Math 31S. Rumbos Fall 2011 1 Solutions to Assignment #9 1

Math 31S. Rumbos
Fall 2011
1
Solutions to Assignment #9
1. Assume that a certain strain of E Coli bacteria in a culture has a doubling time
of about 30 minutes.
(a) Assuming a Malthusian growth model for the bacteria, give an expression,
𝑁 (𝑑), for the number of bacteria in the culture at time 𝑑, given that at
𝑑 = 0 there are π‘π‘œ bacteria in the culture.
Solution: Assuming a Malthusian growth model,
𝑁 (𝑑) = π‘π‘œ π‘’π‘Žπ‘‘ , for all 𝑑 β©Ύ 0,
(1)
where
ln 2
,
(2)
𝜏2
with 𝜏2 being the doubling time. If 𝑑 is measured in hours, then
π‘Ž=
𝜏2 =
1
hours,
2
so that, using (2),
π‘Ž = 2 ln 2 =
Λ™ 1.39,
(3)
where the dot on the equal sign in (3) indicates that the left–
hand side of (3) is a rational approximation to π‘Ž. Substituting
the approximate value for π‘Ž in (3) into (1) yields
𝑁 (𝑑) =
Λ™ π‘π‘œ 𝑒1.39𝑑 ,
(4)
where 𝑑 is measured in hours from 𝑑 = 0.
β–‘
(b) How long does it take a thousand bacteria in the culture to produce one
million?
Solution: Suppose that π‘π‘œ = 1000 in (4). We want to find 𝑑 so
that 𝑁 (𝑑) = 106 . Thus, using (4) we see that we need to solve the
equation
103 𝑒1.39𝑑 =
Λ™ 106 ,
(5)
for 𝑑. The equation in (5) is equivalent to
𝑒1.39𝑑 =
Λ™ 103 ,
Math 31S. Rumbos
Fall 2011
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which can be solved for 𝑑 by taking the natural logarithm on both
sides of the equation to yield
𝑑=
Λ™
3 ln(10)
=
Λ™ 4.97 hours,
1.38
or 4 hours and 58 minutes, or nearly 5 hours.
β–‘
2. Assume that the bacterial colony described in Problem 1 has an unlimited
supply of nutrients conducive to Malthusian growth. Assume also that the
bacteria are spherical with a diameter of 10βˆ’6 meters. Estimate the time that
it would take a single bacterium of E Coli to grow into a mega–colony to fill
R
the Earth’s oceans, seas and bays. Use the estimate given by WolframAlpha⃝
(http://www.wolframalpha.com/) of 1.332 × 1021 liters for the Earth’s oceans,
seas and bays.
Solution: We use the result in (4) with π‘π‘œ = 1 to get that
𝑁 (𝑑) =
Λ™ 𝑒1.39𝑑 ,
(6)
where 𝑑 is measured in hours from 𝑑 = 0. Assuming spherical bacteria
of radii about 10βˆ’6 meters, the volume, 𝑣1 , of one bacterium is about
(
)3
1
4
βˆ’6
× 10
cubic meters,
𝑣1 =
Λ™ πœ‹
3
2
or
𝑣1 =
Λ™ 5.24 × 10βˆ’19 cubic meters.
Using the fact that one cubic meter is equivalent to 1000 liters, we
can write the volume of one bacterium in liters as
𝑣1 =
Λ™ 5.24 × 10βˆ’16 liters.
(7)
Let 𝑁 denote the number of bacteria needed to reach a volume of
1.332 × 1021 liters, or
𝑁 𝑣1 = 1.332 × 1021 .
(8)
Combining (7) and (8) we see that
𝑁 =
Λ™
1.332 × 1021
=
Λ™ 2.54 × 1036 .
5.24 × 10βˆ’16
(9)
Math 31S. Rumbos
Fall 2011
3
According to the values predicted by the Malthusian model in (6),
the value of 𝑁 in (9) is achieved when
𝑒1.39𝑑 = 2.54 × 1036 ,
or
ln(2.54) + 36 ln(10)
=
Λ™ 60.31 hours,
1.39
or 2.51 days, or about 2 days, 12 hours and 14 minutes.
