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Question: A block of mass 1 kg, moving along x with speed $v_i = 10$ m/s enters a rough region ranging from x ...

A block of mass 1 kg, moving along x with speed vi=10v_i = 10 m/s enters a rough region ranging from x = 0.1 m to x = 1.9 m. The retarding force acting on the block in this range is Fr=kxF_r = -kx N, with k = 10 N/m. Then the final speed of the block as it crosses rough region is.

A

6 m/s

B

10 m/s

C

4 m/s

D

8 m/s

Answer

8 m/s

Explanation

Solution

Here's how to solve this problem using the work-energy theorem:

  1. Calculate the work done by the retarding force:

    The work done by a variable force is given by the integral of the force over the distance:

    W=x1x2F(x)dxW = \int_{x_1}^{x_2} F(x) \, dx

    In this case, F(x)=kx=10xF(x) = -kx = -10x N, x1=0.1x_1 = 0.1 m, and x2=1.9x_2 = 1.9 m. So,

    W=0.11.910xdx=10[x22]0.11.9=5[(1.9)2(0.1)2]=5[3.610.01]=5[3.6]=18JW = \int_{0.1}^{1.9} -10x \, dx = -10 \left[ \frac{x^2}{2} \right]_{0.1}^{1.9} = -5 \left[ (1.9)^2 - (0.1)^2 \right] = -5 [3.61 - 0.01] = -5[3.6] = -18 \, \text{J}

  2. Apply the work-energy theorem:

    The work-energy theorem states that the work done on an object is equal to the change in its kinetic energy:

    W=ΔKE=KEfKEiW = \Delta KE = KE_f - KE_i

    Where KEi=12mvi2KE_i = \frac{1}{2}mv_i^2 is the initial kinetic energy and KEf=12mvf2KE_f = \frac{1}{2}mv_f^2 is the final kinetic energy.

    We have m=1m = 1 kg, vi=10v_i = 10 m/s, and W=18W = -18 J. Thus,

    18=12(1)vf212(1)(10)2-18 = \frac{1}{2}(1)v_f^2 - \frac{1}{2}(1)(10)^2

    18=12vf250-18 = \frac{1}{2}v_f^2 - 50

    12vf2=5018=32\frac{1}{2}v_f^2 = 50 - 18 = 32

    vf2=64v_f^2 = 64

    vf=64=8m/sv_f = \sqrt{64} = 8 \, \text{m/s}

Therefore, the final speed of the block as it crosses the rough region is 8 m/s.