Author Archives: Engineering Math

College Physics by Openstax Chapter 2 Problem 39


In 1967, New Zealander Burt Munro set the world record for an Indian motorcycle, on the Bonneville Salt Flats in Utah, of 183.58 mi/h. The one-way course was 5.00 mi long. Acceleration rates are often described by the time it takes to reach 60.0 mi/h from rest. If this time was 4.00 s, and Burt accelerated at this rate until he reached his maximum speed, how long did it take Burt to complete the course?


Solution:

There are two parts to the race: an acceleration part and a constant speed part.

For the acceleration part:

We are given the following values: v_0=0 \ \text{mph} ; v_f=60 \ \text{mph}; and \Delta t=4.00 \ \text{s} .

First, we need to determine how long (both in distance and time) it takes the motorcycle to finish accelerating. During acceleration, the value of the acceleration is given by

a=\frac{60\:\text{mph}}{4\:\text{s}}

To compute for the time it takes to reach its maximum velocity, we are going to use the formula

v_f=v_0+at

Solving for time t in terms of the other variables

t=\frac{v_f-v_0}{a}

Substituting the given values to solve for t_1, the time it takes to accelerate from rest to maximum velocity:

\begin{align*}
t_1 & =\frac{v_f-v_0}{a} \\
t_1 & =\frac{183\:\text{mph}-0\:\text{mph}}{\left(\frac{60\:\text{mph}}{4\:\text{s}}\right)} \\
t_1 & =12.2\:\text{s}
\end{align*}

Since we have a constant acceleration, the distance traveled \Delta x_1 during this period is computed using the formula

\begin{align*}
\Delta x_1 & =v_{ave}t \\
\Delta x_1 & =\left(\frac{v_f+v_0}{2}\right)t \\
\end{align*}

Substituting the given values:

\begin{align*}
\Delta x_1 & =\left(\frac{v_f+v_0}{2}\right)t \\
\Delta x_1 & =\left(\frac{183\:\text{mph}+0\:\text{mph}}{2}\right)\left(12.2\:\text{s}\right) \\
\Delta x_1 & =\left(91.5\:\text{mph}\right)\left(\frac{1\:\text{hr}}{3600\:\text{s}}\right)\left(12.2\:\text{s}\right) \\
\Delta x_1 & =0.31\:\text{mi}
\end{align*}

For the constant speed part:

For the next part of the motion, the speed is constant.

We are given the following values: \Delta x_2=5.0\:\text{mi}-0.3\:\text{mi}=4.7\:\text{mi} .

We are going to solve t_2, the time spent on the course at max speed using the formula

\Delta x_2=v_{max}t_2

Solving for t_2 in terms of the other variables:

t_2=\frac{\Delta x_2}{v_{max}}

Substituting the given values:

\begin{align*}
t_2 & =\frac{\Delta x_2}{v_{max}} \\
t_2  & =\frac{4.7\:\text{mi}}{183\:\text{mph}} \\
t_2  & =\left(0.026\:\text{h}\right)\left(\frac{3600\:\text{s}}{1\:\text{h}}\right) \\
t_2  &=92\:\text{s}
\end{align*}

For the whole course:

So, the total time is

\begin{align*}
t_{total}&=t_1+t_2 \\
t_{total}& =12.2\:\text{s}+\:92\:\text{s} \\
t_{total}& =104\:\text{s} \ \qquad \ \color{DarkOrange} \left( \text{Answer} \right)

\end{align*}

Advertisements
Advertisements

Differential and Integral Calculus by Feliciano and Uy, Exercise 1.3, Problem 3

Advertisements

PROBLEM:

Evaluate  \displaystyle \lim\limits_{x\to 3}\left(\frac{x^3-13x+12}{x^3-14x+15}\right).


Advertisements

SOLUTION:

A straight substitution of x=3 leads to the indeterminate form \frac{0}{0} which is meaningless.

Therefore, to evaluate the limit of the given function, we proceed as follows.

\begin{align*}

\lim\limits_{x\to 3}\left(\frac{x^3-13x+12}{x^3-14x+15}\right)& =\lim\limits_{x\to 3}\left(\frac{\left(x-3\right)\left(x^2+3x-4\right)}{\left(x-3\right)\left(x^2+3x-5\right)}\right)\\
\\
& =\lim\limits_{x\to 3}\left(\frac{x^2+3x-4}{x^2+3x-5}\right)\\
\\
&=\frac{\left(3\right)^2+3\left(3\right)-4}{\left(3\right)^2+3\left(3\right)-5}\\
\\
& =\frac{9+9-4}{9+9-5}\\
\\
& =\frac{14}{13} \ \qquad \ \color{DarkOrange} \left( \text{Answer} \right)\\
\\
\end{align*}

Advertisements
Advertisements

Differential and Integral Calculus by Feliciano and Uy, Exercise 1.3, Problem 2

Advertisements

PROBLEM:

Evaluate \displaystyle \lim\limits_{x\to 2}\left(\frac{x^2+2x-8}{3x-6}\right)


Advertisements

SOLUTION:

A straight substitution of x=2 leads to the indeterminate form \frac{0}{0}  which is meaningless.

