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  • Work-Energy Theorem: Block on Inclined Plane with Friction
    The work done by the horizontal force in moving the block up the inclined plane is:

    $$W = Fd\cos\theta = (75 \text{ N})(8 \text{ m})\cos37° = 466.51 \text{ J}$$

    The work done by the force of kinetic friction in opposing the motion is:

    $$W_f = -f_kd = -(25 \text{ N})(8 \text{ m}) = -200 \text{ J}$$

    The change in the kinetic energy of the block is:

    $$\Delta K = K_f - K_i = \frac{1}{2}mv_f^2 - \frac{1}{2}mv_i^2$$

    We can use the conservation of energy to relate the work done by the forces to the change in kinetic energy:

    $$W + W_f = \Delta K$$

    Substituting in the values we have calculated, we get:

    $$466.51 \text{ J} - 200 \text{ J} = \frac{1}{2}(6 \text{ kg})v_f^2 - \frac{1}{2}(6 \text{ kg})(2 \text{ m/s})^2$$

    Solving for $v_f$, we get:

    $$v_f = 5.24 \text{ m/s}$$

    Therefore, the speed of the block at the end of the 8 m displacement is 5.24 m/s.

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