First order non-linear differential equation

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SUMMARY

The discussion focuses on solving a first-order non-linear differential equation related to a particle of mass m accelerating under Galilean gravity with a non-linear resistive force represented by -μvv. The equation of motion is derived from Newton's second law, resulting in mv' = -gz - μvv. The participant struggles with the integration process, particularly with respect to the velocity vector and the inclusion of the vertical unit vector z, leading to confusion about the validity of their solution involving arctan. The consensus emphasizes the importance of solving the equation as a whole rather than separating it into vector components.

PREREQUISITES
  • Understanding of first-order non-linear differential equations
  • Familiarity with Newton's second law of motion
  • Knowledge of vector calculus and integration techniques
  • Concept of resistive forces in physics, specifically quadratic resistance
NEXT STEPS
  • Study methods for solving non-linear ordinary differential equations (ODEs)
  • Learn about the application of separation of variables in vector contexts
  • Research the effects of quadratic resistance on motion in multiple dimensions
  • Explore numerical methods for approximating solutions to complex ODEs
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Students in physics and engineering, particularly those studying dynamics and differential equations, as well as educators seeking to clarify concepts related to non-linear motion and resistive forces.

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Homework Statement


Hello, I was given an extension problem in a Dynamics lecture today and am struggling to solve it.

It is a simple scenario: a particle of mass m is accelerating due to Galilean gravity, but is subject to a resistive force that is non-linear in the velocity of the particle. This is in the usual Cartesian coordinate system, where z is the unit vector pointing vertically.

I will use bold font to denote vectors, and let v' = dv/dt [not the usual notation, but I do not know how else to easily show derivatives on forums].
Also, v is the speed of the particle, magnitude of velocity v.

Homework Equations



The resistive force is given by : -μvv

Where μ is a constant.

From N II : mv' = -gz - μvv

The Attempt at a Solution



I'm unsure on how to solve this non-linear ODE. My attempt at a solution via separation of variables the equation ended up with a solution involving arctan. However, I was confused about the idea of integrating with respect to v, the vector, particularly when we have z involved - so this solution may be completely invalid. We were told not to split up the differential equation into components of the vectors, but instead to solve completely through as the problem was given.

Any help would be appreciated, thanks.
 
Last edited:
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In the case of quadratic resistance and an arbritary motion of the body in the plane (e.g not constrained to move horizontally or vertically), then the equations of motion for the velocity in the x and y direction do not decouple.

If you separated variables, did you consider the motion to occur in one direction?
 

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