Force field
Work done along the space curve "x=2t^2, y=t, z=4t^2-t, from \\ t=0\\ to\\ t=1"
"=\\displaystyle\\int_{0}^1[3(2t^2)^2\\overrightarrow{i}+(2(2t^2)(4t^2-t)-t)\\overrightarrow{j}+(4t^2-t)\\overrightarrow{k}]\\cdot [4t\\overrightarrow{i}+1\\overrightarrow{j}+(8t-1)\\overrightarrow{k}]dt="
"=\\displaystyle\\int_{0}^1[48t^5+16t^4-4t^3-t+32t^3-4t^2-8t^2+t]dr="
"=[8t^6+{16 \\over 5}t^5+7t^4-4t^3]\\begin{matrix}\n 1 \\\\\n 0\n\\end{matrix}=8+{16 \\over 5}+7-4-0={71 \\over 5}"
Work done along the straight line "x=2t, y=t, z=3t, from \\ t=0\\ to\\ t=1"
"=\\displaystyle\\int_{0}^1[3(2t)^2\\overrightarrow{i}+(2(2t)(3t)-t)\\overrightarrow{j}+3t\\overrightarrow{k}]\\cdot [2\\overrightarrow{i}+1\\overrightarrow{j}+3\\overrightarrow{k}]dt="
"=\\displaystyle\\int_{0}^1[24t^2+12t^2-t+9t]dr="
"=[12t^3+4t^2]\\begin{matrix}\n 1 \\\\\n 0\n\\end{matrix}=12+4-0=16=\\not {71 \\over 5}"
A conservative force is a force with the property that the total work done in moving a particle between two points is independent of the taken path.
Therefore, the force is not conservative.
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