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In an experiment, one of the forces exerted on a proton is F⃗ =−αx2i^, where α=12N/m2. What is the potential-energy function for F⃗ ? Let U=0 when x=0. Express your answer in terms of α and x.

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Answer


\Delta U= \alpha (x^3)/(3) \\

Step-by-step explanation:

given


F = -\alpha x^2 i

where
\alpha = 12 N/m^2

now we know


\int\limits^W_0 {} \, dW = \int\limits^a_b {F.} \, dxi ..................(i)

where dx is infinitesimal distance


W = \int\limits^a_b {-\alpha x^2} \, dx \\

for x = a and b = 0

after integration we get


W = -\alpha (x^3)/(3)

we know work done by conservative force will be equals to negative of potential energy


W = -\Delta U

so we get


-\Delta U= -\alpha (x^3)/(3) \\\\\Delta U= \alpha (x^3)/(3) \\

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