Explanation of proportionality with falling objects.

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SUMMARY

The discussion centers on the physics of falling objects, specifically the forces acting on them, including gravitational force and air resistance. Two equations are presented: (1) mg - kv = ma, which describes linear air resistance, and (2) mg - kv² = ma, applicable at high velocities. The air resistance is explained as being proportional to velocity for small speeds and to the square of velocity for larger speeds, based on phenomenological laws. The conversation highlights the importance of Taylor series expansion in approximating functions and the underlying physics of drag forces.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with Taylor series expansion
  • Basic knowledge of fluid dynamics and air resistance
  • Concept of drag force in physics
NEXT STEPS
  • Study the derivation of Newton's laws of motion
  • Learn about the principles of fluid dynamics and drag coefficients
  • Explore the application of Taylor series in physics
  • Investigate the effects of viscosity on falling objects
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Physics students, educators, and anyone interested in understanding the dynamics of falling objects and the forces acting upon them, particularly in the context of air resistance and fluid mechanics.

zeralda21
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A falling object with no initial velocity with mass m is influenced by a gravitational force g and the air resistance which is proportional to the object´s speed. By Newton´s laws this can be written as:

(1) mg-kv=ma or (2) mg-kv^2=ma (for large velocities).

I assume that k is a positive constant that depends on the geometry of the object and the viscosity. But how can one explain that the air resistance is proportional to the velocity? And to the velocity squared in the second equation?
 
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I think those are phenomenological laws. I mean, they are ansatz forms for the air resistance which aren't based on detailed physics, but rather generic expressions with adjustable parameters to give it flexibility to fit the experiment. We can expect the air resistance to increase monotonically with velocity, but not necessarily linear.

We can approximate many (analytic) functions as linear for small input using a Taylor series expansion. For small enough input, assuming 0 constant term, the linear term (if non-zero) will dominate. This is the basis of a great many laws like Hooke's law or Ohm's law, which don't really have a derivation from fundamental physics. For large input values, the higher order terms will tend to dominate over the linear.

In the case of wind, by symmetry, I expect the squared term to be zero, and the first non-linear term to be velocity cubed.
 
There are two effects at play, both pretty well grounded in basic physics concepts.

One effect is from simple collisions between the object and the air molecules. This results in a force proportional to v2.

The linear-in-v term is due to the tendency of the object to drag the air along with it, and the viscosity of the air.
 

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