1.3 D 1.4 B When the working fluid crosses the boundary, it is a control volume, as during intake and exhaust.. Temperature is the same for the entire room or half the room.. 1.15 B W
Trang 1Solution Manual for Thermodynamics for Engineers 1st Edition by Kroos
1.1 (B) The utilization of energy is not of concern in our study If you use energy to power your
car, or your car seat is your own decision
1.2 (C) All properties are assumed to be uniformly distributed throughout the volume
1.3 (D)
1.4 (B) When the working fluid crosses the boundary, it is a control volume, as during intake
and exhaust The ice plus the water forms the system of (C) The entire atmosphere
forms the system of (D)
1.5 (C) An extensive property doubles if the mass doubles Temperature is the same for the entire
room or half the room
1.6 (D) A process may be very fast, humanly speaking, but molecules move very rapidly so an
engine operating at 4000 rpm is not thermodynamically fast All sudden expansion
processes and combustion processes are non-equilibrium processes Air leaving a balloon is thermodynamically slow
1.7 (B) If force, length, and time had been selected as the three primary dimensions, the newton would
have been selected and mass expressed in terms of the other three But, in Thermo-dynamics,
the newton is expressed as kg·m/s2
1.8 (D) W = J/s = N ⋅ m/s = (kg ⋅ m/s 2
) ⋅ m/s = kg ⋅ m 2
/s 3
1.9 (A) 34 000 000 000 N = 34 × 109
N = 34 GN (or 34 000 MN.)
m3
v = V = 1 = 1
= 0.0008 m3 /kg
SG =
ρ
Hg
3
ρ
1000 kg/m3
water
1.11 (D) We must know if the surface is horizontal, vertical, on an angle? The surface cannot be
assumed to be horizontal just because it is drawn that way on the paper (Sometimes problems aren’t fair This is an example of such a problem.)
1.12 (C) P = Fn = 36cos30° kN
= 1559 kN/m2
or 1560 kPa
m2 /cm2
1.13 (A) Use Eq 1.13 to convert to pascals:
Trang 2= 56 030 kg/m ⋅ s 2
or 56.03×10 3
N/m 2
1
Trang 31.14 (C) ∑ F = 0 PA + Kx = mg
P × π × 0.052 + 400× 0.2 = 40× 9.81. ∴ P = 39 780 N/m2
or 39.8 kPa gage
The atmospheric pressure acts down on the top and up on the bottom of the
cylinder and hence cancels out
1.15 (B) We do not sense the actual temperature but the temperature gradient between our skin and the
water As our skin heats up, the water feels cooler so we increase the water temperature until
it feels warm again This is done until out skin temperature ceases to change An object feels cool if its temperature is less than out skin temperature If that’s the case, a temperature difference occurs between our skin and the object over a very small distance,
creating a temperature gradient (Tskin−Tobject) / x
1.16 (B) The energy equation states that at the position of maximum compression, the kinetic energy of
the vehicle will be zero and the potential energy of the spring will be maximum, that is,
1 2 1 2
2 m V = 2 Kx (The velocity must be expressed in m/s.)
1 80×1000
2 1 ∴ K = 98.8×106
N/m or 100
= × K × 0.1 2
2 3600 2
If the mass is in kg, the velocity in m/s, and x in meters, K will be in N/m But, check the
units to make sure
Get used to always using N, kg, m, and s and the units will work out You don’t have
to always check all those units It takes time and on a multiple-choice test, there are usually problems left over when time runs out
1.17, 1.18, and 1.19 The Internet has the answers!
1.20 True Thermodynamics presents how energy is transferred, stored, and transformed from one
form to another If you use it to dry your hair, power your car, or store it in a battery, we don’t really care Just use it any way that allows you to enjoy life!
