Tuesday, 1 November 2016

Solution Manual for Sustainable Energy 1st Edition by Richard Dunlap

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Chapter 2
Past, Present and Future
World Energy Use
Problem 2.1 Locate information on the total primary energy consumption per capita and per dollar of GDP for five states from different geographical regions in the United States Discuss any relationships between energy use and factors such as climate, population density, types of industry, and other variables that are apparent.
Solution Per capita energy statistics are available for all states at:
http://www.statemaster.com/graph/ene_tot_ene_con_percap-total-electricity-consumption-per-capita
and per $GDP energy statistics are available for all states at:
http://www.statemaster.com/graph/ene_tot_ene_con_pergdp-energy-total-consumption-per-gdp
Choosing the following state the information from the web site is tabulated. Note that values in the table are in BBtu per year. These are converted to GJ as 1055 BBtu = 1GJ. Note that the average over all states is ~350 GJ per capita per year.
State
E(GJ)/Capita
E(GJ)/$GDP
Alaska
1171
0.0229
Alabama
450
0.0148
Maine
392
0.0120
Massachusetts
255
0.00514
Florida
245
0.00734
We expect that the energy per capita will be inversely proportional to the population density and inversely proportional to the average temperature. The population density and per capita GDP are readily available on the internet (e.g. Wikipedia) as given (for Jan 2010) in the table below.
State
population/km2
$GDP per capita
Alaska
0.46
65,143
Alabama
30.4
36,333
Maine
16.6
40,923
Massachusetts
324
58,108
Florida
135
40,106
Per capita energy consumption in Alaska is by far the highest. This is clearly expected on the basis of a very low population density and a very cold climate. Alabama has a warm
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8
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climate but a high per capita energy consumption. This can in fact be due to the moderate population density. This is a bit anomalous in comparison with Maine, which has a lower population density and cooler climate. Massachusetts by comparison with Maine has a slightly warmer climate but a much higher population density and a correspondingly smaller energy use. Florida has a much milder climate than Massachusetts, which compensates for its somewhat lower population density. Economic factors can be accounted for by inspecting the energy use per GDP. Note that
()()1GDP/capitacapita/GDP/−×=EE
Alaska has a high GDP/capita but not enough to compensate for other factors. Alabama has a low GDP/capita which partly accounts for its large energy use. This may be reflected by the presence of rather energy intensive industries. Maine has a higher GDP/capita which may partially explain its lower energy use than Alabama. The order of Massachusetts and Florida are reversed when considering E/GDP rather than E/capita. This is a result of its much larger GDP per capita and is reflection of the presence of more high technology industries and businesses.
Problem 2.2 A quantity has a doubling time of 110 years. Estimate the annual percent increase in the quantity.
Solution From equation (2.9) the annual rate of increase R is given as
DtR2ln100=
where tD is the doubling time. If tD is 110 years then
()()year per %63.0y 110693.0100=×=R
This is much less than 10% so the approximation given in equation (2.9) is valid.
Problem 2.3 The population of a particular country has a doubling time of 45 years. When will the population be three times its present value?
Solution From equation (2.7) the constant a can be determined from the doubling time as
antD21=
so
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©2015 Cengage Learning. All Rights Reserved. May not be scanned, copied or duplicated, or posted to a publicly accessible website, in whole or in part.
Dtna21=
For tD = 45 years then
1y0154.045693.0−==a
From equation (2.4) the quantity of any time is given in terms of the initial value as
()()atNtNexp0=
so solving for t we get
()=0ln1NtNat
for N(t) = 3N0 then we get
()years3.713lny0154.011=

=−t
Problem 2.4 Assume that the historical growth rate of the human population was constant at 1.6% per year. For a population of 7 billion in 2012, determine the time in the past when the human population was 2.
Solution As the annual percentage growth rate is small then we can use the approximation of equation (2.4) to get the doubling time from R so
()()years31.436.1693.01002ln100=×=

=RtD
from equation (2.7) the constant a can be found to be
10.016y43.31y0.6932ln−==