𝑑=
β–‘
3. Suppose a bacterial colony is growing according to the Malthusian model. Assume that the length of a division cycle corresponds to the doubling time. If
the time, 𝑑, is measured in units of division cycle divided by ln 2, give a formula
for 𝑁 (𝑑), given that 𝑁 (0) = π‘π‘œ . By how much does the population increase in
one unit of time?
Solution: Assume first the 𝑁 = 𝑁 (𝜏 ), where 𝜏 is measured in an
arbitrary continuous time unit. Then, the solution to the Malthus
differential equation
𝑑𝑁
= π‘Žπ‘,
π‘‘πœ
subject to 𝑁 (0) = π‘π‘œ , is given by
𝑁 (𝑑) = π‘π‘œ π‘’π‘Žπœ .
ln(2)
and so
𝜏2
)
(
)
(
𝜏
ln(2)
𝜏 = π‘π‘œ exp
.
𝑁 (𝜏 ) = π‘π‘œ exp
𝜏2
𝜏2 / ln(2)
If 𝜏2 is the doubling time, then π‘Ž =
Thus, if 𝑑 counts the number of division cycles divided by ln(2), it
𝜏
follows that 𝑑 =
; and therefore
𝜏2 / ln(2)
𝑁 (𝑑) = π‘π‘œ 𝑒𝑑 .
Thus, in one division cycle divided by ln(2), the population increases
by
𝑁 (1) βˆ’ 𝑁 (0)
π‘π‘œ 𝑒 βˆ’ π‘π‘œ
=
= 𝑒 βˆ’ 1 β‰ˆ 1.718
π‘π‘œ
π‘π‘œ
or about 172%.
β–‘
Math 31S. Rumbos
Fall 2011
4
4. Assume that the rate at which a drug leaves the bloodstream and passes into
the urine is proportional to the quantity of the drug in the blood at that time.
Let 𝑄 = 𝑄(𝑑) denote the amount of the drug in the bloodstream at time 𝑑. In
Problem 3 of Assignment 1, you applied a conservation principle to derive the
differential equation
𝑑𝑄
= βˆ’π‘˜π‘„,
(10)
𝑑𝑑
where π‘˜ is a positive constant of proportionality, and 𝑑 is measured in hours.
(a) Solve the differential equation in (10) for the case in which an initial dose
of π‘„π‘œ is injected directly into the blood at time 𝑑 = 0.
Answer: 𝑄(𝑑) = π‘„π‘œ π‘’βˆ’π‘˜π‘‘ for all 𝑑.
β–‘
(b) Assume that 20% of the initial dose is left in the blood after 3 hours. Write
a formula for computing 𝑄(𝑑) for any time 𝑑, in hours.
Solution: If 𝑄(3) = 0.20 π‘„π‘œ , then
π‘„π‘œ π‘’βˆ’3π‘˜ = 0.20 π‘„π‘œ
1
or π‘’βˆ’3π‘˜ = .
5
( )
1
1
ln 5
Thus, βˆ’π‘˜ = ln
, or π‘˜ =
. Estimating π‘˜ to two decimal
3
5
3
places we obtain that π‘˜ =
Λ™ 0.54. we then have that
𝑄(𝑑) =
Λ™ π‘„π‘œ π‘’βˆ’0.54𝑑 ,
where 𝑑 is measured in hours from the initial time 𝑑 = 0.
(11)
β–‘
(c) What percentage of the initial dosage of the drug is left in the patient’s
body after 6 hours?
Solution: After 6 hours, the amount of drug present in the patient’s blood is
𝑄(6) = π‘„π‘œ π‘’βˆ’0.54(6) =
Λ™ 0.04π‘„π‘œ ,
or 4% of the initial dose.
