Debate over the experimental procedure for Newton's 2nd Law

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Discussion Overview

The discussion revolves around the experimental procedure for demonstrating Newton's Second Law using a cart and weights on a pulley system. Participants debate the correct methodology for measuring acceleration and the implications of mass considerations in the setup.

Discussion Character

  • Debate/contested
  • Experimental/applied
  • Mathematical reasoning

Main Points Raised

  • One participant argues that the total mass should include both the cart and the weights, suggesting that weights should be added by removing mass from the cart to keep the total mass constant.
  • Another participant supports this view, stating that if the mass of the weights is small compared to the cart, it may only be a minor correction, but extreme cases should be considered.
  • Some participants present a mathematical expression for acceleration, indicating that keeping the total mass fixed leads to a proportional relationship with the mass on the string.
  • There is a counter-argument regarding the analogy of people pulling a car, with some asserting that if the people are accelerating, their masses must be included in the calculations.
  • A participant expresses uncertainty about the experimental setup, indicating a lack of clarity without a visual aid.
  • Another participant suggests that if the constant mass protocol is followed, the entire mass should be considered in the acceleration measurement, and they propose a method for plotting results to validate this approach.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the correct methodology for the experiment. Multiple competing views remain regarding the treatment of mass in the context of Newton's Second Law.

Contextual Notes

Some participants note the absence of a figure to clarify the experimental setup, which may contribute to misunderstandings. There are also references to friction and other factors that could influence the results, but these remain unresolved.

ekrabappel
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Hi,

I'm currently having an ongoing debate with some teachers regarding a practical for Newton's Second Law. The prac involves a cart attached to some weights via a string on a pulley. The protocol as it stands has students add increasing mass to the end of the string (not changing the mass of the cart) while measuring the time it takes for the cart to travel a certain distance. The students run the experiment with several different masses and calculate the cart acceleration using time and distance. They then plot the mass at the end of the string against acceleration. The slope is the mass of the cart thus supporting Newton's second Law. I have been arguing that the cart and weight at the end of the string should be used as a total mass and weight should be added to the string by removing it from the cart thus keeping the total mass constant. The calculated mass from the slope is the mass of the entire setup. This has been counter argued that if you had 2 people pulling a car along the road with a rope and you added a third person then you wouldn't take the mass of the people pulling the rope into consideration. Who is right here?
 
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You are right.
ekrabappel said:
I have been arguing that the cart and weight at the end of the string should be used as a total mass and weight should be added to the string by removing it from the cart thus keeping the total mass constant.
That would be better, yes.

If the mass of the weights is small compared to the mass of the car it is only a small correction, but you can consider extreme cases: Use an elephant as weight. Will the acceleration depend on the mass of the cart? Not measurably, the elephant will just fall down freely. If you use two elephants as weight you get the same acceleration.

People pulling on a rope is different because the people don't move - there is no force involved in accelerating these people.
 
ekrabappel said:
Summary: Correct method for Newton's 2nd Law experiment

Who is right here?
If you work out the math for this problem you get $$a=g\frac{m_{\text{string}}}{m_{\text{string}}+m_{\text{car}}}$$

So if you keep the total mass fixed then the denominator is a constant and the acceleration is proportional to the mass on the string. If you keep the car mass fixed you shouldn’t get a straight line (of course with friction it probably doesn’t matter anyway)

ekrabappel said:
Summary: Correct method for Newton's 2nd Law experiment

This has been counter argued that if you had 2 people pulling a car along the road with a rope and you added a third person then you wouldn't take the mass of the people pulling the rope into consideration.
This scenario is simple enough to analyze directly. No need to make imperfect analogies with other scenarios.
 
ekrabappel said:
This has been counter argued that if you had 2 people pulling a car along the road with a rope and you added a third person then you wouldn't take the mass of the people pulling the rope into consideration.
If the people themselves are accelerating at the same rate as the car, then you would have to include their masses to get the acceleration from the total external force at their feet. Otherwise the scenario/question is not equivalent.
 
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Dale said:
If you work out the math for this problem you get $$a=g\frac{m_{\text{string}}}{m_{\text{string}}+m_{\text{car}}}$$
I am not sure I have understood the setup 100% (unfortunately for me no figure provided) but from what I understand I think the acceleration of the system is $$a=g\frac{m_{string}-m_{car}}{m_{string}+m_{car}}$$

EDIT: OK i think i see my mistake now, the car is supported on a horizontal surface...o:)
 
Delta2 said:
unfortunately for me no figure provided
I agree. A figure is always helpful for this sort of thing.
 
If you design the experiment following the constant mass protocol (moving mass from the end of the string to the cart) suggested by @Dale in post #3, you can write$$m_{string}g=Ma$$where ##M## is the constant combined mass ##m_{string}+m_{cart}##. This equation shows that even though the Earth exerts an unbalanced force on only part of the two-mass system, it's the entire mass ##M## that has the measured acceleration ##a##. Should you choose to go this way, I would suggest that ##m_{string}## not be used as an independent variable. Consider plotting the two sides of the equation on the same graph versus run number. Then see whether the points overlap to within the error bars for each run. This should persuade your detractors that they are using the wrong analogy. It's the Earth that does the "pulling" and, of course, its mass is not included anywhere.

BTW, if you want only the mass of the cart to be your system, then you will need to measure the tension independently, perhaps with a force gauge, and plot measured tension versus measured acceleration. Under ideal conditions, the slope will be the mass of the cart.
 
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