Callahan
7.2: 2, 4, 5, 7, 9, 10, 18, 26, 27
7.3: 10, 18 (Use Euler's Method)
![[Graphics:Images/springwk2_gr_1.gif]](Images/springwk2_gr_1.gif)
2) Determine the period and frequency of the following functions:
a)
:
To find the period we set the term inside the sine or cosine function equal to
(the natural period these functions) and solve for the variable:
![[Graphics:Images/springwk2_gr_4.gif]](Images/springwk2_gr_4.gif)
![[Graphics:Images/springwk2_gr_5.gif]](Images/springwk2_gr_5.gif)
We know that the frequency equals
, so:
![[Graphics:Images/springwk2_gr_7.gif]](Images/springwk2_gr_7.gif)
And:
![[Graphics:Images/springwk2_gr_8.gif]](Images/springwk2_gr_8.gif)
![[Graphics:Images/springwk2_gr_9.gif]](Images/springwk2_gr_9.gif)
![[Graphics:Images/springwk2_gr_10.gif]](Images/springwk2_gr_10.gif)
If we graph sums of periodic functions we see that if the function with the longer period has period that is a integer multiple of the function with the shorter period then the longer period is the period of the overall function:
![[Graphics:Images/springwk2_gr_11.gif]](Images/springwk2_gr_11.gif)
![[Graphics:Images/springwk2_gr_12.gif]](Images/springwk2_gr_12.gif)
![[Graphics:Images/springwk2_gr_13.gif]](Images/springwk2_gr_13.gif)
![]()
![[Graphics:Images/springwk2_gr_15.gif]](Images/springwk2_gr_15.gif)
b)
:
![[Graphics:Images/springwk2_gr_17.gif]](Images/springwk2_gr_17.gif)
![[Graphics:Images/springwk2_gr_18.gif]](Images/springwk2_gr_18.gif)
![[Graphics:Images/springwk2_gr_19.gif]](Images/springwk2_gr_19.gif)
And:
![[Graphics:Images/springwk2_gr_20.gif]](Images/springwk2_gr_20.gif)
![[Graphics:Images/springwk2_gr_21.gif]](Images/springwk2_gr_21.gif)
![[Graphics:Images/springwk2_gr_22.gif]](Images/springwk2_gr_22.gif)
In this case we can't just use the period of the function with the longest period, rather we need to find out what the smallest integer multiple of one period is that equals an integer multiple of the other period:
![[Graphics:Images/springwk2_gr_23.gif]](Images/springwk2_gr_23.gif)
![[Graphics:Images/springwk2_gr_24.gif]](Images/springwk2_gr_24.gif)
![[Graphics:Images/springwk2_gr_25.gif]](Images/springwk2_gr_25.gif)
So our period is:
![[Graphics:Images/springwk2_gr_26.gif]](Images/springwk2_gr_26.gif)
![[Graphics:Images/springwk2_gr_27.gif]](Images/springwk2_gr_27.gif)
![]()
![[Graphics:Images/springwk2_gr_29.gif]](Images/springwk2_gr_29.gif)
c)
:
![[Graphics:Images/springwk2_gr_31.gif]](Images/springwk2_gr_31.gif)
![[Graphics:Images/springwk2_gr_32.gif]](Images/springwk2_gr_32.gif)
![[Graphics:Images/springwk2_gr_33.gif]](Images/springwk2_gr_33.gif)
And:
![[Graphics:Images/springwk2_gr_34.gif]](Images/springwk2_gr_34.gif)
![[Graphics:Images/springwk2_gr_35.gif]](Images/springwk2_gr_35.gif)
![[Graphics:Images/springwk2_gr_36.gif]](Images/springwk2_gr_36.gif)
And:
![[Graphics:Images/springwk2_gr_37.gif]](Images/springwk2_gr_37.gif)
![[Graphics:Images/springwk2_gr_38.gif]](Images/springwk2_gr_38.gif)
![[Graphics:Images/springwk2_gr_39.gif]](Images/springwk2_gr_39.gif)
![[Graphics:Images/springwk2_gr_40.gif]](Images/springwk2_gr_40.gif)
![]()
![[Graphics:Images/springwk2_gr_42.gif]](Images/springwk2_gr_42.gif)
![[Graphics:Images/springwk2_gr_43.gif]](Images/springwk2_gr_43.gif)
*4)
a) What are the amplitude and frequency of
?
