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Question: A conservative force \[\vec F = (6.0x - 12)\hat{i}\,N\] where, \(x\) is in metres, acts on a particl...

A conservative force F=(6.0x12)i^N\vec F = (6.0x - 12)\hat{i}\,N where, xx is in metres, acts on a particle moving along an X axis. The potential energy UU associated with this force is assigned a value of 27J27J at x=0x = 0 .
(a) Write an expression for U as a function of xx ,with U in Joules and xx in metres.
(b) What is the maximum positive potential energy? At what (c) negative value and (d) positive value of xx is the potential energy equal to zero?

Explanation

Solution

In physics, when the force acts on a body and it causes a displacement in the body , it’s called body has done some work and when this work done by a force is independent of path taken, then it’s called conservative force and this conservative force is related with potential energy as F=UxF = - \dfrac{{\partial U}}{{\partial x}}.

Complete step by step answer:
(a) It’s given us that U(0)=27JU(0) = 27J and we can write F=UxF = - \dfrac{{\partial U}}{{\partial x}} as
U=0x(6x12)dx- U = \int\limits_0^x {(6x - 12)dx}
U=(3x212x)\Rightarrow - U = (3{x^2} - 12x)
U=27+12x3x2\therefore U = 27 + 12x - 3{x^2}
Hence, the function of U is U(x)=27+12x3x2U(x) = 27 + 12x - 3{x^2}

(b) To find maximum potential energy its derivative must be zero which is the given force, hence
(6.0x12)=0(6.0x - 12) = 0
x=2x = 2
Hence finding U(x)=27+12x3x2U(x) = 27 + 12x - 3{x^2} at x=2x = 2
U(2)=27+2412U(2) = 27 + 24 - 12
Umax(2)=39Joule{U_{\max }}(2) = 39Joule
Hence, maximum potential energy is Umax(2)=39Joule{U_{\max }}(2) = 39\,Joule

(c) Equating this equation U(x)=27+12x3x2U(x) = 27 + 12x - 3{x^2} to zero we get,
27+12x3x2=027 + 12x - 3{x^2} = 0
Or Taking common factor we can write
(x+1.6)(x5.6)=0(x + 1.6)(x - 5.6) = 0
Equate both factors to zero we get,
x=1.6m\therefore x = - 1.6\,m

(d) From part (c) we get, (x+1.6)(x5.6)=0(x + 1.6)(x - 5.6) = 0
x=5.6x = 5.6
Hence, x=5.6x = 5.6 is the positive value of xx at which potential energy is zero.

Note: It should be remembered that, partial derivative of potential energy is taken because force is a vector quantity and its derivative has to be taken in every component’s direction. The relation between force and potential energy can also be written in form of gradient at F=UF = - \vec \nabla U