This preview shows pages 1–14. Sign up to view the full content.
This preview has intentionally blurred sections. Sign up to view the full version.
View Full DocumentThis preview has intentionally blurred sections. Sign up to view the full version.
View Full DocumentThis preview has intentionally blurred sections. Sign up to view the full version.
View Full DocumentThis preview has intentionally blurred sections. Sign up to view the full version.
View Full DocumentThis preview has intentionally blurred sections. Sign up to view the full version.
View Full DocumentThis preview has intentionally blurred sections. Sign up to view the full version.
View Full DocumentThis preview has intentionally blurred sections. Sign up to view the full version.
View Full Document
Unformatted text preview: ASE 362K, Assignment No 3 Thursday, February 8, 2007 1) Review the section in Anderson on normal shock waves. 2) A blunt nosed projectile is moving at Mach 4 at sealevel where the static pressure
P = 1 atmosphere, and the static temperature T = ZOEC.
a) What is the projectile speed in m/s?
b) What are the static pressure, static temperature and the velocity dewnstream of the
normal shock wave?
c) What is the Mach # downstream of the wave, M2? d) How much does the downstream Mach number change if we double, then
quadruple the ﬂight Mach #? e) What is M2 if we accelerate to M1 = 00? 3) This question, on the attached sheet, is from Quiz #1, given when I taught this class in
spring 2006. It was in the closed book part. Try it without using your notes. Note that
to answer these questions you don’t have to remember normal shock equations and be
able to do c0mplicated arithmetic in your head. . ..you just need to bear in mind the
conservation equations and other basic things that are “fundamental” to normal shock waves such as the stagnation temperature is constant across the wave, the stagnation
pressure goes down etc ...... ..and which should be second nature to you. 4) A normal shock occurs in a ﬂuid which is not a perfect gas. In fact, the pressure and density are related by the expression p [dp/dp] = c, where c = a constant. Show that in this case the upstream and down stream Mach numbers are related by the equation
log (Mlz/Mgz) = M[2 — M22. £9.52 A
5) The Cylinder on the right is ﬂying at
sealevel. (1‘31=latm=105 Nm"2). Given that the drag comes entirely M C
from the pressure on face "A", what ' 6
is the ratio of the drag at Mach 3 to that at Mach 0.8? [You can assume
the pressure on face A is uniform]. 6) A normal shock wave is, in essence, a thermodynamic process (namely a
compression) and the change in properties across it can be expressed solely in terms
of thermodynamic variables, rather than introducing a "ﬂow" quantity, the Mach #. a+af1 1i 2 laugﬂ P
(y — l)+ (2/ + 1):;
and that the density ratio can be written as & = p, (y+1)+(y—1)%' Show that the change in internal energy can be written as (22 — el 2 In a student laboratory measurements are being made downstream of a normal shock
wave. The conditions upstream of the shock wave were measured by the instructor and
are all correct. The wave forms in air for which R = 287J/kg, Cp = 1005 I/kg and Y = 1.4.
Some of the measurements are shown on the attached sheet. If you think an error has been made say so and indicate the error, or errors. If you think the measurements are
okay, say so (NN points). Note: no answer = no points) N5 Answer iii
in i] $5 Suﬁ (0qu? (G'W‘O‘WW ' Lia“ (mid al° ly v.1 h“ R5115 (Back ’3 QAoLuaox.) Ov vu'k
V1,, 'www (awMe calwlala. 0r duct ‘7:
may“. 5w baa human “ﬂank aux M'
MM.\P“‘q\M 3m cowld Ac ('1. (WatsonMl “3a..
.Llpﬂaw a) Man ~.—. Von/om 3o VaQ = aloQHoo I:
ad, __ L (l'+>(28’?>CZ°CS>3 "' b Hm "'=‘+
khan = ‘3}; "*1" 5) Pa. ._ War (“‘2’”) = “1M” ’6’”)
72‘ M ‘S'H Pilp‘ ; PL: lg'SaLM : [Hgf. 153): 1+ («£20621
. (Zia>06) ._ WW“ 7;: (Lro46‘i>CZC\3> : [1%S’}W (warn: 3:] ‘h Wear ShuntTom) we COM Cheri. wineHav
COVEM; CW5v¢aLR {om ‘noUVr Leah
ulbkaﬁdb W OHM: CamouaAJLFa vsolo‘ﬁd, (1') M do ncL MM (3‘ W P‘ so
cannch c‘nc‘ck E 5&2 N comnguﬂQw
anme haw1: bet—w U;FIO‘FCA. How
Oi‘pw)!‘ amass CTo. =“n.)? T54 = T4 (1+ \63 mg)
7'
1:” EMEHC‘ZDC‘Q} *— 5H—OH'
T01. = TLC1+ \"1\ H17")
1 _
— mo +(z)(sw)‘) » mm Tcm .3 cwwd— (maﬁa. TL; H, M 5° SMtHwib was» Irar Mara—Z) ua'hA
‘81th H,“ W TL (ﬂ m1.) owl Hal
“w ‘Fnw 1i LM‘ T15 H2 :5 she’s) 2'. . H 1.”) we could (OkiwAaJI Pc\ “(a—5%» W améwsnm 0E3 shocL.
P0; =— 19; Cl+ L H‘>3'§
1‘ 7 WW at;
P03. _ P,_(H2.H’;>3.;
t 7+ 33( 10653} 5"
s a ma. an. I002. cm...» I? ‘99:. “((13); 5ko0L vow: . at. nWm\ ‘35 Maﬁa?» M; h” .13 (2660.“ HI 9 a“ (oi/{wax at) O'HI "" qul "_"" o PI+ 01‘1‘?‘ ‘ Fiﬁ" (Dzth "—'—— g
em 69 Pln = e ——— C9
n. afaeral all: :quz — H15— Smaz :32». A? ._._ 3...; [LU
‘ C’ b? e wW __' Mat magmaMS. £0119 .,. Cjolf
I (’ km “(9 C “49739 ‘* C (050.2) —_ c le$(hL1/hf ———®
MR6) “‘1 6 " [‘35 till) ﬁzz..le 0v (obvlrlar— HF—hz? ___ B’qu
Q PGI 1 F’.]_I+~:_:H~12
7.
3"
= P. [1+(2)('5‘*)3 3
'= [53H P1 ' hawc um“ ‘31 a “Wmn‘ shoal. wane akﬁéol 6 Qua Pf “and F0“; A an.“ be? “ac CEOHQWW prPathﬂ' 3 WC
how3 clawan 3 HM 5kocL mm d. [’01. . Pea. aw M=1 W“) “ 0.3183 Fm ‘0”  me1 Pan: Ps (Ii3:} H1”) It
P61 .». PL ([+cz)(°a))3’° ~ gm P,
\ﬁﬁna Q: A .. (0 357.3%) 6 ‘7‘) P\ '7— F,\ 1' Hales G‘Do Ill3" P01/ P; '0; Wm; SulaSF\IVuE MOA reamMob}; (3‘ 1 XI :— XJ—J — \_/_1
X'l) V7. e2.
(9) P;
{y12+( {14) IF. (V+D*(Y") PUP: ...
View
Full
Document
 Spring '07
 DOLLING,D

Click to edit the document details