The expression for the number of molecules in a Maxwellian gas having speeds in
the range v to v + dv is
dNV=4(3.14)N((M/(2(3.14)kBT))3/2 V2 exp[-(mv2/2kBT)]dV)
Using this relation, obtain an expression for average speed. Also, plot Maxwellian
distribution function versus speed at three different temperatures.
"f(v)dv=(\\frac{m}{2\\pi k T})^{\\frac 32}4\\pi v^2 e^{-\\frac{mv^2}{2kT}}dv,"
"\\frac{df(v)}{dv}=-8\\pi(\\frac{m}{2\\pi k T})^{\\frac 32}v e^{-\\frac{mv^2}{2kT}}(\\frac{mv^2}{2kT}-1)=0,"
"\\frac{mv^2}{2kT}-1=0,"
"v=\\sqrt{\\frac{2kT}{m}}=\\sqrt{\\frac{2RT}{M}}."
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