Net force on a Swinging Pendulum

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SUMMARY

The discussion focuses on the net force acting on a weight tied to a string spinning in a horizontal circle, emphasizing Newton's third law of motion. It clarifies that while the force exerted by the string on the weight is equal and opposite to the force exerted by the weight on the string, these forces act on different objects and do not cancel each other out. The inward net force results in radial acceleration, as the direction of the weight changes while its speed remains constant. The conversation also notes that complexities arise when additional forces are applied during the motion.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Basic knowledge of circular motion dynamics
  • Familiarity with concepts of force and acceleration
  • Comprehension of vector forces and their interactions
NEXT STEPS
  • Study the implications of Newton's third law in different physical scenarios
  • Explore the principles of centripetal force in circular motion
  • Learn about the effects of additional forces on pendulum motion
  • Investigate the role of tension in flexible strings during circular motion
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Physics students, educators, and anyone interested in understanding the dynamics of circular motion and the application of Newton's laws in real-world scenarios.

Conservation
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Hello everyone,

Consider a weight tied to a string spinning in a horizontal circle.

According to Newton's third law, the force of the string on the weight (inward) is opposite and equal to the force of the weight on the string (outward).

If this is the case, how can there be a net acceleration inward?

Thanks.
 
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The forces in a third law pair act on different objects, so you don't sum them to get a net force.
 
Conservation said:
how can there be a net acceleration inward?
Because the sum of all forces on the weight is inward.
 
Conservation said:
Hello everyone,

Consider a weight tied to a string spinning in a horizontal circle.

According to Newton's third law, the force of the string on the weight (inward) is opposite and equal to the force of the weight on the string (outward).

If this is the case, how can there be a net acceleration inward?

Thanks.

The speed of the mass in a tangential direction does not change but the direction does. That means the only force is inwards towards the centre. That makes the acceleration radial as well.
This only applies if there is no extra forces applied at the time - the string is just going around under its own steam. But a totally flexible string can only transmit a force along its length so getting it up to speed, you need to be moving your hand round in a circle; things get more complicated then.
 

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