1.08k, 1.08l - Separable differential equations and their solutions
Find general and particular solutions of first-order differential equations by direct integration or separation of variables. You will keep constant solutions, select valid branches and interpret rates, limits and restrictions in a motion model.
Solutions and initial information
Can a falling object keep speeding up without ever reaching ? A supplied model gives its downward velocity by , starting from rest. At , its acceleration is ; at , it is ; at , it is only , all in . Solving the equation will tell us whether the speed reaches and when it reaches halfway.
You already know
Integration reverses differentiation. An indefinite integral needs an arbitrary constant. The chain rule differentiates a composite function, and for .
A solution must satisfy the rate rule throughout its interval, not merely pass through one point.
General and particular solutions
A solution is a differentiable function satisfying the differential equation. A general solution contains an arbitrary constant describing a family of solutions. An initial condition, such as , can select a particular solution. For example, every solves , but only gives .
If the derivative depends only on the independent variable, integrate directly. This solution method is not in the formula sheet: learn it.
Worked example 1: a point selects a curve
Question. Solve , given .
Plan. Integrate with a constant, then substitute both coordinates of the initial point.
Why this step? The given ordinate is , but the other terms at contribute , so is not .
Answer. , for real .
Check. Differentiating gives , and .
Change only the input of the initial point from to . The derivative stays the same, so the curves differ only by a vertical translation.
Worked example 2: a different initial input
Question. Solve , given .
Plan. Use the same general solution and fit its constant to the new point.
Why this step? A point condition selects the member of the family; it does not change the differential equation.
Answer. .
Check. The derivative is still , and .
A domain can split a family into separate intervals. For , direct integration gives . The equation is undefined at , so a condition at selects an interval on the right, never a solution passing through the pole.
Watch out
Wrong: take the initial ordinate as without substitution. Right: substitute the entire point into the integrated equation. Then check both the derivative and the point condition.
Move the initial input once more in the next problem.
Separating variables before integration
When the right-hand side involves both variables, first look for a product of a function of and a function of . Factorisation may be the step that reveals it.
Separation of variables
If
then, where , separate and integrate:
Check constant solutions from separately, and restrict the solution to an interval where the equation is defined.
Not in the formula sheet: learn it.
The notation is backed by the chain rule: differentiating the left integral with respect to produces . It is not permission to treat a varying as constant in an integral with respect to .
Worked example 3: factor before separating
Question. Solve , given .
Plan. Factor out , separate the variables, then use the initial condition after integrating.
Why this step? Exponentiating converts an additive logarithmic constant into a multiplicative constant. The positive initial value selects a positive branch.
Answer. , for real . The constant solution , excluded during division, does not meet this initial condition.
Check. Differentiation gives , and .
Change only the dependent-variable factor from to . Separate the whole factor; the quantity inside the logarithm changes with it.
Worked example 4: a shifted dependent variable
Question. Solve , given .
Plan. Factor into , then integrate the reciprocal of .
Why this step? The common factor is , so dividing by would not separate the equation.
Answer. , for real . The separate equilibrium fails the initial condition.
Check. , and .
The same calculation solves proportional decay. For , , separation gives , then . Its derivative is negative, but its magnitude decreases as the positive quantity gets smaller. These exponential solutions are derived here; they are not printed in the formula sheet.
Watch out
Wrong: after . Right: . A real signed includes the branch sign; check in the equation before including it.
For the next shifted equation, change the scale of the right-hand side and the initial value. Show the separation rather than only writing a remembered exponential.
Recovering equilibria and choosing a valid branch
Division can erase a perfectly good constant solution. Record the zero factors first, and use the initial value to choose the relevant branch afterwards.
Equilibrium solution
An equilibrium solution is a constant function satisfying the differential equation. For , both and have derivative zero and make the right-hand side zero. A constant such as is not an equilibrium: its derivative is zero but the right-hand side is .
Partial fractions from your earlier integration work handle a product of two linear factors. Keep the minus sign from integrating .
Worked example 5: keep both constant solutions
Question. Identify the equilibria of , then solve with .
Plan. Check the zero factors, separate the nonconstant solutions and use partial fractions.
Why this step? Division excluded both equilibria. The logarithmic relation describes only the other solutions, so it cannot by itself be the complete answer about equilibria.
Answer. The equilibria are and . The particular solution is , for real .
Check. With , , and . Also .
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