![[Graphics:Images/springwk2_gr_45.gif]](Images/springwk2_gr_45.gif)
![[Graphics:Images/springwk2_gr_46.gif]](Images/springwk2_gr_46.gif)
![[Graphics:Images/springwk2_gr_47.gif]](Images/springwk2_gr_47.gif)
![[Graphics:Images/springwk2_gr_48.gif]](Images/springwk2_gr_48.gif)
![[Graphics:Images/springwk2_gr_49.gif]](Images/springwk2_gr_49.gif)
b) What are the amplitude and frequency of
?
![[Graphics:Images/springwk2_gr_51.gif]](Images/springwk2_gr_51.gif)
![[Graphics:Images/springwk2_gr_52.gif]](Images/springwk2_gr_52.gif)
![[Graphics:Images/springwk2_gr_53.gif]](Images/springwk2_gr_53.gif)
![[Graphics:Images/springwk2_gr_54.gif]](Images/springwk2_gr_54.gif)
![[Graphics:Images/springwk2_gr_55.gif]](Images/springwk2_gr_55.gif)
![[Graphics:Images/springwk2_gr_56.gif]](Images/springwk2_gr_56.gif)
![[Graphics:Images/springwk2_gr_57.gif]](Images/springwk2_gr_57.gif)
![[Graphics:Images/springwk2_gr_58.gif]](Images/springwk2_gr_58.gif)
![[Graphics:Images/springwk2_gr_59.gif]](Images/springwk2_gr_59.gif)
5)
a) Is the antiderivative
periodic?
![[Graphics:Images/springwk2_gr_61.gif]](Images/springwk2_gr_61.gif)
![[Graphics:Images/springwk2_gr_62.gif]](Images/springwk2_gr_62.gif)
![[Graphics:Images/springwk2_gr_63.gif]](Images/springwk2_gr_63.gif)
![[Graphics:Images/springwk2_gr_64.gif]](Images/springwk2_gr_64.gif)
So it is periodic:
![[Graphics:Images/springwk2_gr_65.gif]](Images/springwk2_gr_65.gif)
![[Graphics:Images/springwk2_gr_66.gif]](Images/springwk2_gr_66.gif)
![[Graphics:Images/springwk2_gr_67.gif]](Images/springwk2_gr_67.gif)
b) If so what are its amplitude and frequency?
![[Graphics:Images/springwk2_gr_68.gif]](Images/springwk2_gr_68.gif)
![[Graphics:Images/springwk2_gr_69.gif]](Images/springwk2_gr_69.gif)
![[Graphics:Images/springwk2_gr_70.gif]](Images/springwk2_gr_70.gif)
7)
a) What is the average value of the function
over the interval
?
From p.351 we have the average value of an arbitrary function is given by:
![[Graphics:Images/springwk2_gr_73.gif]](Images/springwk2_gr_73.gif)
So:
![[Graphics:Images/springwk2_gr_74.gif]](Images/springwk2_gr_74.gif)
![[Graphics:Images/springwk2_gr_75.gif]](Images/springwk2_gr_75.gif)
So the average value of the function
over the interval
is
.
![[Graphics:Images/springwk2_gr_79.gif]](Images/springwk2_gr_79.gif)
b) What is the average value of the function
over the interval
?
![[Graphics:Images/springwk2_gr_82.gif]](Images/springwk2_gr_82.gif)
![[Graphics:Images/springwk2_gr_83.gif]](Images/springwk2_gr_83.gif)
![[Graphics:Images/springwk2_gr_84.gif]](Images/springwk2_gr_84.gif)
c) What is the average value of the function
over the interval
?
![[Graphics:Images/springwk2_gr_87.gif]](Images/springwk2_gr_87.gif)
![[Graphics:Images/springwk2_gr_88.gif]](Images/springwk2_gr_88.gif)
![[Graphics:Images/springwk2_gr_89.gif]](Images/springwk2_gr_89.gif)
d) What is the average value of the function
over the interval
for any real number
?
![[Graphics:Images/springwk2_gr_93.gif]](Images/springwk2_gr_93.gif)
![[Graphics:Images/springwk2_gr_94.gif]](Images/springwk2_gr_94.gif)
e) Your work should demonstrate that the average value of
over the full period does not depend on the point
where you begin the period. Is the same true for the average value over the half period?
So yes the average value of
over the full period does not depend on the point
.
However the average value over a half period varies over the range
because the function lacks symmetry over the half period.-
![[Graphics:Images/springwk2_gr_100.gif]](Images/springwk2_gr_100.gif)
*9) The function
and
have the same amplitude and frequency; they differ only in phase. In other words,
![[Graphics:Images/springwk2_gr_103.gif]](Images/springwk2_gr_103.gif)
for an appropriately chosen phase difference
. What is
?
