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A force-time graph is given. Calculate the impulse applied to an object and its change in momentum. The graph shows a force of 5 N applied from 0-3s (triangular), 3-5s (rectangular), and 5-8s (triangu

Physics

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Answer

A\text{A}

Step-by-step solution

3 steps

To solve this problem, we need to use the impulse-momentum theorem, which states that the impulse applied to an object is equal to the change in its momentum. The impulse is the area under the force-time (F-t) graph.

The formula for impulse is:

Impulse=Δp=m(vf−vi)\text{Impulse} = \Delta p = m(v_f - v_i)

where Δp\Delta p is the impulse, mm is the mass, vfv_f is the final velocity, and viv_i is the initial velocity.

  1. Calculate the total impulse from the F-t graph.

    The graph can be divided into three geometric shapes:

    • Area 1 (0 s to 3 s): A triangle. Area1=12×base×height=12×(3 s−0 s)×5 N=12×3 s×5 N=7.5 N⋅s\text{Area}_1 = \frac{1}{2} \times \text{base} \times \text{height} = \frac{1}{2} \times (3 \text{ s} - 0 \text{ s}) \times 5 \text{ N} = \frac{1}{2} \times 3 \text{ s} \times 5 \text{ N} = 7.5 \text{ N}\cdot\text{s}
    • Area 2 (3 s to 5 s): A rectangle. Area2=width×height=(5 s−3 s)×5 N=2 s×5 N=10 N⋅s\text{Area}_2 = \text{width} \times \text{height} = (5 \text{ s} - 3 \text{ s}) \times 5 \text{ N} = 2 \text{ s} \times 5 \text{ N} = 10 \text{ N}\cdot\text{s}
    • Area 3 (5 s to 8 s): A triangle. Area3=12×base×height=12×(8 s−5 s)×5 N=12×3 s×5 N=7.5 N⋅s\text{Area}_3 = \frac{1}{2} \times \text{base} \times \text{height} = \frac{1}{2} \times (8 \text{ s} - 5 \text{ s}) \times 5 \text{ N} = \frac{1}{2} \times 3 \text{ s} \times 5 \text{ N} = 7.5 \text{ N}\cdot\text{s}

    The total impulse is the sum of these areas:

    Total Impulse=Area1+Area2+Area3=7.5 N⋅s+10 N⋅s+7.5 N⋅s=25 N⋅s\text{Total Impulse} = \text{Area}_1 + \text{Area}_2 + \text{Area}_3 = 7.5 \text{ N}\cdot\text{s} + 10 \text{ N}\cdot\text{s} + 7.5 \text{ N}\cdot\text{s} = 25 \text{ N}\cdot\text{s}

    The mass of the particle is given as m=5 kgm = 5 \text{ kg}.

  2. Calculate the final velocity if the particle is initially at rest.

    Given vi=0 m/sv_i = 0 \text{ m/s}.
    Using the impulse-momentum theorem:

    Impulse=m(vf−vi)\text{Impulse} = m(v_f - v_i) 25 N⋅s=5 kg×(vf−0 m/s)25 \text{ N}\cdot\text{s} = 5 \text{ kg} \times (v_f - 0 \text{ m/s}) 25=5vf25 = 5 v_f vf=255=5 m/sv_f = \frac{25}{5} = 5 \text{ m/s}
  3. Calculate the final velocity if the particle is initially with a velocity of −4 m/s-4 \text{ m/s}.

    Given vi=−4 m/sv_i = -4 \text{ m/s}.
    Using the impulse-momentum theorem:

    Impulse=m(vf−vi)\text{Impulse} = m(v_f - v_i) 25 N⋅s=5 kg×(vf−(−4 m/s))25 \text{ N}\cdot\text{s} = 5 \text{ kg} \times (v_f - (-4 \text{ m/s})) 25=5(vf+4)25 = 5 (v_f + 4)

    Divide both sides by 5:

    5=vf+45 = v_f + 4 vf=5−4=1 m/sv_f = 5 - 4 = 1 \text{ m/s}

    The final velocities are 5 m/s5 \text{ m/s} when initially at rest, and 1 m/s1 \text{ m/s} when initially at −4 m/s-4 \text{ m/s}.

    Comparing these results with the given options, option A matches.

    The final answer is A\text{A}.

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