=Dta
from equation (2.4) we start with an initial population of N0 = 2 at t = 0 then N(t) = 6.7 × 109 then from
()()atNtNexp0=
so
()y13742107ln016.01ln190=×==NtNat
in the past or at year 2012 – 1374 = 638 (obviously growth rate was not constant).
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©2015 Cengage Learning. All Rights Reserved. May not be scanned, copied or duplicated, or posted to a publicly accessible website, in whole or in part.
Problem 2.5 What is the current average human population density (i.e., people per square kilometer) on earth?
Solution The radius of the Earth is 6378 km (assumed spherical). The total area (including oceans) is ()()()2822km101.5km637814.344×=××==rAÏ€. The total current population is 6.7 × 109, so the population density is
2289people/km1.13km101.5107.6=××
If only land area is included, the land area on Earth is from various values given on the web range from 1.483 × 108 km2 to 1.533 × 108 km2. Using 1.5 × 108 km2we find
2289people/km7.44km105.1107.6=××
Problem 2.6 The total world population in 2012 was about 7 billion and Figure 2.11 shows that at that time the actual world population growth rate was about 1% per year. The figure also shows an anticipated roughly linear decrease in growth rate that extrapolates to zero growth in about the year 2080. Assuming an average growth rate of 0.5% between 2012 and 2080, what would the world population be in 2080? How does this compare with estimates discussed in the text for limits to human population?
Solution If R = 0.5% per year then the doubling time is found from equation (2.9) to be
()()y6.1385.0693.01002ln10=×==RtD
using equation (2.7) to get the constant a
1y005.0y6.138693.02ln−===Dta
then equation (2.4) gives
()()atNtNexp0=
so from 90107×=N people and years6820122080=−=twe find
()()()()()people108.9y68y005.0exp107919×=××=−tN
This is consistent with comments in the text which suggest that the limit to human population can not be much more than 10 billion.
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©2015 Cengage Learning. All Rights Reserved. May not be scanned, copied or duplicated, or posted to a publicly accessible website, in whole or in part.
Problem 2.7 The population of a state is 25,600 in the year 1800 and 218,900 in the year 1900. Calculate the expected population in the year 2000 if (a) the growth is linear and (b) the growth is exponential.
Solution If population growth is linear then for 100 years between 1800 and 1900 it grows by ()33103.193106.259.218×=×−, so the population would grow by another 3103.193×during the 100 years from 1900 to 2000 for a total of
()people102.412103.1939.21833×=×+
If the population growth is exponential then from equation (2.4) for 90107.6×=N in 1800 then for t = 100 years, N(t) is 3109.218×. From this a can be found to be
()1330y0215.0106.25109.218lny1001ln1−=

×××

==NtNta
Then using 30109.218×=N in year 1900 the population at 100y (i.e. in year 2000) is
()()()()()6131087.1y100y0215.0exp109.218×=×××=−tN
about 4.5 times the value for linear growth.
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©2015 Cengage Learning. All Rights Reserved. May not be scanned, copied or duplicated, or posted to a publicly accessible website, in whole or in part.
Problem 2.8 The population of a country as a function of time is shown in the following table. Is the growth exponential?
year
population (millions)
1700
0.501
1720
0.677
1740
0.891
1760
1.202
1780
1.622
1800
2.163
1820
2.884
1840
3.890
1860
5.176
1880
6.761
1900
8.702
1920
10.23
1940
11.74
1960
13.18
1980
14.45
2000
15.49
Solution For exponential growth
()()()00expttaNtN−= so ()()00lnttaNtN−=