Since the phase difference
is a constant we can choose any convenient value of
and find
:
![[Graphics:Images/springwk2_gr_109.gif]](Images/springwk2_gr_109.gif)
But since both functions are
periodic:
![[Graphics:Images/springwk2_gr_111.gif]](Images/springwk2_gr_111.gif)
![[Graphics:Images/springwk2_gr_112.gif]](Images/springwk2_gr_112.gif)
10) The function
and
also differ only in phase. What is
?
![[Graphics:Images/springwk2_gr_116.gif]](Images/springwk2_gr_116.gif)
Since the phase difference
is a constant we can choose any convenient value of
and find
:
![[Graphics:Images/springwk2_gr_120.gif]](Images/springwk2_gr_120.gif)
But since both functions are
periodic:
![[Graphics:Images/springwk2_gr_122.gif]](Images/springwk2_gr_122.gif)
![[Graphics:Images/springwk2_gr_123.gif]](Images/springwk2_gr_123.gif)
![[Graphics:Images/springwk2_gr_124.gif]](Images/springwk2_gr_124.gif)
18)
a) Let
. Using a graphical utility, sketch the graph of
.
![]()
![[Graphics:Images/springwk2_gr_128.gif]](Images/springwk2_gr_128.gif)
a) The function
is periodic. What is its period? Estimate the amplitude from the graph:
![[Graphics:Images/springwk2_gr_130.gif]](Images/springwk2_gr_130.gif)
![[Graphics:Images/springwk2_gr_131.gif]](Images/springwk2_gr_131.gif)
c) In fact,
can be viewed as a "phase-shifted" sine function:
![[Graphics:Images/springwk2_gr_133.gif]](Images/springwk2_gr_133.gif)
From your graph, estimate the phase difference
and the amplitude
.
![[Graphics:Images/springwk2_gr_136.gif]](Images/springwk2_gr_136.gif)
To find the phase difference
we solve for a value of
where
:
![[Graphics:Images/springwk2_gr_140.gif]](Images/springwk2_gr_140.gif)
![[Graphics:Images/springwk2_gr_141.gif]](Images/springwk2_gr_141.gif)
So we have:
![[Graphics:Images/springwk2_gr_142.gif]](Images/springwk2_gr_142.gif)
![[Graphics:Images/springwk2_gr_143.gif]](Images/springwk2_gr_143.gif)
*26) The function whose graph is sketched at the left has the form:
![[Graphics:Images/springwk2_gr_144.gif]](Images/springwk2_gr_144.gif)
Determine the values of
,
,
, and
.
First lets find
using the peak-to-peak amplitude:
![[Graphics:Images/springwk2_gr_150.gif]](Images/springwk2_gr_150.gif)
![[Graphics:Images/springwk2_gr_151.gif]](Images/springwk2_gr_151.gif)
Second lets find
using the
:
![[Graphics:Images/springwk2_gr_154.gif]](Images/springwk2_gr_154.gif)
Third lets find
using the period given in the graph:
![[Graphics:Images/springwk2_gr_156.gif]](Images/springwk2_gr_156.gif)
So because
when
we have:
![[Graphics:Images/springwk2_gr_159.gif]](Images/springwk2_gr_159.gif)
![[Graphics:Images/springwk2_gr_160.gif]](Images/springwk2_gr_160.gif)
Last, lets find
using the fact that
normally passes through the origin. We can see that if the graph were not vertically shifted
, it would just be a sine shifted
of its period to the right. So in order to be shifted to the right the expression inside the sine term must equal zero at the point
. This fact allows us to determine the value of
:
![[Graphics:Images/springwk2_gr_167.gif]](Images/springwk2_gr_167.gif)
![[Graphics:Images/springwk2_gr_168.gif]](Images/springwk2_gr_168.gif)
So our overall equation is:
![[Graphics:Images/springwk2_gr_169.gif]](Images/springwk2_gr_169.gif)
![]()
![[Graphics:Images/springwk2_gr_171.gif]](Images/springwk2_gr_171.gif)
![[Graphics:Images/springwk2_gr_172.gif]](Images/springwk2_gr_172.gif)
27) Write equations for three different functions all having amplitude 4 and period 5, whose graphs pass through the point
:
![[Graphics:Images/springwk2_gr_174.gif]](Images/springwk2_gr_174.gif)
To make the amplitude and period correct we set
and
, and because
when
:
![[Graphics:Images/springwk2_gr_179.gif]](Images/springwk2_gr_179.gif)
![[Graphics:Images/springwk2_gr_180.gif]](Images/springwk2_gr_180.gif)
To make a point on this curve pass through the point
we adjust
and
