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At t = 0 a 4.0 kg object is passing the origin, moving right with an initial speed of 1.0 m/s. Consider the following two cases: Case A: A force F(x) = (1.0N/m) x to the right acts on the object for 4.0 m. Case B: A force F(t) = (1.0 N/s) t to the right acts on the object for 4.0 s. What is the change in kinetic energy for the object?

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Answer:

Case A:

Work-energy theorem states that the total work done on an object is equal to the change in the kinetic energy of the object.


W_(total) = \int{F(x)} \, dx = \int\limits^4_0 {x} \, dx = (x^2)/(2)\left \{ {{x = 4} \atop {x=0}} \right. = (16 - 0)/(2) = 8~J

Case B:

In this case, we cannot calculate the total work done by
W = \int{F(t)} \, dx, because the force is a function of time, not position.

So, we need to calculate the initial and final kinetic energies.


K_1 = (1)/(2)mv^2 = (1)/(2)4(1^2) = 2~J

For the final kinetic energy, we need to find the final velocity. What we have is the force as a function of time. From Newton’s Second Law we can find the acceleration as a function time:


a(t) = F(t)/m = ((1.0 N/s)t)/(4) = (t)/(4)~m/s^2


v(t) = \int{a(t)} \, dt = \int{(1)/(4)t} \, dt = (t^2)/(8)

From this function, at t = 4.0 s, v = 2 m/s.


K_2 = (1)/(2)mv_2^2 = (1)/(2)4(2^2) = 8~J

So, the change in the kinetic energy is


\Delta K = K_2 - K_1 = 8 - 2 = 6~J

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