and the ln of the related population should be linear in time. Calculating ()0/NtN from the values above gives the tabulated values. They are plotted as a function of t - tD as shown
year
population (millions)
year - 1700
ln[N(t)/N(1700)]
1700
0.501
0
0
1720
0.677
20
0.301065
1740
0.891
40
0.575738
1760
1.202
60
0.875136
1780
1.622
80
1.174809
1800
2.163
100
1.462645
1820
2.884
120
1.750327
1840
3.89
140
2.049558
1860
5.176
160
2.335182
1880
6.761
180
2.60232
1900
8.702
200
2.854702
1920
10.23
220
3.016474
1940
11.74
240
3.154151
1960
13.18
260
3.26985
1980
14.45
280
3.361844
2000
15.49
300
3.431344
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The graph shows that the ln is linear and hence the population is exponential until ~ 1900 when the increase is less than exponential.
00.511.522.533.54050100150200250300350year-1700ln[n(t)/n(1700)]
Problem 2.9 Consider a solar photovoltaic system with a total rated output of 10 MWe and a capacity factor of 29%. If the total installation cost is $35,000,000, calculate the decrease in the cost of electricity per kilowatt-hour if the payback period is 25 years instead of 15 years. Assume a constant interest rate of 5.8%.
Solution From Example 2.3 the contribution to the cost of electricity per kWh due to the capital cost is
()()()()111h/y87601−++×TTiiiRf
Using I = 35,000,000, i = 0.058, R = 104 kW, f = 0.29, then for a payback period of 15 years the cost per kWh is
()()()/kWh140.0$102.0378.11058.1058.1058.0876029.010105.3151547=×=−×××××
For a payback period of 25 years the cost is
()()()kWh/106.0$0767.0378.11058.1058.1058.0 378.12525=×=−××
or a decrease of (0.140 – 0.106) = $0.034 per kWh.
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Solution Manual for Simulation with Arena 6th Edition by Kelton-16

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Exercise 2-16 Solution file from Kelton/Sadowski/Zupick, Simulation With Arena, 6th edition, McGraw-Hill, 2015
As noted in the text, the mean of the ten given interarrival times is 4.08 minutes, and the mean of the ten given service times is 3.46 minutes. In Exercise 2-4, each service time was to be increased by 3 minutes, so of course the mean of these ten new service times would be 3 + 3.46 = 6.46 minutes. Now this is greater than the 4.08-minute mean interarrival time, so that it takes (on average) longer to serve a part than the average time between successive part arrivals, so over a long time period the system will just get more and more full, i.e. it will “explode,” and will grow without bound. So in the long run this system is unstable and wouldn’t operate in any sort of acceptable way.
This file was downloaded
from the Solutions area of
the website for the 6th ed.
of "Simulation With Arena"
by Kelton, Sadowski, and
Zupick, McGraw-Hill, 2015.

Solution Manual for Simulation with Arena 6th Edition by Kelton-09

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Exercise 2-9 Solution file from Kelton/Sadowski/Zupick, Simulation With Arena, 6th edition, McGraw-Hill, 2015
The drill press is down for 4 of the 20 minutes, so the proportion of downtime is obviously 4/20 = 0.20, and this will be true regardless of what the interarrival and service-time input data happen to be. From the solution to Exercise 2-8, the drill press is busy all the rest of the time (16 minutes) so the proportion of time up and busy is 16/20 = 0.80 and the proportion of time idle but up is 0; these last two figures will, however, be dependent on what the interarrival and service-time data happen to be.
This file was downloaded
from the Solutions area of
the website for the 6th ed.
of "Simulation With Arena"
by Kelton, Sadowski, and
Zupick, McGraw-Hill, 2015.