1.21 Energy derived from coal is not sustainable since coal will eventually not be available,
even though that may take 500 years If an energy source is not available indefinitely, it is not sustainable
1.22 Consult the Internet
1.23 A large number of engineers were required when the industrial revolution occurred
1.24 Trains were traveling the rails in the mid-1800s so mechanical engineers were needed, not
to drive the trains, but to design them! Coal was mined with a pick and shovel until the late 1800’s Power plants and automobiles also came near the end of the 1800’s
1.25 It’s CO2 and it keeps things very cold Check it out on the Internet
Trang 4© 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
Trang 51.26 i) A system, ii) a control volume, iii) a system, iv) a system No fluid crosses the boundary of
a system Fluid crosses the boundary of a control volume
1.27 Before
The system and c.v are identical
Control surface
After
The system is the air inside plus that which has exited The c.v
extends to the exit of the balloon nozzle
1.28 The number of molecules in a cubic meter of air at sea level is (3×1016
)×109
=3×1025
4
10 12 molecules
3×10
25
molecules/m
3
1.29 Catsup is not a fluid It is a pseudo plastic or a shear-thinning liquid, whatever that is! A fluid
always moves if acted upon by a shear A plastic can resist a shear but then moves when the shear is sufficiently large Catsup is like that: first it won’t move, then it suddenly comes
1.30 From Wikipedia, 1 stone = 6.35 kg (= 14 lbm) ∴6.3 stones = 6.3× 6.35 = 40 kg
1.31 The units using Newton’s 2nd
law are simpler:
32.2 ft/s 2 lbf = slug ×
ft
is simpler than lbf=lbm×
The conversion between mass and weight does not require the use of a gravitational
constant when using the slug as the mass unit in the English system
1.32 Volume is extensive since it increases when the mass is increased, other properties
remaining constant
1.33 % change=
×100= −0.992% or
1
−1 % 0.001008
1 = 57.2 lbm/ft3 ρwater = 62.4 lbm/ft3
So, ice is lighter than water at
1.34 ρice= =
v 0.01747 32ºF, so ice floats If ice was heavier than water, it would freeze from the bottom up That would be rather disastrous Fish as well as skaters would have a problem You can speculate as
to the consequences
3
Trang 61.35 SGHg= 13 600 = 13.6
1000
kg m
W = γ V = 13 600 3 × 9.81 2 × 2 m3 = 266 800 N
m s
W = 266 800 N × 0.2248 lbf = 59,980 lbf
1.36 a ) ρ = 1
= 1 = 0.2 kg/m3
, m = ρV = 0.2× 2 = 0.4 kg, W = mg = 0.4× 9.8 = 3.92 N
/kg, ρ = 1 = 500 kg/m3
, v = 1 = 1 = 0.0196 m 3 /kg
ρ 51
1.37 a ) ρ = 1 = 1 = 0.02 lbm/ft3
, m = ρV = 0.02× 20 = 0.4 lbm,
32.2 ft/s2
W = m g = 0.4 lbm × = 0.4 lbf
g c
32.2 ft-lbm/lbf-s2
b ) v = 1 = 1 = 50 ft3
/lbm , m = ρV = 0.02× 20 = 0.4 lbm,
ρ 0.02
g 32.2 ft/s2
g c
2 = 1000 lbf
g c 32.2 ft-lbm/lbf-s2
v = V = 20 = 0.02 ft3
/lbm , ρ = 1
= 1 = 50 lbm/ft3
d ) m = W g
c = 500 lbf × 32.2 ft-lbm/lbf-s
2
= 500 lbm
32.2 ft/s2
v = V = 20 = 0.04 ft3
/lbm, ρ = 1 = 1 = 25 lbm/ft3
m 500 v 0.04 This problem should demonstrate the difficulty using English units with lbm and lbf! Note that
lbm and lbf are numerically equal at sea level where g = 32.2 ft/s2
, which will be true for
problems of interest in our study In space travel, g is not 32.2 ft/s2
1.38 ρ= 1
= 1 = 0.25 kg/m 3
, SG= ρx = 0.25 = 0.00025 ,m = V = 8 m 3
= 2 kg
ρ
2 =
water
W = mg = 2 kg × 9.81 19.62 N (We used N = kg·m/s2
.)
Trang 81 1
5 ft3 ρ x 0.2 lbm/ft3
1.39 v = = = /lbm , SG=
ρ
m = ρV = 0.2× 20 = 4 lbm, W = m g = 4 lbm × 32.2 ft/s
2
= 4 lbf
g c 32.2 ft-lbm/lbf-s2
1.40 Only (ii) can be considered a quasi-equilibrium process Process (i) uses a temperature
distribution in the room to move the heated air to other locations in the room, i.e., the temperature is not uniform When the membrane in process (iii) is removed, a sudden expansion occurs, which cannot be considered a quasi-equilibrium process
1.41 From Table B-1 in the Appendix, we observe that So,
i) SG = 1.225 kg/m3
=
0.001225 1000 kg/m3
ii) SG = 0.6012×1.225 kg/m3= 0.000
736 1000 kg/m3 iii) SG = 0.3376×1.225 kg/m3= 0.000
414 1000 kg/m3
1.42 From Table B-1 in the Appendix, we observe find the local atmospheric pressure First,
or 206 kPa gage
(We used N = kg·m/s2.)
