Differential Equations Notes
Differential Equations
9.1 Modeling with Differential Equations
A mathematical model often takes the form of a differential equation, which contains an unknown function and some of its derivatives.
Models of Population Growth
A population growth model assumes the population grows at a rate proportional to its size, which is reasonable for bacteria or animals under ideal conditions.
Variables:
= time (independent variable)
= number of individuals in the population (dependent variable)
The rate of growth of the population is the derivative .
The assumption that the growth rate is proportional to population size can be written as: , where k is the proportionality constant.
This is a differential equation because it contains an unknown function and its derivative .
If k > 0, then \frac{dP}{dt} > 0 for all , meaning the population is always increasing.
As increases, becomes larger, so the growth rate increases as the population increases.
A solution to the equation is an exponential function of the form .
Taking the derivative:
The family of solutions is .
Since populations have only positive values, we are interested in solutions with C > 0 and t > 0.
When , , so is the initial population, .
A more realistic model must account for limited resources, where the population levels off when it approaches its carrying capacity .
Assumptions for a refined model:
If is small, the growth rate is proportional to .
If P > M, then decreases if it ever exceeds .
A simple expression incorporating both assumptions is:
If is small compared with , then is close to 0, so .
If P > M, then is negative, so \frac{dP}{dt} < 0.
The equation is called the logistic differential equation.
The constant functions and are solutions because one of the factors on the right side of the equation is zero; these are equilibrium solutions.
If the initial population lies between 0 and , then \frac{dP}{dt} > 0 and the population increases.
If the population exceeds the carrying capacity (P > M), then is negative, so \frac{dP}{dt} < 0 and the population decreases.
If the population approaches the carrying capacity (), then , which means the population levels off.
A Model for the Motion of a Spring
Consider the motion of an object with mass at the end of a vertical spring.
Hooke’s Law: If the spring is stretched (or compressed) units from its natural length, then it exerts a force that is proportional to : restoring force , where is a positive constant (the spring constant).
Ignoring external resisting forces, by Newton’s Second Law (force equals mass times acceleration), we have .
This is a second-order differential equation because it involves second derivatives.
The equation can be rewritten as: , which means the second derivative of is proportional to but has the opposite sign.
General Differential Equations
A differential equation is an equation that contains an unknown function and one or more of its derivatives.
The order of a differential equation is the order of the highest derivative that occurs in the equation.
and are first-order equations.
is a second-order equation.
The independent variable (e.g., ) doesn’t always have to represent time.
For example, in the differential equation , is an unknown function of .
A function is a solution of a differential equation if the equation is satisfied when and its derivatives are substituted into the equation.
is a solution of if for all values of in some interval.
To solve a differential equation means to find all possible solutions of the equation.
We have already solved simple differential equations of the form .
The general solution of is , where is an arbitrary constant.
Example 1
Show that every member of the family of functions is a solution of the differential equation .
Solution
Using the Quotient Rule to differentiate :
The right side of the differential equation becomes:
Therefore, for every value of , the given function is a solution of the differential equation.
When applying differential equations, we are usually interested in finding a particular solution that satisfies an additional requirement, rather than a family of solutions (the general solution).
In many physical problems, we need to find the particular solution that satisfies a condition of the form .
This is called an initial condition, and the problem of finding a solution of the differential equation that satisfies the initial condition is called an initial-value problem.