Respuesta :
The work-energy theorem states that the change in kinetic energy of the particle is equal to the work done on the particle:
[tex]\Delta K = W[/tex]
The work done on the particle is the integral of the force on dx:
[tex]W= \int\limits^{3L}_L {F(x)} \, dx = \int\limits^{3L}_L {cx^2} \, dx = \frac{26}{3}cL^3 [/tex]
So, this corresponds to the change in kinetic energy of the particle.
[tex]\Delta K = W[/tex]
The work done on the particle is the integral of the force on dx:
[tex]W= \int\limits^{3L}_L {F(x)} \, dx = \int\limits^{3L}_L {cx^2} \, dx = \frac{26}{3}cL^3 [/tex]
So, this corresponds to the change in kinetic energy of the particle.
The change in kinetic energy during that time is : [tex]\frac{26}{3} cl^{3}[/tex]
Given data :
Direction of particle = x
Net force = F(x) = cx²
Initial position = l
Final position = 3l
Determine the change in kinetic energy during this time
we will apply the work energy theorem which is : ΔK = W
To determine change in kinetic energy we have to determine the work done on the particle.
Work done on particle ( W ) = [tex]\int\limits^3_l F({x}) \, dx[/tex] = [tex]\int\limits^3_l c{x^{2} } \, dx =[/tex] [tex]\frac{26}{3} cl^{3}[/tex]
Hence the change in kinetic energy during that time is : [tex]\frac{26}{3} cl^{3}[/tex]
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