Solving a differential equation: f = ma, f = -kx -bv

Click For Summary
SUMMARY

The discussion focuses on solving the second-order linear homogeneous differential equation derived from Newton's second law, f = ma, and the spring-damper system equation, f = -kx - bv. The characteristic equation is established as s² + 2ζωₙs + ωₙ² = 0, where ωₙ² = k/m and 2ζωₙ = b/m. The general solution is expressed as x(t) = A e^{-ζωₙt}cos(ω_d t + φ), with the damped frequency ω_d = ωₙ√(1 - ζ²). The constants A and φ are determined by initial conditions, and understanding the characteristic equation is essential for solving such differential equations.

PREREQUISITES
  • Understanding of Newton's second law (f = ma)
  • Familiarity with second-order linear differential equations
  • Knowledge of characteristic equations and their derivation
  • Basic concepts of oscillations, including natural frequency and damping ratio
NEXT STEPS
  • Study the derivation and application of characteristic equations in differential equations
  • Learn about the Euler identity and its use in solving differential equations
  • Explore the concepts of natural frequency and damping ratio in mechanical systems
  • Practice solving second-order linear homogeneous differential equations with varying initial conditions
USEFUL FOR

Students and professionals in physics and engineering, particularly those studying mechanics, control systems, or any field involving oscillatory motion and differential equations.

DaveMan
Messages
9
Reaction score
0
so, f = ma, and f = -kx -bv.
rearrange to the form of a differential equation.
i am stuck when the next line simply states the general solution.
i have done this for first differential only, not second derivatives.
please help!
 
Physics news on Phys.org
For the homogeneous solution to ma = -kx -bv, it is standard practice to find the characteristic equation:

First, rewrite into a standard form:

\ddot{x} + \frac{b}{m}\dot{x} + \frac{k}{m}x

Set
\frac{k}{m} = \omega_n^2

\frac{b}{m} = 2\zeta\omega_n

(the reason why should be clear by the end of the problem; natural frequency and damping ration are useful, meaningful quantities in the study of oscillations)

characteristic equation:

s^2 + 2\zeta\omega_n s + \omega_n^2 = 0

find the roots of the characteristic equation (it's just a quadratic in s), s 1,2 , so that the solution to the differential equation is written:

x(t) = C_1 e^{s_1 t} + C_2 e^{s_2 t}

using the Euler identity and some algebra, you end up with the solution:

x(t) = A e^{-\zeta\omega_n t}\cos\left(\omega_d t + \phi \right)

where the damped frequency \omega_d = \omega_n \sqrt{1-\zeta^2} and the constants A and φ (magnitude and phase) are determined by the initial conditions. (You can solve it with a sine or cosine, you'll just end up with a different phase.) That's just the basics off the top of my head, but I hope that helps.
 
I don't understand how you get the charateristic equation.
 
That's usually one of the first things you learn in an introductory differential equation course.

The linear homogeneous differential equation a y"+ by'+ cy= 0 has
"characteristic equation" ar2+ br+ c= 0.


More generally, you replace the nth derivative with rn.
 

Similar threads

  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 2 ·
Replies
2
Views
4K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 7 ·
Replies
7
Views
4K