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