Therefore, to evaluate the limit of the given function, we proceed as follows

\begin{align*}

\lim\limits_{x\to 2}\left(\frac{x^2+2x-8}{3x-6}\right)& =\lim\limits_{x\to 2}\left(\frac{\left(x+4\right)\left(x-2\right)}{3\left(x-2\right)}\right)\\
\\
&=\lim\limits_{x\to 2}\left(\frac{x+4}{3}\right)\\
\\
&=\frac{2+4}{3}\\
\\
&=\frac{6}{3}\\
\\
& =2 \ \qquad \ \color{DarkOrange} \left( \text{Answer} \right)\\
\\
\end{align*}

Advertisements
Advertisements

College Physics by Openstax Chapter 2 Problem 38


A bicycle racer sprints at the end of a race to clinch a victory. The racer has an initial velocity of 11.5 m/s and accelerates at the rate of 0.500 m/s2 for 7.00 s.

(a) What is his final velocity?

(b) The racer continues at this velocity to the finish line. If he was 300 m from the finish line when he started to accelerate, how much time did he save?

(c) One other racer was 5.00 m ahead when the winner started to accelerate, but he was unable to accelerate, and traveled at 11.8 m/s until the finish line. How far ahead of him (in meters and in seconds) did the winner finish?


Solution:

We are given the following: v_0=11.5 \ \text{m/s} ; a=0.500 \ \text{m/s}^2; and \Delta t=7.00 \ \text{s}.

Part A

To solve for the final velocity, we are going to use the formula

v_f=v_0+at

Substituting the given values:

\begin{align*}
v_f &=v_0+at\\
v_f&=11.5\ \text{m/s}+\left( 0.500\ \text{m/s}^2 \right)\left( 7.00\ \text{s} \right)\\
v_f&=15.0\ \text{m/s} \ \qquad \ \color{DarkOrange} \left( \text{Answer} \right)

\end{align*}

Part B

Let  t_{const} be the time it takes to reach the finish line without accelerating:

\begin{align*}
t_{const}&=\frac{x}{v_0}\\
t_{const}&=\frac{300\ \text{m}}{11.5\ \text{m/s}}\\
t_{const}&=26.1\ \text{m/s}
\end{align*}

Now let d be the distance traveled during the 7 seconds of acceleration. We know t=7.00 \ \text{s} so

\begin{align*}
d&=v_0t+\frac{1}{2}at^2\\
d&=\left( 11.5\ \text{m/s} \right)\left( 7.00\ \text{s} \right)+\frac{1}{2}\left( 0.500\ \text{m/s} ^2\right)\left( 7.00\ \text{s} \right)^2\\
d&=92.8\ \text{m}
\end{align*}

Let t' be the time it will take the rider at the constant final velocity to complete the race:

\begin{align*}
t'&=\frac{x-d}{v}\\
t'&=\frac{300\ \text{m}-92.8\ \text{m}}{15.0\ \text{m/s}}\\
t'&=13.8\ \text{s}
\end{align*}

So the total time T it will take the accelerating rider to reach the finish line is 

\begin{align*}
T&=t+t'\\
T&=7.00\ \text{s}+13.8\ \text{s}\\
T&=20.8\ \text{s}
\end{align*}

Finally, let T^{*} be the time saved. So 

\begin{align*}
T^{*}&=26.1\ \text{s}-20.8\ \text{s}\\
T^{*}&={\color{DarkGreen} 5.3\ \text{s}} \ \qquad \ \color{DarkOrange} \left( \text{Answer} \right)

\end{align*}

Part C

For rider 2, we are given the following values: \Delta x'=295 \ \text{m} ; v'=11.8 \ \text{m/s}

Let  t_2 be the time it takes for rider 2 to reach the finish line.

We are going to use the formula

t_2=\frac{\Delta x'}{v'}

Substituting the given values:

\begin{align*}
t_2 & =\frac{x'}{v'} \\
t_2 & =\frac{295\:\text{m}}{11.8\:\text{m/s}} \\
t_2 & =25.0\:\text{s}
\end{align*}

The time difference is

\begin{align*}
\text{time difference} & =t_2-T \\
\text{time difference} & =25.0\:\text{s}-20.817\:\text{s} \\
\text{time difference} & =4.2\:\text{s} \ \qquad \ \color{DarkOrange} \left( \text{Answer} \right)

\end{align*}

Therefore, he finishes 4.2 s after the winner.

