$(i)$ $\begin{array}{*{20}{c}}
{\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,C{H_3}} \\
{\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,|} \\
{C{H_3} - {C^ \mathbf{-} }} \\
{\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,|} \\
{\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,C{H_3}}
\end{array}$
$(ii)\;\;CH_2 = CH -\stackrel{\mathbf{-}}{C}H_2$
$(iii)\;\;CH \equiv \stackrel{\mathbf{-}}{C}$
$(iv)\;\;\stackrel{\mathbf{-}}{C}H_3$
$(v)\;\;\stackrel{\mathbf{-}}{C}N$
$(v)$ In figure $5 , sp$ hybridised carbon is more electronegative. -ve charge on more electronegative atom makes it more stable. [ref. image]
Also, there is $-I$ effect.
$\therefore$ It is most stable.
$(iii)$ $H - C \equiv \overline{ C }$
sp hybridized carbon carry -ve charge.
$\therefore$ Hence, it is also more stable
$(ii)$ In figure $2$, resonance is taking place. [ref. image]
$\therefore$ It is more stable.
$(iv)$ $\overline{ C } H _3$
-ve charge is carried by $sp ^3$ hybridised carbon.
$\therefore$ It is less stable.
$(i)$ In figure $1$ , the central $C$ is surrounded by $CH _3$ and hence it shows $+ I$ effect from $3$ sides. [ref. image]
$\therefore$ Hence, it is least stable.
$\therefore \text { (v) }\,<\,\text { (iii) }\,<\,\text { (ii) }\,<\,\text { (iv) }\,<\,\text { (i) }$
$\begin{matrix}
\overset{\Theta }{\mathop{\overset{\centerdot \,\centerdot }{\mathop{C}}\,}}\,{{H}_{2}}-C-C{{H}_{3}} \\
|| \\
O \\
\end{matrix}$ અને $\begin{matrix}
C{{H}_{2}}=C-C{{H}_{3}} \\
| \\
:\underset{\Theta }{\mathop{\underset{\centerdot \,\centerdot }{\mathop{O}}\,}}\,: \\
\end{matrix}$
સૂચિ $I$ (એમાઈન) | સૂચિ $II$ (pK_b) |
$A$ એનિલીન | $I$ $3.25$ |
$B$ ઈથેનામાઈન | $II$ $3.00$ |
$C$ $N-$ ઈથાઈલઈથેનામાઈન | $III$ $9.38$ |
$D$ $N,N-$ ડાયઈથાઈલઈથેનામાઈન | $IV$ $3.29$ |
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