Constants in Second Order Differential Equation Solutions - A Simple Explanation

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In summary, the constants c1 and c2 appearing in the second order differential equation solutions can be any number and the equation has infinite solutions. To specify one of them, additional constraints in the form of initial conditions are needed, the number of which equals the order of the equation. In the case of f’’(t)=5f(t), the solution is f(t)=0 if the initial conditions are both set to 0, as this represents an object that is not moving. However, changing the frame of reference does not change the solution unless the initial conditions are also changed.
  • #1
luckis11
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I use the calculator
http://www.wolframalpha.com/input/?i=f’’(t)=f(t)

What are the constants c1 and c2 appearing in the second order dif. eq. solutions?
A guess of mine is that c1=f(0) and c2=f ' (0), but I am not sure.
 
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  • #2
The constants can be every number you like, and in any case you get a solution of the aquation. That is to say, the equation has infinite solutions. To specify one of them, you have to give additional constraints. These are usually the initial conditions, the values of the functions and its derivatives at a certain initial time t0. The number of initial conditions needed equals the order od the equation, that is, the higher derivative of the function that appears in the equations, and it's also the number of constants you get in the solution. In your case f(0) = c1 + c2 and f'(0) = c1 - c2.
 
  • #3
But then e.g. for case that the acceleration is analogous to the distance travelled, e.g.
f’’(t)=5f(t), where f(t)=(distance travelled), f''(t)=(acceleration),
at the wolframalfa.com solution of this dif. eq.
when replacing c1=c2=0 (because f(0)=0 and f'(0)=0)
I get the nonsense that f(t)=0.
What’s going on?
 
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  • #4
luckis11 said:
But then e.g. for case that the acceleration is analogous to the distance travelled, e.g. f’’(t)=5f(t), where f(t)=(distance travelled), f''(t)=(acceleration),
at the wolframalfa.com solution of this dif. eq.
when replacing c1=c2=0 (because f(0)=0 and f'(0)=0)
I get the nonsense that f(t)=0.
What’s going on?

What's going on is that f(t) = 0 is the unique solution to any linear homogeneous differential equation will all initial conditions being zero. Your initial conditions do not describe what you think they describe. The acceleration depends on the displacement, so if at time t = 0 the object isn't displaced there's no acceleration. The only way the object could have a non-zero displacement and hence non-zero acceleration at a later time is if at t = 0 the object was moving, but it's not by your initial condition on the velocity. What you're describing is an object that's sitting still, and you got the correct solution for that initial condition.
 
  • #5
Mute said:
The acceleration depends on the displacement, so if at time t = 0 the object isn't displaced there's no acceleration. The only way the object could have a non-zero displacement and hence non-zero acceleration at a later time is if at t = 0 the object was moving, but it's not by your initial condition on the velocity. What you're describing is an object that's sitting still, and you got the correct solution for that initial condition.

No. At the spring its motion dx is 0 at t=0, and the problem can be solved using dif.eq. just by setting that at t=0 its position is not zero, but A, i.e. just change the frame of reference. At t=0 its velocity x'(t=0) is 0.
 
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  • #6
luckis11 said:
No. At the spring its motion dx is 0 at t=0, and the problem can be solved using dif.eq. just by setting that at t=0 its position is not zero, but A, i.e. just change the frame of reference. At t=0 its velocity x'(t=0) is 0.

A differential equation + initial conditions is an initial value problem. For your differential equation, y'' - y = 0, the solution is y = c1et + c2e-2, just as given in WolframAlpha.

If the initial conditions are y(0) = 0 and y'(0) = 0, the unique solution to the DE is y [itex]\equiv[/itex] 0. The initial conditions mean that at time t = 0, the object is at the origin and its velocity is 0. If the velocity is 0, the object isn't moving, so its acceleration is 0, so the object will remain at the origin. For these initial conditions, the solution y(t) = 0 is not nonsensical.
 
  • #7
luckis11 said:
No. At the spring its motion dx is 0 at t=0, and the problem can be solved using dif.eq. just by setting that at t=0 its position is not zero, but A, i.e. just change the frame of reference. At t=0 its velocity x'(t=0) is 0.

No, the differential equation in question breaks translation invariance and so is not invariant under a change of reference frame. If you have

[tex]\ddot{x}(t) - x(t) = 0,[/tex]
with initial conditions [itex]x(0) = x_0[/itex], [itex]\dot{x}(0) = \dot{x}_0[/itex], then changing reference frame amounts to setting [itex]x(t) = X(t) + x_0[/itex], so you get the initial conditions [itex]X(0) = 0[/itex] and [itex]dX/dt(0) = \dot{x}_0[/itex], but the differential equation is now

[tex]\ddot{X}(t) - X(t) = x_0.[/tex]

This is equation is no longer homogeneous, so the unique solution is not zero unless the initial conditions are both zero.
 
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1. What are constants in second order differential equation solutions?

Constants in second order differential equation solutions are numerical values that are added to the general solution of the differential equation to account for variations in initial conditions. They are usually represented by the letters C or K.

2. Why are constants necessary in second order differential equation solutions?

Constants are necessary in second order differential equation solutions because they allow for the general solution to be adjusted to fit specific initial conditions. Without these constants, the solution would only be valid for a single set of initial conditions.

3. How do you determine the values of constants in second order differential equation solutions?

The values of constants in second order differential equation solutions can be determined by using the initial conditions provided in the problem. These conditions can be substituted into the general solution to solve for the values of the constants.

4. Can constants in second order differential equation solutions be negative?

Yes, constants in second order differential equation solutions can be negative. The values of constants are not restricted to positive numbers, and their signs are determined by the initial conditions and the form of the general solution.

5. Are constants in second order differential equation solutions always present?

No, constants in second order differential equation solutions are not always present. If the initial conditions are such that the general solution does not require any additional constants, then the solution will not contain any constants.

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