When the other racer reaches the finish line, he has been traveling at 11.8 m/s for 4.2 seconds, so the other racer finishes

\begin{align*}
\Delta x & =\left(11.8\:\text{m/s}\right)\left(4.2\:\text{s}\right) \\
\Delta x & =49.56\:\text{m} \ \qquad \ \color{DarkOrange} \left( \text{Answer} \right)

\end{align*}

behind the other racer.


Advertisements
Advertisements

Successive Wins: Challenging Problem in Probability


To encourage Elmer’s promising tennis career, his father offers him a prize if he wins (at least) two tennis sets in a row in a three-set series to be played with his father and the club champion alternately: father-champion-father or champion-father-champion, according to Elmer’s choice. The champion is a better player than Elmer’s father. Which series should Elmer choose?


Solution:

Since the champion plays better than the father, it seems reasonable that fewer sets should be played with the champion. On the other hand, the middle set is the key one, because Elmer cannot have two wins in a row without winning the middle one. Let C stand for the champion, F for father, and W and L for win and loss by Elmer. Let f be the probability of Elmer’s winning any set from his father, c the corresponding probability of winning from the champion. The table shows only possible prize-winning sequences together with their probabilities, given independence between sets, for the two choices.

Set with:

Father First

FCFProbability
WWWfcf
WWLfc(1-f)
LWW(1-f)cf
Totalfc(2-f)

Champion First

CFCProbability
WWWcfc
WWLcf(1-c)
LWW(1-c)fc
Totalfc(2-c)

Since Elmer is more likely to best his father than to beat the champion, f is larger than c, and 2-f is smaller than 2-c, and so Elmer should choose CFC. For example, for f=0.8, c=0.4, the chance of winning the prize with FCF is 0.384, that for CFC is 0.512. Thus, the importance of winning the middle game outweighs the disadvantage of playing the champion twice.

Many of us have a tendency to suppose that the higher the expected number of successes, the higher the probability of winning a prize, and often this supposition is useful. But occasionally a problem has special conditions that destroy this reasoning by analogy. In our problem, the expected number of wins under CFC is 2c+f, which is less than the expected number of wins for FCF, 2f+c. In our example with f=0.8 and c=0.4, these means are 1.6 and 2.0 in that order. This opposition of answers gives the problem flavor.


Advertisements
Advertisements

The Sock Drawer: Challenging Problem in Probability


A drawer contains red socks and black socks. When two socks are drawn at random, the probability that both are red is 1/2.

a) How small can the number of socks in the drawer be?

b) How small if the number of black socks is even?


Solution:

Just to set the pattern, let us do a numerical example first. Suppose there were 5 red and 2 black socks; then the probability of the first sock’s being red would be 5/(5+2). If the first were red, the probability of the second’s being red would be 4/(4+2), because one red sock has already been removed. The product of these two numbers is the probability that both socks are red:

\frac{5}{5+2}\times \frac{4}{4+2}=\frac{5\left( 4 \right)}{7\left( 6 \right)}=\frac{10}{21}

This result is close to 1/2, but we need exactly 1/2. Now let us go at the problem algebraically.

Let there be r red and b black socks. The probability of the first sock’s being red is \frac{r}{r+b}; and if the first sock is red, the probability of the second’s being red now that a red has been removed is \frac{r-1}{r+b-1}. Then we require the probability that both are red to be \frac{1}{2}, or

\frac{r}{r+b}\times \frac{\:r-1}{r+b-1}=\frac{1}{2}

One could just start with b=1 and try successive values of r, then go to b=2 and try again, and so on. That would get the answer quickly. Or we could play along with a little more mathematics. Notice that

\frac{r}{r+b}>\frac{\:r-1}{r+b-1}

Therefore, we can create the inequalities

\left(\frac{r}{r+b}\right)^2>\frac{1}{2}>\left(\frac{\:r-1}{r+b-1}\right)^2

Taking the square roots, we have, for r>1.

\frac{r}{r+b}>\frac{1}{\sqrt{2}}>\frac{\:r-1}{r+b-1}

From the first inequality we get

r>\frac{1}{\sqrt{2}}\left( r+b \right)

or

\begin{align*}
r & >\frac{1}{\sqrt{2}-1}b \\ \\
r & > \left( \sqrt{2}+1 \right)b
\end{align*}

From the second we get

\left( \sqrt{2}+1 \right)b>r-1

or all told

\left(\sqrt{2}+1\right)b+1>r>\left(\sqrt{2}+1\right)b

For b=1, r must be greater than 2.414 and less than 3.414, and so the candidate is r=3. For r=3, \ b=1, we get

P\left(2\:\text{red socks}\right)=\frac{3}{4}\cdot \frac{2}{3}=\frac{1}{2}

And so, the smallest number of socks is 4.

