SInce, (https://en.wikipedia.org/wiki/Del)
∇ ( u ⃗ ⋅ v ⃗ ) = ( u ⃗ ⋅ ∇ ) v ⃗ + ( v ⃗ ⋅ ∇ ) u ⃗ + u ⃗ × ( ∇ × v ⃗ ) + v ⃗ × ( ∇ × u ⃗ ) {\displaystyle \nabla ({\vec {u}}\cdot {\vec {v}})=({\vec {u}}\cdot \nabla ){\vec {v}}+({\vec {v}}\cdot \nabla ){\vec {u}}+{\vec {u}}\times (\nabla \times {\vec {v}})+{\vec {v}}\times (\nabla \times {\vec {u}})} ∇ ( u ⋅ v ) = ( u ⋅ ∇ ) v + ( v ⋅ ∇ ) u + u × ( ∇ × v ) + v × ( ∇ × u ) Now, put u → = v → \overrightarrow{u}=\overrightarrow{v} u = v ,we get
∇ ( v ⃗ ⋅ v ⃗ ) = ( v ⃗ ⋅ ∇ ) v ⃗ + ( v ⃗ ⋅ ∇ ) v ⃗ + v ⃗ × ( ∇ × v ⃗ ) + v ⃗ × ( ∇ × v ⃗ ) {\displaystyle \nabla ({\vec {v}}\cdot {\vec {v}})=({\vec {v}}\cdot \nabla ){\vec {v}}+({\vec {v}}\cdot \nabla ){\vec {v}}+{\vec {v}}\times (\nabla \times {\vec {v}})+{\vec {v}}\times (\nabla \times {\vec {v}})} ∇ ( v ⋅ v ) = ( v ⋅ ∇ ) v + ( v ⋅ ∇ ) v + v × ( ∇ × v ) + v × ( ∇ × v )
⟹ ∇ ( v 2 ) = 2 ( v ⃗ ⋅ ∇ ) v ⃗ + 2 v ⃗ × ( ∇ × v ⃗ ) ⟹ ( v ⃗ ⋅ ∇ ) v ⃗ = 1 2 ∇ ( v 2 ) − v ⃗ × ( ∇ × v ⃗ ) \implies {\displaystyle \nabla ( {v^2})=2({\vec {v}}\cdot \nabla ){\vec {v}}+2{\vec {v}}\times (\nabla \times {\vec {v}})}\\
\implies{ ({\vec {v}}\cdot \nabla ){\vec {v}}= \frac{1}{2}{\displaystyle \nabla ( {v^2})}-{\vec {v}}\times (\nabla \times {\vec {v}})} ⟹ ∇ ( v 2 ) = 2 ( v ⋅ ∇ ) v + 2 v × ( ∇ × v ) ⟹ ( v ⋅ ∇ ) v = 2 1 ∇ ( v 2 ) − v × ( ∇ × v )
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