MATH 315: Fall 2024
Assignment
1
Due: Monday, September 16
Quote
of the Day
The idea that something – anything –
could be known with certainty... was delightful, intoxicating, especially when
... it opened up the possibility that other things too
might be amenable to strict, mathematical proof. Perhaps even disputes between
people might be resolved in this way. ‘I hoped,’ Russell wrote in Portraits from Memory, ‘that in time
there would be a mathematics of human behavior as precise as the mathematics of
machines.’
-
Ray Monk, Bertrand Russell The Spirit of Solitude
I. Mathematical Models.
Read
Preface and Chapter 1 of our text by this Wednesday.
Read
the excerpts from David R. Causton, A Biologist's Mathematics, London:
Edward Arnold, 1977.
Write
up solutions for Exercises 10, 12 - 16, 26, and 27 in Chapter 1 and the problem
on Vertical Motion with a Retarding Force on the next page. Although this
problem has many parts, each one only involves material from single variable
calculus and some algebraic manipulations. The link Solving
y’ = ay+ b on our course website may be useful.
For Exercise 10, you may wish to
consider some of your favorite similes or metaphors. Here are a couple of
famous ones:
“A dream deferred dries up like a
raisin in the sun” - Langston Hughes
“The righteous shall flourish like
the palm tree,
and grow mighty like a cedar in
Lebanon.
Planted in the house of the Lord,
They shall flourish in the courts of
our God.
Even in old age they shall bring
forth fruit,
They shall be full of vigor and
strength.”
-
Psalm 92
You
may also wish to comment on the confusion caused by such clumsy “mixed
metaphors” as Milking the migrant workers for all they were
worth, the supervisors barked orders at them.
Vertical Motion With a Retarding Force
Suppose we
project a ball of
mass m vertically upward from the Earth’s surface with a positive
initial velocity .
Let y(t) represent the height of the ball above the surface at
time t while v(t) represents its velocity.
Assume
that the gravitational force g is constant and that there is a retarding
force (e.g., friction, air resistance) opposite to the direction of motion and
having magnitude proportional to the velocity.
1)
Show
that in both the ascent and descent of the ball, the total force acting on the
ball at time t is
2)
Explain why Newton’s Second Law of Motion implies
3)
Solve the differential equation and show
4)
Integrate
the expression for v(t) to find y(t) as an explicit function of t.
5)
Let
t* be the time it takes the ball to ascend to its maximum height where its
velocity is 0. Show that
6)
Explain
why implies that the time of descent exceeds
the time of ascent; that is, the ball spends more time falling than rising.
7)
Find
as
an explicit function of t.
8)
Let
and show
9)
Explain
why we know x > 1.
10) Using your result from (7), show
11) Consider the function for x ≥ 1. Sketch a graph of F
and use its derivative
to
give a convincing argument that F is a strictly increasing function.
12) Explain why is positive and hence the time of ascent is less than the
time of descent.
13) (Optional Extra Credit): The assumption
that the retarding force is proportional to velocity is a reasonable one in
some situations, but fails in others. The drag on a
skydiver or parachutist is better approximated as proportional to the square of
the velocity, for example. The drag on a golf ball (because of spin) is more
accurately assumed to be proportional to
Suppose all we know about the retarding force – f(v) is that it is a
continuously differentiable function of velocity that satisfies
that
is, f(v) > 0 if v > 0 and f(v) < 0 if v
< 0.
Show that the time of ascent is less than the time of descent.