Differential Equations Homework Assignment 2 for Math 308 - Fall 2002, Assignments of Differential Equations

A homework assignment for math 308 - differential equations, due on september 20, 2002. It includes five differential equations and their corresponding slope fields, and asks students to match the equations with the slope fields, sketch the functions for given initial conditions, and analyze the behavior of the solutions for various friction models. The document also provides some background information on differential equations and their applications.

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Math 308 - Differential Equations Fall 2002
Homework Assignment 2
Due Friday, September 20.
1. On the last page of this assignment are five differential equations for u(t), and five slope fields. Match
the equation with the slope field.
2. In each of the slope fields in Problem 1, sketch the function u(t) for which u(0) = 1.
3. Consider an object falling through a viscous medium. According to Newton’s second law of motion,
the motion of an object is governed by the equation F=ma, where Fis the total force acting on the
object, mis the mass of the object, and ais the acceleration of the object. If we let y(t) be the height
of the object, then v(t) = dy
dt is the velocity, and a(t) = dv
dt =d2y
dt2is the acceleration. Note that with
this choice of y, a positive velocity (v > 0) means the object is moving up.
The forces acting on the object are gravity (a constant force given by mg, where gis the acceleration
due to gravity), and friction. The frictional force depends on how fast the object is moving, and is
always directed in the opposite direction of the motion. Let Fd(v) be the force due to friction (the d
subscript refers to drag).
(a) Write down the differential equation satisfied by v, the velocity of the object. Assume that g > 0
(so you must be sure to put the correct sign in the equation), and that when v > 0, Fd(v)<0.
If the object is released from height y0when t= 0, what is the initial condition for the differential
equation?
(b) Consider no friction, so Fd(v) = 0. Solve the initial value problem for v(t). What happens to v
at tincreases? That is, what is the long-term behavior of v?
(c) Suppose the friction force is proportional to the velocity. That is, let Fd(v) = Cdv, where
Cd>0 is a constant (the drag coefficient). Solve the initial value problem. What happens to v
as tincreases?
(d) Now suppose that the friction force is proportional to the square of the velocity: let Fd(v) =
Cdv|v|. Solve the new problem, and describe the long-term behavior.
Note that v|v|=(v2v0
v2v0. I’ve written it this way to ensure that the friction force always
opposes the velocity.
Also, observe that for any non-zero constant a,
1
v2a2=1
(v+a)(va)=1
2a(v+a)+1
2a(va).
This is an example of a partial fraction expansion. It can be useful when you try to integrate the
separated equation.
(e) If yis measured in meters, tin seconds, and mass in kilograms, what must the units of Cdbe in
the previous two questions? (Note: the units are not the same in the two cases.)
4. The logistic equation
dP
dt =kµ1P
NP
is a first order autonomous differential equation, so it is separable. Find the general solution to this
differential equation.
1
pf3

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Math 308 - Differential Equations Fall 2002

Homework Assignment 2

Due Friday, September 20.

  1. On the last page of this assignment are five differential equations for u(t), and five slope fields. Match the equation with the slope field.
  2. In each of the slope fields in Problem 1, sketch the function u(t) for which u(0) = 1.
  3. Consider an object falling through a viscous medium. According to Newton’s second law of motion, the motion of an object is governed by the equation F = ma, where F is the total force acting on the object, m is the mass of the object, and a is the acceleration of the object. If we let y(t) be the height of the object, then v(t) = dydt is the velocity, and a(t) = dvdt = d

(^2) y dt^2 is the acceleration. Note that with this choice of y, a positive velocity (v > 0) means the object is moving up. The forces acting on the object are gravity (a constant force given by mg, where g is the acceleration due to gravity), and friction. The frictional force depends on how fast the object is moving, and is always directed in the opposite direction of the motion. Let Fd(v) be the force due to friction (the d subscript refers to drag).

(a) Write down the differential equation satisfied by v, the velocity of the object. Assume that g > 0 (so you must be sure to put the correct sign in the equation), and that when v > 0, Fd(v) < 0. If the object is released from height y 0 when t = 0, what is the initial condition for the differential equation? (b) Consider no friction, so Fd(v) = 0. Solve the initial value problem for v(t). What happens to v at t increases? That is, what is the long-term behavior of v? (c) Suppose the friction force is proportional to the velocity. That is, let Fd(v) = −Cdv, where Cd > 0 is a constant (the drag coefficient). Solve the initial value problem. What happens to v as t increases? (d) Now suppose that the friction force is proportional to the square of the velocity: let Fd(v) = −Cdv|v|. Solve the new problem, and describe the long-term behavior.

Note that v|v| =

v^2 v ≥ 0 −v^2 v ≤ 0

. I’ve written it this way to ensure that the friction force always

opposes the velocity. Also, observe that for any non-zero constant a, 1 v^2 − a^2

(v + a)(v − a)

2 a(v + a)

2 a(v − a)

This is an example of a partial fraction expansion. It can be useful when you try to integrate the separated equation. (e) If y is measured in meters, t in seconds, and mass in kilograms, what must the units of Cd be in the previous two questions? (Note: the units are not the same in the two cases.)

  1. The logistic equation dP dt = k

P

N

P

is a first order autonomous differential equation, so it is separable. Find the general solution to this differential equation.

Note: To integrate the separated equation, the following may be helpful:

1 ( 1 − PN

P

N − P

P

This is another example of a partial fraction expansion.

  1. We consider again the clearance of a drug from a patient’s blood. Suppose a(t) is the amount of a drug in the bloodstream, measured in milligrams. We assume that the drug “clears” at a rate that is proportional to the amount present, and we take the proportionality constant to be 0.2 per hour. Suppose that the patient is being given the drug intravenously. The drug is dissolved in a solution with a concentration of 1.4 milligrams per liter, and this solution enters the bloodstream continuously at the rate of 0.1 liters per hour.^1 The body regulates the volume of the blood so that the total volume of blood remains 5 liters. Assume that when the patient first starts receiving the drug, there is no drug already in the blood.

(a) Give the initial value problem for a(t) that models this situation. (b) Solve the initial value problem. (c) What is the amount of the drug in the bloodstream after one hour? After one day? After a “long time”? (In other words, what is limt→∞ a(t)?)

Text Problems:

  • Section 1.4/ 2, 5, 6, 10, 11

(^1) This is not meant to be a realistic flow rate for the intravenous administration of a drug.