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Question: Graph shows a hypothetical speed distribution for a sample of \(N\) gas particle (for \[V > {V_0}\]​...

Graph shows a hypothetical speed distribution for a sample of NN gas particle (for V>V0V > {V_0}​;dNdV=0\dfrac{{dN}}{{dV}} = 0,dNdV\dfrac{{dN}}{{dV}}​ is a rate of change of number of particles with change velocity.)

A. The value of aV0a{V_0} is 2N2N
B. The ratio of VavgV0\dfrac{{{V_{avg}}}}{{{V_0}}} is equal to 23\dfrac{2}{3}
C. The ratio of VrmsV0\dfrac{{{V_{rms}}}}{{{V_0}}} is equal to 12\dfrac{1}{{\sqrt 2 }}
D. Three fourth of the total particle has a speed between 0.5V00.5{V_0}and V0{V_0}

Explanation

Solution

To solve this problem find the value of the rate of change of number of particles with change in velocity. Then find the relation between the V0{V_0} and the number of particles NN.

Formula used:
The equation of straight line is given by,
y=mx+cy = mx + c
where, mm is the slope of the straight line and cc is the interception on the Y-axis.

Complete step by step answer:
From the graph we can see that the slope of the curve is, aV0\dfrac{a}{{{V_0}}} since the maximum value of Y-axis is aa and on the X-axis it is V0{V_0} minimum value is zero. The interception on the Y-axis is zero. The Y variable is here the rate of change of number of particles with change in velocity dNdV\dfrac{{dN}}{{dV}} and the X-axis plot is V0{V_0}.

Hence, we can write the equation of the curve as, dNdV=aV0V\dfrac{{dN}}{{dV}} = \dfrac{a}{{{V_0}}}V
Now, we can rewrite this as, dN=aV0VdVdN = \dfrac{a}{{{V_0}}}VdV
Integrating over the limit for NN 0N0 \to N and for VV 0V00 \to {V_0} we have,
0NdN=aV00V0VdV\int\limits_0^N {dN} = \dfrac{a}{{{V_0}}}\int\limits_0^{{V_0}} {VdV}
Putting the value of the limit we have,
N=aV0V022N = \dfrac{a}{{{V_0}}}\dfrac{{{V_0}^2}}{2}
Up on simplifying we have, N=aV02N = \dfrac{{a{V_0}}}{2}
So, we can see, 2N=aV02N = a{V_0}
Hence, the value of aV0a{V_0} is 2N2N

Hence, option A is the correct answer.

Note: The r.m.s value of VV is Vrms=1N0V0V2dN{V_{rms}} = \dfrac{1}{N}\int\limits_0^{{V_0}} {{V^2}dN} which is equal to the aV034N\sqrt {\dfrac{{a{V_0}^3}}{{4N}}} and the average value of VV is Vavg=1N0V0VdN{V_{avg}} = \dfrac{1}{N}\int\limits_0^{{V_0}} {VdN} which is equal to the value aV023N\dfrac{{a{V_0}^2}}{{3N}}. Hence, all the options except option (A) are incorrect. You can perform the integration by yourself to check the answers for further insight.