|
AME 436 |
Assigned: Friday
4/3/09 |
|
Problem Set #5 |
á Due Monday 4/13/09 at 4:30 pm in OHE 430J á Email to the grader (Thada Suksila,
suksila@usc.edu) or fax to 213-740-8071 if youŐre off campus á DEN students submit through the usual
channels |
For each of the following equations a) – c)
used frequently in this course, state whether or not each of the following
restrictions i) – viii) apply.
i.
Steady
ii.
one-dimensional flow
iii.
ideal gas
iv.
constant specific
heats
v.
reversible
vi.
adiabatic
vii.
no work transfer
viii.negligible change in kinetic energy
a)
Thrust
equation: T =
a[(1+FAR)ue-u1] +
(Pe-Pa)Ae
b)
Enthalpy/velocity
relation between states 1 and 2: ![]()
c)
Temperature/pressure
relation between states 1 and 2: ![]()
Problem
#2 (10 points)
Using
the Brequet range equation, estimate the range of an albatross. When estimating the heating value of
albatross food, note that 1 diet calorie = 1000 thermodynamic calories. (This question always throws students
for a loop. The point is not to
get an exact answer, but to estimate each of the terms in the Brequet range
equation, and see if the result is reasonable or not.)
Problem
#3 (20 points) (from last yearŐs final exam)

Consider a simple hypersonic propulsion system for
an aircraft at an initial Mach number of 7 that consists of two processes:
Process A: Decelerate the
incoming flow reversibly and adiabatically until the static temperature is 10
times the ambient temperature Ta
Process B: Add heat at constant
temperature until the pressure is equal to 10 times the ambient pressure
Assume air is an ideal gas with constant specific
heats, and the fuel-to-air ratio (FAR) << 1.
a)
Compute the Mach
number after deceleration (station 2)
b)
Compute the static
(not stagnation) pressure relative to Pa after deceleration (station
2)
c)
Compute the Mach
number at the exit (station 3)
d)
Compute the
non-dimensional specific thrust
e)
Compute the overall
efficiency
f)
Are the area changes
between stations 1 and 2 and between stations 2 and 3 shown in the figure
qualitatively correct? Why or why
not?
Problem #4 (20 points)
Consider a flowing gas with g = 1.4, R = 287 J/kgK, M = 3, Tt = 840K
and Pt = 36.73 atm.
a)
If there is no heat
addition but there is friction loss in a constant-area duct of length L,
diameter d, and friction coefficient Cf = 1 x 10-6, what
is the maximum L/d for which this flow can be transmitted? What is the stagnation pressure at the
end of the duct?
b)
If there is no
friction but heat is added at constant area until thermal choking (M = 1), how
much heat has been added to the gas (in J/kg)? At this condition, what is the stagnation pressure?
c)
How much heat could
be added at constant pressure (in J/kg, starting at M = 3, Tt = 840K
and Pt = 36.73 atm) before the stagnation pressure in part (b) is
reached?
d)
How much heat could
be added at constant temperature (in J/kg, starting at M = 3, Tt =
840K and Pt = 36.73 atm) before the stagnation pressure in part (b)
is reached?
Problem #5 (30 points)

Consider a very simple
propulsion system operating at a flight Mach number of 5 that consists of 2
processes:
Process
1: Shock at entrance to duct
Process
2: Heat addition in a constant-area
duct until thermal choking
occurs
a) Compute all of the following properties
of this system:
i. Static (not stagnation) temperature relative to T1
after the shock
ii. Static (not stagnation) pressure relative to P1
after the shock
iii. Static (not stagnation) temperature relative to T1
at the exit
iv. Static (not stagnation) pressure relative to P1
at the exit
v. Dimensionless heat addition {qin
divided by RT1 = CP(T3t-T2t)/RT1
= [g/(g‑1)](T3t-T2t)/T1}
vi. Specific thrust = Thrust /(
ac1) (c1 = sound speed at
ambient conditions = (gRT)1/2)
(assume FAR << 1 in the thrust calculation)
vii. Overall efficiency
viii.Draw this cycle on a T - s diagram. Include appropriate Rayleigh and Fanno
curves.
b) Repeat (a) if a nozzle is added after
station 3 that expands the flow isentropically back to P = P1.
c) Repeat (a) if there is no shock and no
nozzle (but still constant area heat addition.)
d) Repeat (a) if there is a shock followed
by constant temperature (not constant area) heat addition until the pressure is equal to
ambient pressure. (Are we having
fun yet?)
e) Answer the following questions:
i.
Why
was no thrust generated in parts (a) and (c)?
ii.
Why
did part (b) generate thrust whereas part (a) did not?
iii.
Why
did part (d) generate thrust whereas part (c) did not?
iv.
Why
was the performance of part (b) so much better than that of part (d)?