iii) P = 206 kPa + 101× 0.5334 kPa = 260 kPa
1.43 Refer to Fig 1.6 and Eq 1.14 The pressure in the tire would be P2 and P1 would be open to the
atmosphere:
P = 3 4 kg × 1002 cm 2
× 9.81 m = 334 000 kg ⋅ m/s2 = 334 000 N/m2
gage cm 2 m 2 s 2 m 2
P − P = ρ g h 334 000 N = (1000 × 13.6 ) kg × 9.81 m × h ∴ h = 2.50 m or 2500 mm
m2
m3
1.44 P=ρ gh 100 000 m2 = 786m3 × 9.81 s2 × h ∴ h = 13.0 m (We used N = kg·m/s )
1.45 P= 10 atm ⋅ 100 kPa
= 1000 kPa ∴ P = 1000 kPa − 100 kPa = 900 kPa
5
Trang 91.46 P=ρ g h = 1000 kg × 9.81 m × 0.25 m = 2453 Pa = 2.45 kPa gage
water m3 s2
P = ρHg g hHg 2453 = (1000× 13.6)× 9.81× hHg ∴ hHg = 0.0184m or 0.724 in 1.47 A measured pressure is a gage pressure a) P = ρ gh = 13 600 × 9 81× 0.10 = 13 340 Pa or 13.34 kPa gage b) P = ρ gh = 13 600 × 9 81× 0.28 = 37 360 Pa or 37.36 kPa gage P = P +P 1.48 a) abs gage atm =5+0.371×14.7=10.45 psia or 1505 psfa P = P +P b) abs gage atm= 20 + 0.371× 14.7 = 25.45 psia or 3665 psfa 1.49 Consult the Internet 1.50 Consult the Internet 1.51 T ( °R ) = T( °F) + 460 = 120 + 460 = 580°R 1.52 T ( °C) = T(K) − 273 = 3 − 273 = −270°C 1.53 T ( °R) = T(° F) + 460 = 400 + 460 = 860°R 1.54 T (K) = 37 + 273 = 310 K
1.55 Use Eq 1.20:
a) R = R e β ( T0−T )/T0T = 3000e4220(25 − 60)/ 298 ×333 = 677 Ω
0
= 97.8 Ω b) R=R e β(T0 −T )/T 0 T = 3000e4220(25 −120)/ 298 ×393
0 c)
= 23.6 Ω R=R e β ( T0−T )/T0T = 3000e4220(25 −180)/ 298 ×453
0
1.56 Use V = β V T
0.00018 2 4 3
π H = 0.00018× 3 π × 0.003 × 20
∴ H = 0.016 m or 16 mm a) 4
0.000182 4 3
b) π 4 H = 0.00018× 3 π × 0.003 × 40 ∴ H = 0.032 m or 32 mm 0.000182 4 3
c) π 4 H = 0.00018× 3 π × 0.003 × 60 ∴ H = 0.048 m or 48 mm 1.57 V = 60 mi ×5280 ft/mi = 88 ft/s , KE = m V 2
hr 3600 s/hr 2g c
= 2500 lbm × 882 = 300,600 ft-lbf
2 × 32.2 ft-lbm/lbf-s2
6
Trang 10or 300,600 ft-lbf = 386 Btu
778 ft-lbf/Btu The English unit on energy is most often the Btu (some authors use BTU)
1.58 KE + PE =
1
2 m V 2 + mgh =
1
2 × 5000 × 802 + 5000 × 9.81× 1000 = 65× 106 N ⋅ m = 65 MJ
1.59 At 10 000 m, g=9.81−3.32×10−6
Wsurface = mg = 140 000 × 9.81 = 1.373×106 N
W10 km = mg = 140 000 × 9.777 = 1.369 ×106 N
10 000 10 000
PE = ∫ mgdh = ∫ 140 000(9.81− 3.32 ×10−6
h ) dh
10 0002
2
= 1.371× 10 10 N ⋅
× 10 − 0.0023×10
7
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