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07 Pulling a Slackened Rope

Aim

To show that only a short impulse is needed to make a student move.

Subjects

Diagram

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Figure 1:.

Equipment

Presentation

The two students stand each on a cart. Between them is a slackened rope. Slowly they increase the tension in the rope and at a certain moment both carts start moving towards each other. The rope slackens again, but both carts keep on moving. (Eventually friction will stop their movement.)

When there is a clear mass difference between the two students, the difference in their respective speeds will be clearly observable.

Explanation

The tension in the rope implies an impulse FΔtF \Delta t to the cart + student. This impulse changes the momentum p=m1Δv1p=m_{1} \Delta v_{1} of the cart + student. Applying Newton’s second law we can say: FΔt=m1Δv1F \Delta t=m_{1} \Delta v_{1}. When the initial velocity is zero, then m1m_{1} will move with v1v_{1} after the short impulse is over.

Applying ‘conservation of linear momentum’ to the whole system it is clear that the change of momentum of m2m_{2} is Δp=m2Δv2-\Delta p=m_{2} \Delta v_{2}. v2v_{2} will be opposite to v1v_{1} and when m2>m1m_{2}>m_{1}, v2v_{2} will be lower than v1v_{1}.

Sources