Second-order first-degree autonomous differential equation: Difference between revisions

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Definition

Following the convention for autonomous differential equations, we denote the dependent variable by x and the independent variable by t.

Form of the differential equation

A (one-dimensional and degree one) second-order autonomous differential equation is a differential equation of the form:

d2xdt2=F(x,dxdt)

Solution method and formula

We set a variable v=dx/dt Then, we can rewrite dt=(dx)/v. In particular, d2x/dt2=(d/dt)(dx/dt)=dv/dt=dv/((dx)/v)=vdv/dx. Plug this in:

vdvdx=F(x,v)

Solve this to obtain the general solution for v in terms of x. Plug this expression in:

dxdt=v(x)

and solve this first-order differential equation. Note that if v is not expressible as an explicit function of x, but we instead have a relational solution R(x,v)=0, then solve the first-order differential equation:

R(x,dxdt)=0

Particular cases

Case where the function on the right depends only on x and not on dx/dt

Consider a situation of the form:

d2xdt2=g(x)

We do the same substitution v=dx/dt and obtain:

vdvdx=g(x)

This is now a separable differential equation relating x and v. Integrate and obtain:

vdv=g(x)dx

We thus get:

v22=g(x)dx

In particular, if G is an antiderivative for g, then we get:

v=±2G(x)+C1

where C1R is a parameter. Each choice of C1 gives a different solution.

Plug this back in and get:

dxdt=±2G(x)+C1

(The ± indicates that there are in fact two differential equations and we need to take the union of their solution sets).

This is a first-order autonomous differential equation, and in particular a separable differential equation. Rearrange and get:

±dx2G(x)+C1=dt

An additional constant, C2, arises from this indefinite integration. The upshot is that the general solution relates x to t and has two parameters C1,C2, as we might expect from the degree of the equation.

Case where the function on the right is multiplicatively separable

Consider a situation of the form:

d2xdt2=g(x)h(dxdt)

We do the same substitution v=dx/dt and obtain:

vdvdx=g(x)h(v)

This is a separable differential equation and we can rearrange it to obtain:

vdvh(v)=g(x)dx

We now perform the integration both sides. Suppose H(v)=vdvh(v) and G(x)=g(x)dx. We get:

H(v)=G(x)+C1

If H can locally be inverted, we can write v as an explicit function of x We now plug this into the original differential equation and get:

H(dx/dt)=G(x)+C1

This is now a first-order differential equation. If H can locally be inverted, we can write dx/dt as an explicit function of x (locally) and then solve the resultant separable differential equation. Otherwise, there may be some other method available.