Vertical Motion with Linear Drag Derivation

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SUMMARY

The discussion focuses on the derivation of vertical motion with linear drag, specifically analyzing the equation m˙vy = mg - bvy and its implications for terminal velocity (vter). The key point is that as the projectile approaches terminal velocity, the equation transforms to m˙vy = -b(vy - vter), indicating that gravity is counteracted by drag. This derivation is specific to one-dimensional motion where gravity acts as the opposing force to drag.

PREREQUISITES
  • Understanding of Newton's second law of motion
  • Familiarity with the concept of terminal velocity
  • Basic knowledge of linear drag forces
  • Experience with differential equations in physics
NEXT STEPS
  • Study the derivation of terminal velocity in various drag scenarios
  • Learn about non-linear drag forces and their effects on motion
  • Explore the application of differential equations in classical mechanics
  • Investigate the implications of drag in multi-dimensional motion
USEFUL FOR

Students of physics, educators teaching classical mechanics, and anyone interested in the mathematical modeling of motion under drag forces.

opprobe
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I was looking through a Taylor's Classical Mechanics chapter and I have a question about the derivation.

So basically, it starts out with m\dot{v}_{y}=mg - bv_{y} and you find v_{ter} by letting m\dot{v}_{y}=0 where when you solve for v_{y} you will get v_{ter}. Now the book states how we must now discuss how the projectile approaches that speed and the formula it writes is m\dot{v}_{y} = -b(v_{y} - v_{ter}). Although I get the general idea behind it, can someone explain to me exactly what's going on?

Is this function specific to the 1D case where gravity is the counteracting force to drag?
How was he able to replace v_{y} with v_{y} - v_{ter} and exclude gravity?

Thanks!
 
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opprobe said:
I was looking through a Taylor's Classical Mechanics chapter and I have a question about the derivation.

So basically, it starts out with m\dot{v}_{y}=mg - bv_{y} and you find v_{ter} by letting m\dot{v}_{y}=0 where when you solve for v_{y} you will get v_{ter}. Now the book states how we must now discuss how the projectile approaches that speed and the formula it writes is m\dot{v}_{y} = -b(v_{y} - v_{ter}). Although I get the general idea behind it, can someone explain to me exactly what's going on?

Is this function specific to the 1D case where gravity is the counteracting force to drag?
How was he able to replace v_{y} with v_{y} - v_{ter} and exclude gravity?

Thanks!
substitute: mg = bvter ... hint: what is the terminal velocity equal to?

This equation is very specific yes, the idea is to give you an idea about derivations. Drag is not normally linear.
 
Haha. Alright - I got it thanks!
 

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