Solution Manual for Simulation with Arena 6th Edition by Kelton-08

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Exercise 2-8 Solution file from Kelton/Sadowski/Zupick, Simulation With Arena, 6th edition, McGraw-Hill, 2015
Introduce a new event type (Down) and schedule it on initialization to happen at time 4; the extra event record is shaded in the table below. This does nothing to the state
variables or statistical accumulators until time 4 rolls around and the Down event is executed. At that time, the time of departure of the part in service (entity no. 2) is changed
from its prior value (4.66) to that plus the 4-minute downtime, or 4.66 + 4 = 8.66 (new event time shaded in the event calendar at that time). We also schedule an event for the
drill press to come back up (Up) at time 4 + 4 = 8 (event record shaded). In this particular realization, having such an “Up” event might not be deemed necessary, but in general it
could be in the case that the Down event happened when the machine happened to be idle, in which case we’d need to define it as busy at that time (blocking arrivals during the
downtime from entering service), and when it comes back up execute logic to release the first part in queue (if any) to begin service. The calculations in the table below are
similar to what’s in Section 2.4.3 so we leave it to you to recreate this table and check your work. Here’s a crude plot of the number-in-queue curve:
The final output performance measures are:
Total production = 4
Average waiting time in queue = 27.17/5 = 5.43 minutes per part (5 parts)
Maximum waiting time in queue = 12.16 minutes
Average total time in system = 31.58/4 = 7.90 minutes per part (4 parts)
Maximum total time in system = 12.78 minutes
Time-average number of parts in queue = 29.09/20 = 1.45 parts
Maximum number of parts in queue = 3 parts
Drill-press utilization = 20.00/20 = 1.00
Comparing these results to those in Table 2-3, we see that the downtime had the effect of reducing production and increasing congestion ... OK, maybe not surprising, but it would
have been hard to quantify this without the simulation. A legitimate question (that we hope you’re asking yourself) is whether the observed differences are statistically significant
... stay tuned (Exercise 6-18).
Just-Finished Event Variables Attributes Statistical Accumulators Event Calendar
Entity Time Event Arrival Times:
No. t Type Q(t) B(t) (In Queue) In Service P N WQ WQ* TS TS* Q Q* B [Entity No., Time, Type]
  [1, 0.00, Arr]
– 0.00 Init 0 0 ( ) – 0 0 0.00 0.00 0.00 0.00 0.00 0 0.00 [–, 4.00, Down]
[–, 20.00, End]
[2, 1.73, Arr]
1 0.00 Arr 0 1 ( ) 0.00 0 1 0.00 0.00 0.00 0.00 0.00 0 0.00 [1, 2.90, Dep]
[–, 4.00, Down]
[–, 20.00, End]
[1, 2.90, Dep]
2 1.73 Arr 1 1 (1.73) 0.00 0 1 0.00 0.00 0.00 0.00 0.00 1 1.73 [3, 3.08, Arr]
[–, 4.00, Down]
[–, 20.00, End]
This file was downloaded
from the Solutions area of
the website for the 6th ed.
of "Simulation With Arena"
by Kelton, Sadowski, and
Zupick, McGraw-Hill, 2015.

Solution Manual for Simulation with Arena 6th Edition by Kelton-07

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Exercise 2-7 Solution file from Kelton/Sadowski/Zupick, Simulation With Arena, 6th edition, McGraw-Hill, 2015
Here are the results from the original model (i.e., Table 2-4), followed by those from the new model, with the new summary measures in italics:
Original Model
Replication
Sample
Performance Measure
1
2
3
4
5
Average
Std. Dev.
Half Width
Total production
5
3
6
2
3
3.80
1.64
2.04
Average waiting time in queue
2.53
1.19
1.03
1.62
0.00
1.27
0.92
1.14
Average total time in system
6.44
5.10
4.16
6.71
4.26
5.33
1.19
1.48
Time-average no. parts in queue
0.79
6.63
0.36
0.16
0.05
1.60
2.83
3.51
Drill-press utilization
0.92
0.59
0.90
0.51
0.70
0.72
0.18
0.23
Double-Time Arrivals
Replication
Sample
Performance Measure
1
2
3
4
5
Average
Std. Dev.
Half Width
Total production
6
4
6
4
5
5.00
1.00
1.24
Average waiting time in queue
7.38
2.10
3.52
2.81
2.93
3.75
2.09
2.60
Average total time in system
10.19
5.61
5.90
6.93
5.57
6.84
1.95
2.42
Time-average no. parts in queue
2.88
0.52
1.71
0.77
2.25
1.63
0.99
1.23
Drill-press utilization
1.00
0.92
1.00
0.95
1.00
0.97
0.04
0.05
One not-quite-right, but still-reasonable, approach is to see if the original-model and changed-model confidence intervals for a given measure overlap or not—if they overlap we’re not getting a clear indication of a real difference. Taking a look at the above results, all five pairs of confidence intervals overlap, so while the averages seem to indicate higher production, congestion, and utilization, there is just too much uncertainty to conclude this firmly. There is a quite-right-indeed way to do this comparison, and Arena has a built-in way to help you do it (in the Output Analyzer); see Chapter 6.
This file was downloaded
from the Solutions area of
the website for the 6th ed.
of "Simulation With Arena"
by Kelton, Sadowski, and
Zupick, McGraw-Hill, 2015.