Beyond this, we investigate even values of b.

br is betweeneligible rP\left(2 \ \text{red socks}\right)
25.8, 4.85\frac{5\left( 4 \right)}{7\left( 6 \right)} \neq \frac{1}{2}
410.7, 9.710 \frac{10\left( 9 \right)}{14\left( 13 \right)} \neq \frac{1}{2}
615.5, 14.515 \frac{15\left( 14 \right)}{21\left( 20 \right)} = \frac{1}{2}

 

And so, 21 is the smallest number of socks when b is even. If we were to go on and ask for further values of r and b so that the probability of two red socks is 1/2, we would be wise to appreciate that this is a problem in the theory of numbers. It happens to lead to a famous result in Diophantine Analysis obtained from Pell’s equation. Try r = 85, b = 35.


Advertisements
Advertisements

College Physics by Openstax Chapter 2 Problem 37


Dragsters can actually reach a top speed of 145 m/s in only 4.45 s—considerably less time than given in Example 2.10 and Example 2.11.

(a) Calculate the average acceleration for such a dragster.

(b) Find the final velocity of this dragster starting from rest and accelerating at the rate found in (a) for 402 m (a quarter mile) without using any information on time.

(c) Why is the final velocity greater than that used to find the average acceleration? Hint: Consider whether the assumption of constant acceleration is valid for a dragster. If not, discuss whether the acceleration would be greater at the beginning or end of the run and what effect that would have on the final velocity.


Solution:

We are given the following: v_0=0\ \text{m/s} ; v_f=145 \ \text{m/s}; and \Delta t=4.45 \ \text{sec} .

Part A

To compute for the average acceleration a, we are going to use the formula

a=\frac{\Delta v}{\Delta t}=\frac{v_f-v_0}{\Delta t}

Substituting the given values, we have

\begin{align*}
a & =\frac{v_f-v_0}{\Delta t} \\
a & =\frac{145\:\text{m/s}-0\:\text{m/s}}{4.45\:\text{s}} \\
a & =32.6\:\text{m/s}^2 \ \qquad \ \color{DarkOrange} \left( \text{Answer} \right)
\end{align*}

Part B

We are given the following: a=32.6 \ \text{m/s}^2 ; v_0=0 \ \text{m/s}; and \Delta x=402 \ \text{m} .

Since we do not have any information on time, we are going to use the formula

\left(v_f\right)^2=\left(v_0\right)^2+2a\Delta x

To compute for the final velocity, we have

v_f=\sqrt{\left(v_0\right)^2+2a\Delta \:x}

Substituting the given values:

\begin{align*}
v_f & =\sqrt{\left(v_0\right)^2+2a\Delta \:x} \\
v_f & =\sqrt{\left(0\:\text{m/s}\right)^2+2\left(32.6\:\text{m/s}^2\right)\left(402\:\text{m}\right)} \\
v_f & =162\:\text{m/s} \ \qquad \ \color{DarkOrange} \left( \text{Answer} \right)

\end{align*}

Part C

The final velocity is greater than that used to find the average acceleration because the assumption of constant acceleration is not valid for a dragster. A dragster changes gears and would have a greater acceleration in first gear than second gear than third gear, etc. The acceleration would be greatest at the beginning, so it would not be accelerating at 32.6 m/s2 during the last few meters, but substantially less, and the final velocity would be less than  162\:\text{m/s}.


Advertisements
Advertisements

Hydrology and Floodplain Analysis by Bedient et.al. Chapter 1 Problem 1


What is the hydrologic cycle? What are the pathways that precipitation falling onto the land surface of the Earth is dispersed to the hydrologic cycle?


Solution:

The hydrologic cycle is a continuous process in which water is evaporated from water surfaces and the oceans, moves inland as moist are masses, and produces precipitation if the correct vertical lifting conditions exist.

A portion of precipitation (rainfall) is retained in the soil near where it falls and returns to the atmosphere via evaporation (the conversion of water vapor from a water surface) and transpiration (the loss of water vapor through plant tissue and leaves). Combined loss is called evapotranspiration and is a maximum value if the water supply in the soil moisture conditions and soil may reenter channels layer as interflow or may percolate to recharge the shallow groundwater. The remaining portion of the precipitation becomes overland flow or direct runoff which flows generally in a downgradient direction to accumulate in local streams that then flow into rivers.


Advertisements
Advertisements