appropriately. To start with, lets just translate the point
on the sine curve to the point
:
![[Graphics:Images/springwk2_gr_186.gif]](Images/springwk2_gr_186.gif)
![[Graphics:Images/springwk2_gr_187.gif]](Images/springwk2_gr_187.gif)
So we have:
![[Graphics:Images/springwk2_gr_188.gif]](Images/springwk2_gr_188.gif)
![[Graphics:Images/springwk2_gr_189.gif]](Images/springwk2_gr_189.gif)
![[Graphics:Images/springwk2_gr_190.gif]](Images/springwk2_gr_190.gif)
![[Graphics:Images/springwk2_gr_191.gif]](Images/springwk2_gr_191.gif)
![[Graphics:Images/springwk2_gr_192.gif]](Images/springwk2_gr_192.gif)
![[Graphics:Images/springwk2_gr_193.gif]](Images/springwk2_gr_193.gif)
And the general form is:
![[Graphics:Images/springwk2_gr_194.gif]](Images/springwk2_gr_194.gif)
![[Graphics:Images/springwk2_gr_195.gif]](Images/springwk2_gr_195.gif)
7.3: 10, 18 (use Euler's method to estimate the answers)
![[Graphics:Images/springwk2_gr_196.gif]](Images/springwk2_gr_196.gif)
10) Nonlinear Spring: (p386)
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![[Graphics:Images/springwk2_gr_201.gif]](Images/springwk2_gr_201.gif)
![[Graphics:Images/springwk2_gr_202.gif]](Images/springwk2_gr_202.gif)
![[Graphics:Images/springwk2_gr_203.gif]](Images/springwk2_gr_203.gif)
![[Graphics:Images/springwk2_gr_204.gif]](Images/springwk2_gr_204.gif)
a) Suppose the acceleration
of the weight on a hard spring depends on the displacement
of the weight according to the formula
. If you pull the weight down
, hold it motionless, and then release it, what will its frequency be?
![[Graphics:Images/springwk2_gr_209.gif]](Images/springwk2_gr_209.gif)
![[Graphics:Images/springwk2_gr_210.gif]](Images/springwk2_gr_210.gif)
![[Graphics:Images/springwk2_gr_211.gif]](Images/springwk2_gr_211.gif)
![[Graphics:Images/springwk2_gr_212.gif]](Images/springwk2_gr_212.gif)
![[Graphics:Images/springwk2_gr_213.gif]](Images/springwk2_gr_213.gif)
b) How far must you pull the weight so that its frequency will be double the frequency in part (a)?
![[Graphics:Images/springwk2_gr_214.gif]](Images/springwk2_gr_214.gif)
![[Graphics:Images/springwk2_gr_215.gif]](Images/springwk2_gr_215.gif)
![[Graphics:Images/springwk2_gr_216.gif]](Images/springwk2_gr_216.gif)
![[Graphics:Images/springwk2_gr_217.gif]](Images/springwk2_gr_217.gif)
![[Graphics:Images/springwk2_gr_218.gif]](Images/springwk2_gr_218.gif)
from visual.graph import *
graph = gdisplay()
tinitial = 0
tfinal = 6
t = tinitial
x = 2
v = 0
numberofsteps = 10000
deltat = (tfinal - tinitial) / float(numberofsteps)
vcurve = gcurve()
xcurve = gcurve()
for k in range(numberofsteps):
vprime = -16*x-(x**3)
xprime = v
deltav = vprime * deltat
deltax = xprime * deltat
t = t + deltat
v = v + deltav
x = x + deltax
vcurve.plot(pos=(t,v))
xcurve.plot(pos=(t,x))
![[Graphics:Images/springwk2_gr_219.gif]](Images/springwk2_gr_219.gif)
*18) The Pendulum: (p392)
|
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Take
and give the pendulum three different initial impulses:
![[Graphics:Images/springwk2_gr_225.gif]](Images/springwk2_gr_225.gif)
Using Euler's method to determine the period of the motion in each case. Are the periods noticeably different?
![[Graphics:Images/springwk2_gr_226.gif]](Images/springwk2_gr_226.gif)
The periods are not noticeably different, however the amplitude is:
|
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![[Graphics:Images/springwk2_gr_228.gif]](Images/springwk2_gr_228.gif)
from visual.graph import *
graph = gdisplay()
for i in [0.05, 0.1, 0.2]:
tinitial = 0
tfinal = 7
t = tinitial
x = 0
v = i
numberofsteps = 10000
deltat = (tfinal - tinitial) / float(numberofsteps)
xcurve = gcurve()
xcurve.plot(pos=(t,x))
for k in range(numberofsteps):
vprime = -sin(x)
xprime = v
deltav = vprime * deltat
deltax = xprime * deltat
t = t + deltat
v = v + deltav
x = x + deltax
xcurve.plot(pos=(t,x))