How Do You Solve a Spring-Damper System with a Piecewise Force Function?

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Homework Help Overview

The discussion revolves around a spring-damper system described by the equation f(t) = kx(t) + c(dx/dt), where a piecewise force function is applied. Participants are tasked with determining the resulting displacement x(t) and sketching the function based on the given parameters and conditions.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants explore breaking down the force function f(t) into three segments based on time intervals and consider how to derive x(t) for each segment. There are discussions about using Laplace transforms and integration to solve the equations of motion. Questions arise regarding the continuity of x(t) at transition points and the general solution of the constraint equation.

Discussion Status

Some participants express confidence in their approach and suggest that the original poster is on the right track. There is an ongoing exploration of the general solution to the differential equation, with hints provided about the role of constants of integration and continuity conditions. Multiple interpretations of the problem are being examined without reaching a consensus.

Contextual Notes

Participants are working under the constraints of the problem statement and the initial conditions provided, while also questioning the assumptions related to the continuity of x(t) at specific time intervals.

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Homework Statement



Spring-Damper system has a force applied such that the formula f(t)= kx(t)+c(dx/dt) holds
Determine the resulting displacement x(t) and sketch the function.
What is the displacement at t=1 sec?

Homework Equations


k=10^4 Nm^-1
c=1.25x10^4 Nsm^-1
x(0)=0

the is also a graph that has time on the horizontal axis and f(t) on the vertical axis f(t). It goes up linearly from 0 to f(0.5)=100 and then linearly drops with negative gradient to 0 at f(1)=0 and then carries on at infinitely at f(t)=0 for t>1

The Attempt at a Solution



I think we have to define the graph first in three steps

0<t<0.5 f(t)=200t
0.5<t<1 f(t)=200(1-t)
t>1 f(t)=0

after this I'm confused on how to proceed. Initially I took each set of conditions and converted them to X(s) via laplace transforms then solved by partial fractions and then converted back to X(t). I'm not sure if this is the right method.

Another way would be to solve each condition by integration,
i.e. when 0<t<0.5 then f(t)=integral between 0 and 0.5 of exp^-st*200t dt
then substitute this value back into f(t) in the equation of motion.

some guidance would be nice.

thanks
 
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You broke up f(t) into three steps; can you guess an x(t) for each step that satisfies the constraint equation?
Once you've got this what is the most general solution of the constraint equation? You should be able to solve the problem now using the initial condition and continuity of x(t).

(Though I'm not sure if x(t) will satisfy the equation at .5 and 1).
 
fantispug said:
You broke up f(t) into three steps; can you guess an x(t) for each step that satisfies the constraint equation?
Once you've got this what is the most general solution of the constraint equation? You should be able to solve the problem now using the initial condition and continuity of x(t).

(Though I'm not sure if x(t) will satisfy the equation at .5 and 1).

between 0<t<0.5
i plugged in 200t=kx+c(dx/dt)
now---> 200/s^2=kX(s)+c[sX(s)-X(0)]
I re arranged in terms of X(s)=200/s^2*(k+cs)
after using partial fractions i get X(s)=-1/40s+1/50*s^2+1/40*(k/c+s)
which would give X(t)=-1/40+t/50+exp^(-k/c*t)/40

doing the same for 0.5<t<1

I get X(t)=1/200-t/250-exp^(-k/c*t)/200
i assume the third condition to be 0 as f(t)is 0 for t>1

am I going in the right direction up to now?

I didn't understand your last tip fully what do you mean by "general solution of the constraint equation"
what do I do for each x(t) equation?

many thanks
 
Yeah, it certainly looks like you're moving in the right direction. When I was talking about "general solution" I meant that a generic first order differential equation has a parameter family of solutions (i.e. you typically get a constant of integration that can be any number).Now suppose you've got an inhomogeneous linear differential equation; that is if D is some linear differential operator (here D=k+ c d/dt) and you want to solve
D X(t) = f(t) for some function f(t).
Now suppose we've got one solution X and we want to find another solution Y,
D X = f
D Y = f and so by linearity
D (Y-X) = 0. Thus any other solution is of the form X + U where D(U) = 0.

(To give you an example: Solve f'(t) = t. Well we know X(t)=t^2/2 is a solution, and any other solution is X + U, where U'(t) = 0, i.e. U = constant. So the general solution is t^2/2 + constant).

Now it looks like you've got one solution: given the above hints can you find the most general solution (i.e. the one with the arbitrary constant of integration). Continuity of X(t) at 0 and 0.5 should force a particular value of this constant of integration.
 

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