Solution Manual for Simulation with Arena 6th Edition by Kelton-06

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Exercise 2-6 Solution file from Kelton/Sadowski/Zupick, Simulation With Arena, 6th edition, McGraw-Hill, 2015
(a) (Reason 1): The estimates of the expected interarrival and service times are subject to random variation, so they are not exact; thus, the 19.31 from the M/M/1 queueing formula is not exact since it depends on these numbers. (Reason 2): The queueing-theoretic formula assumes interarrival and service times that are both exponentially distributed, and we don’t know that this is true for the (given) values in Table 2-1. (Reason 3): The formula is for long-run (infinite-length) performance, but our simulation was for only 20 simulated minutes, which may not be “close enough” to infinity. (Reason 4): The formula is an exact value (no variance), but our simulation output is for the interarrival and service times that happen to have been given in Table 2-1; other input values, even if from the same “source,” would, in general, clearly produce different output results.
(b) It’s different from the 2.53 from the 20-minute simulation run since it’s longer (much longer), yielding different input so different output. It’s different from the 19.31 for reasons (1), (2), and (4) given in our solution to part (a); reason (3), while technically still valid, is perhaps not as convincing since a million is closer to infinity than 20 is.
(c) The M/M/1 formula for the expected waiting time in queue with these values is 3.332/(5 – 3.33) = 6.67. This differs from the 19.31 since we’re now using exact, not estimated, values for the mean interarrival and service times. It’s different from the 2.53 for any of reasons (2), (3), and (4) given in our solution to part (a). It’s different from the 3.60 for reasons (2) and (4) given in our solution to part (a).
(d) This is actually quite close to the theoretical result of 6.67 from part (c) since the conditions are similar—long run (if not quite infinite), exponential interarrival and service times—the only probable explanation for the small discrepancy is that the simulation produces results that are subject to uncertainty (though not much in such a long simulation, producing lots of output data). It differs from the 3.60 since we’re using a different interarrival-time distribution here (exponential instead of triangular) even though the mean is the same, and also due to the fact that both results are subject to variation. It differs from the 2.53 due to the different service-time distribution, different run length, and the fact that both results are subject to variation. It differs from the 19.31 since the parameters used for the 19.31 were not exact, and since the simulation result here is subject to variation.
This file was downloaded
from the Solutions area of
the website for the 6th ed.
of "Simulation With Arena"
by Kelton, Sadowski, and
Zupick, McGraw-Hill, 2015.

Solution Manual for Simulation with Arena 6th Edition by Kelton-05

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Exercise 2-5 Solution file from Kelton/Sadowski/Zupick, Simulation With Arena, 6th edition, McGraw-Hill, 2015
There are now two “spots” in the server rather than one, shown in the table as two underlined spaces for In Service Arrival Times. Departure records are still placed on the event calendar, but we need to indicate in parentheses after the Arrival Times of entities in service their entity number to match them up with the correct departure records. Table 2-2 becomes:
Just-Finished Event
Variables
Attributes
Statistical Accumulators
Event Calendar
Entity
Time
Event
Arrival Times:
No.
t
Type
Q(t)
B(t)
(In Queue)
In Service
P
N
WQ
WQ*
TS
TS*
Q
Q*
B
[Entity No.,
Time,
Type]


[1,
0.00,
Arr]

0.00
Init
0
0
()

0
0
0.00
0.00
0.00
0.00
0.00
0
0.00
[–,
20.00,
End]

[2,
1.73,
Arr]
1
0.00
Arr
0
1
()
0.00 (1)
0
1
0.00
0.00
0.00
0.00
0.00
0
0.00
[1,
2.90,
Dep]

