- A$\left[ NiCl _4\right]^{2-}$
- B$\left[ CoCl _6\right]^{3-}$
- C$\left[ CoF _6\right]^{3-}$
- ✓$\left[ Co \left( NH _3\right)_6\right]^{3+}$
(2) Paramagnetic, High Spin and Octahedral
(3) Paramagnetic, High Spin and Octahedral
(4) Diamagnetic, Low Spin and Octahedral
$\left[ Co \left( NH _3\right)_6\right]^{3+}, CN =6(\text { Octahedral })$
$NH _3= SFL$
$Co ^{+3}=[ Ar ] 3 d ^6$
Diamagnetic and Low spin complex
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$Mg^{2+} + 2{e^ - } \to Mg(s)\;E^o = - 2.37\,V$
$Cu^{2+} + 2e^- \to Cu(s)\;E^o = + 0.34\,V$

$H _2( g )+\frac{1}{2} O _2( g ) \rightarrow H _2 O (\ell)$
The work derived from the cell on the consumption of $1.0 \times 10^{-3} mol$ of $H _2( g )$ is used to compress $1.00 mol$ of a monoatomic ideal gas in a thermally insulted container. What is the change in the temperature (in $K$ ) of the ideal gas ?
The standard reduction potentials for the two half-cells are given below.
$\left. O _2( g )+4 H ^{+} \text {(aq. }\right)+4 e ^{-} \rightarrow 2 H _2 O (\ell), E ^{\circ}=1.23 V,$
$\left.2 H ^{+} \text {(aq. }\right)+2 e ^{-} \rightarrow H _2( g ), E ^{\circ}=0.00 V.$
Use $F =96500 C mol ^{-1}, R =8.314 J mol ^{-1} K ^{-1}$