given by the following formula:
C*= $\sqrt {\dfrac{{2RT}}{M}} $
-Average speed (\[\overline C \]): Movement of gaseous molecules is in random speeds and in random directions. The Maxwell-Boltzmann Distribution describes the average speeds of collection gaseous particles at a given temperature. And it is given by:
\[\overline C \]=$\sqrt {\dfrac{{8RT}}{{\pi M}}} $
-Root mean square speed (C or ${C_{rms}}$): As the name represents roots of mean of squares of the velocities is known as the root-mean-square (RMS) velocity, and it is represented as follows:
C or ${C_{rms}}$=$\sqrt {\dfrac{{3RT}}{M}} $
On comparing these three velocities:
${C^*}$: $\overline C $ : C = $\sqrt {\dfrac{{2RT}}{M}} $ : $\sqrt {\dfrac{{8RT}}{{\pi M}}} $: $\sqrt {\dfrac{{3RT}}{M}} $
=$\sqrt 2 :\sqrt {\dfrac{8}{\pi }} :\sqrt 3 $
=1 : 1.128 : 1.225
So, the correct option is (B) 1: 1.128: 1.225 .
Note:
Most probable speed, average speed, and root mean square speed are related to each other by the formula stated above.Their relation can be expressed as a graph as shown below:
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