β–‘
5. In a one–compartment dilution experiment, a substance is found dissolved in
water in an initial amount π‘„π‘œ (in moles) in a compartment with constant volume
𝑉 . Suppose pure distilled water flows into the compartment at a constant rate
π‘Ÿ (in moles per liter) and that the well–stirred mixture is drained from the tank
Math 31S. Rumbos
Fall 2011
5
at the same rate. Suppose that in the experiment the following concentrations
of the substance were observed as a function of time:
𝑑[sec]
0
1
2
3
4
𝐢[moles/liter]
0.024
0.011
0.0048
0.0024
0.0010
If π‘„π‘œ = 0.1 mole, find the flow rate π‘Ÿ and the volume 𝑉 .
(Suggestion: Plot the natural logarithm of the concentration, ln 𝐢, versus time,
𝑑, and find the best straight line that fits the data.)
Solution: Applying the conservation principle
𝑑𝑄
= Rate of 𝑄 in βˆ’ Rate of 𝑄 out,
𝑑𝑑
with
Rate of 𝑄 in = 0,
since distilled water is flowing into the compartment, and
Rate of 𝑄 out =
𝑄
π‘Ÿ,
𝑉
we obtain that
π‘Ÿ
𝑑𝑄
= βˆ’ 𝑄.
(12)
𝑑𝑑
𝑉
Solving the differential equation in (12) subject to the initial condition
in (12) yields
( π‘Ÿ )
𝑄(𝑑) = π‘„π‘œ exp βˆ’ 𝑑 , for all 𝑑.
(13)
𝑉
Dividing the expression in (13) we obtain the following expression for
the concentration, 𝐢 = 𝐢(𝑑), of the substance in the solution,
( π‘Ÿ )
π‘„π‘œ
𝐢(𝑑) =
exp βˆ’ 𝑑 , for all 𝑑.
(14)
𝑉
𝑉
Taking the natural logarithm function on both sided of (14) yields
( )
π‘„π‘œ
π‘Ÿ
ln(𝐢) = ln
βˆ’
𝑑, for all 𝑑.
(15)
𝑉
𝑉
Math 31S. Rumbos
Fall 2011
Thus, according to (15) plotting ln(𝐢) versus
( 𝑑)should yield a straight
π‘Ÿ
π‘„π‘œ
line with slope βˆ’
and 𝑦–intercept ln
. Hence, if we want
𝑉
𝑉
to estimate π‘Ÿ and 𝑉 , in a plot of ln(𝐢) versus 𝑑, we can find the
best linear fit to the data and use the fit to get estimates for the
slope and 𝑦–intercept. Table 1 shows the values of 𝑑 and ln(𝐢), the
latter rounded up to four decimal places. Figure 1 shows a plot of the
𝑑
(sec)
0
1
2
3
4
ln(𝐢)
βˆ’3.7297
βˆ’4.5099
βˆ’5.3391
βˆ’6.0323
βˆ’6.9078
Table 1: Values of 𝑑 and ln(𝐢)
Figure 1: Linear Fit of Data in Table 1
data in Table 1 and the least–squares best fitting line obtained using
R
WolframAlpha⃝
. The equation of the best fitting line is
𝑦 = βˆ’3.72804 βˆ’ 0.78786 𝑑.
(16)
( )
π‘„π‘œ
Thus, in view of (16), we see that an estimate for ln
is
𝑉
βˆ’3.72804 so that
( )
π‘„π‘œ
ln
=
Λ™ βˆ’ 3.72804,
𝑉
6
Math 31S. Rumbos
Fall 2011
so that
π‘„π‘œ
=
Λ™ 0.0240.
(17)
𝑉
Solving for 𝑉 in (17) and using the value of 0.1 mole for π‘„π‘œ , we obtain
from (17) that
𝑉 =
Λ™ 4.17 liters.
(18)
To find π‘Ÿ, use the equation of the best–fitting line in (16) to obtain
the estimate
π‘Ÿ
=
Λ™ 0.78786.
(19)
𝑉
Thus, using the estimate for 𝑉 in (18), we obtain from (19) that
π‘Ÿ=
Λ™ 3.29 secβˆ’1 .
β–‘
7