Radial wave function of hydrogen atom in 2p state is "R_{21}=\\frac{1}{\\sqrt{3}}(\\frac{1}{2a})^{\\frac{3}{2}}(\\frac{r}{a})e^{-(\\frac{r}{2a})}"
The radial probability is
"|R_{21}|^2r^2=\\frac{1}{{3}}(\\frac{1}{2a})^{3}(\\frac{r}{a})^2e^{-(\\frac{r}{a})}r^2"
To find the maximum value of above equation, Differentiating above equation with respect to r and equating to zero, we get
"\\frac{d}{dr}|R_{21}|^2r^2=0"
"\\frac{d}{dr}[\\frac{1}{{3}}(\\frac{1}{2a})^{3}(\\frac{r}{a})^2e^{-(\\frac{r}{a})}r^2]=0"
"\\frac{d}{dr}[r^4e^{-(\\frac{r}{a})}]=0"
"[4r^3e^{-(\\frac{r}{a})}+r^4(-\\frac{1}{a})e^{-(\\frac{r}{a})}]=0"
"4r^3+r^4(-\\frac{1}{a})=0 \\implies r-4a=0"
"r=4a" since "a" is the Bohr radius.
Hence, An electron has maximum probability at radius is "r=4a" .
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