[–,
20.00,
End]
[1,
2.90,
Dep]
2
1.73
Arr
0
2
()
0.00 (1)
0
2
0.00
0.00
0.00
0.00
0.00
0
1.73
[3,
3.08,
Arr]
1.73 (2)
[2,
3.49,
Dep]
[–,
20.00,
End]
[3,
3.08,
Arr]
1
2.90
Dep
0
1
()

1
2
0.00
0.00
2.90
2.90
0.00
0
4.07
[2,
3.49,
Dep]
1.73 (2)
[–,
20.00,
End]
[2,
3.49,
Dep]
3
3.08
Arr
0
2
()
3.08 (3)
1
3
0.00
0.00
2.90
2.90
0.00
0
4.25
[4,
3.79,
Arr]
1.73 (2)
[3,
6.47,
Dep]
[–,
20.00,
End]
[4,
3.79,
Arr]
2
3.49
Dep
0
1
()
3.08 (3)
2
3
0.00
0.00
4.66
2.90
0.00
0
5.07
[3,
6.47,
Dep]

[–,
20.00,
End]
[5,
4.41,
Arr]
4
3.79
Arr
0
2
()
3.08 (3)
2
4
0.00
0.00
4.66
2.90
0.00
0
5.37
[3,
6.47,
Dep]
3.79 (4)
[4,
8.31,
Dep]
[–,
20.00,
End]
[3,
6.47,
Dep]
5
4.41
Arr
1
2
(4.41)
3.08 (3)
2
4
0.00
0.00
4.66
2.90
0.00
1
6.61
[4,
8.31,
Dep]
3.79 (4)
[6,
18.69,
Arr]
[–,
20.00,
End]
[4,
8.31,
Dep]
3
6.47
Dep
0
2
()
4.41 (5)
3
5
2.06
2.06
8.05
3.39
2.06
1
10.73
[5,
10.93,
Dep]
3.79 (4)
[6,
18.69,
Arr]
[–,
20.00,
End]
[5,
10.93,
Dep]
4
8.31
Dep
0
1
()
4.41 (5)
4
5
2.06
2.06
12.57
4.52
2.06
1
14.41
[6,
18.69,
Arr]

[–,
20.00,
End]
[6,
18.69,
Arr]
5
10.93
Dep
0
0
()

5
5
2.06
2.06
19.09
6.52
2.06
1
17.03
[–,
20.00,
End]

[7,
19.39,
Arr]
6
18.69
Arr
0
1
()
18.69 (6)
5
6
2.06
2.06
19.09
6.52
2.06
1
17.03
[–,
20.00,
End]

[6,
23.05,
Dep]
[–,
20.00,
End]
7
19.39
Arr
0
2
()
18.69 (6)
5
7
2.06
2.06
19.09
6.52
2.06
1
17.73
[7,
21.46,
Dep]
19.39 (7)
[6,
23.05,
Dep]
[8,
34.91,
Arr]
[7,
21.46,
Dep]

20.00
End
0
2
()
18.69 (6)
5
7
2.06
2.06
19.09
6.52
2.06
1
18.95
[6,
23.05,
Dep]
19.39 (7)
[8,
34.91,
Arr]
This file was downloaded
from the Solutions area of
the website for the 6th ed.
of "Simulation With Arena"
by Kelton, Sadowski, and
Zupick, McGraw-Hill, 2015.
Here are the summary results:
Performance Measure
Value
Result from Table 2-3
Change
Total
production
5 parts
5 parts No change
Average waiting time in queue 0.29 minute per part (7 parts)
2.53 minutes per part
(6 parts) Decreased
Maximum waiting time in queue 2.06 minutes
8.16 minutes Decreased
Average total time in system 3.82 minutes per part (5 parts)
6.44 minutes per part
(5 parts) Decreased
Maximum total time in system 6.52 minutes
12.62 minutes Decreased
Time-average number of parts in queue 0.10 part
0.79 part Decreased
Maximum number of parts in queue 1 part
3 parts Decreased
Drill-press utilization 0.47 [= 18.95/(2  20)]
(dimensionless proportion)
0.92
(dimensionless proportion) Decreased
Congestion is considerably relieved on all measures; the average total time in system is reduced the least since parts must still endure their (same) processing times no matter how little time they have to wait in queue.