Velocity field \(\left( v \right); = ;2i; + ;\left( {x; + ;y} \right);j; + ;\left( {xyz} \right);k\)
\(Acceleration;\left( {{a_n}} \right) = \left( {\frac{{\delta v}}{{\delta t}}} \right) + \left( {u\frac{{\delta v}}{{\delta x}} + v\frac{{\delta v}}{{\delta y}} + w\frac{{\left( {\delta v} \right)}}{{\delta z}}} \right)\)
Where \(\left( {\frac{{\delta v}}{{\delta t}}} \right) \Rightarrow Local;accelaration\)
\(\left( {u\frac{{\delta v}}{{\delta x}} + v\frac{{\delta v}}{{\delta y}} + w\frac{{\left( {\delta v} \right)}}{{\delta z}}} \right) \Rightarrow Convective;accelaration;\)
Here, \(u; = ;2,;v; = ;x; + ;y,;w; = ;xyz,;t; = ;0,\) n is direction
\({a_x} = 0 + 2 \times \frac{\partial }{{\partial x}}\left( 2 \right) + \left( {x + y} \right) \times \frac{{\partial \left( 2 \right)}}{{\partial y}} + \left( {xyz} \right) \times \frac{{\partial \left( 2 \right)}}{{\partial z}}\)
ax = 0
\({a_y} = 0 + 2 \times \frac{{\partial \left( {x + y} \right)}}{{\partial x}} + \left( {x + y} \right) \times \frac{{\partial \left( {x + y} \right)}}{{\partial y}} + \left( {xyz} \right) \times \frac{{\partial \left( {x + y} \right)}}{{\partial z}}\)
ay = 2 + x + y
\({a_z} = 0 + 2 \times \frac{{\partial \left( {xyz} \right)}}{{\partial x}} + \left( {x + y} \right) \times \frac{{\partial \left( {xyz} \right)}}{{\partial y}} + xyz \times \frac{{\partial \left( {xyz} \right)}}{{\partial z}}\)
= 0 + 2yz + (x + y) × (xz) + xyz × xy
az = 2yz + (x + y) × (xz) + x2y2z
Acceleration = axi + ayj + azk
\(a; = ;0; + ;\left( {2; + ;x; + ;y} \right);j + ;\left( {2yz; + ;\left( {x + y} \right)xz; + ;{x^2}{y^2}z} \right)k\)
\({a_{\left( {1,1,2} \right)}}; = ;0; + ;\left( {2; + ;1; + ;1} \right)j + ;\left( {2; \times ;1; \times ;2; + \left( {1; + ;1} \right) \times 1; \times ;2; + ;{1^2}; \times ;{1^2} \times ;2} \right)k\)
\(\therefore a; = ;4j; + ;\left( {4; + ;4; + ;2} \right)k; = ;4j; + ;10k\)