Rijke Tube Apparatus
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![Page 1: Rijke Tube Apparatus](https://reader033.fdocuments.net/reader033/viewer/2022052702/5695d4fa1a28ab9b02a38b65/html5/thumbnails/1.jpg)
The Rijke TubeInvestigating ThermoAcoustic Dynamics and Control
Bassam Bamieh
Mechanical Engineering &Center for Control, Dynamical Systems & Computation
UNIVERSITY OF CALIFORNIA AT SANTA BARBARA
SpongFest 2012, UTD
() SpongFest, Nov ’12 1 / 24
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Outline
1 The Rijke Tube Experiment, Empirically
2 ThermoAcoustic Energy Conversion
3 ThermoAcoustic Dynamics & Control
4 Optimal Periodic Control
() SpongFest, Nov ’12 2 / 24
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THE RIJKE TUBE EXPERIMENT, EMPIRICALLY
() SpongFest, Nov ’12 3 / 24
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The Rijke Tube Experiment
Observations:Heated coil induces convective flow upwardsWhen coil is sufficient hot, tube begins to hum loudly
() SpongFest, Nov ’12 4 / 24
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Observing the ThermoAcoustic Instability
vp
v
qqv =
Acoustic mode: standing wave1/2 wavelength = L
q: Heat release from coildepends on velocity fluctuations v
(convective heat transfer)
Acoustic Dynamics Coil Heat Releasev
q
TheromAcoustic Instabilities are caused by an unstable feedback betweenAcoustic Dynamics and a Flow-Dependent Heat Release Process
() SpongFest, Nov ’12 5 / 24
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Observing the ThermoAcoustic Instability
vp
v
qqv =
Acoustic mode: standing wave1/2 wavelength = L
q: Heat release from coildepends on velocity fluctuations v
(convective heat transfer)
Acoustic Dynamics Coil Heat Releasev
q
TheromAcoustic Instabilities are caused by an unstable feedback betweenAcoustic Dynamics and a Flow-Dependent Heat Release Process
() SpongFest, Nov ’12 5 / 24
![Page 7: Rijke Tube Apparatus](https://reader033.fdocuments.net/reader033/viewer/2022052702/5695d4fa1a28ab9b02a38b65/html5/thumbnails/7.jpg)
Observing the ThermoAcoustic Instability
vp
v
qqv =
Acoustic mode: standing wave1/2 wavelength = L
q: Heat release from coildepends on velocity fluctuations v
(convective heat transfer)
Acoustic Dynamics Coil Heat Releasev
q
TheromAcoustic Instabilities are caused by an unstable feedback betweenAcoustic Dynamics and a Flow-Dependent Heat Release Process
() SpongFest, Nov ’12 5 / 24
![Page 8: Rijke Tube Apparatus](https://reader033.fdocuments.net/reader033/viewer/2022052702/5695d4fa1a28ab9b02a38b65/html5/thumbnails/8.jpg)
Empirical (ID-based) Approach to the Rijke Tube
Amp
mic
speaker
heatingcoil
w
Rijke Tube
-k1k2
speaker micpre-amp/
variable amppower amp
w
With simple proportional acoustic feedback K, can stabilize this system!
0 Kfundamental mode unstable stable higher harmonic is unstable
Kmin Kmax
Observation: Which higher harmonic becomes unstable at high gain (e.g. 3’rd or 5’th, ..)depends on mic placement!
() SpongFest, Nov ’12 6 / 24
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Empirical (ID-based) Approach to the Rijke Tube
Amp
mic
speaker
heatingcoil
w
Rijke Tube
-k1k2
speaker micpre-amp/
variable amppower amp
w
With simple proportional acoustic feedback K, can stabilize this system!
0 Kfundamental mode unstable stable higher harmonic is unstable
Kmin Kmax
Observation: Which higher harmonic becomes unstable at high gain (e.g. 3’rd or 5’th, ..)depends on mic placement!
() SpongFest, Nov ’12 6 / 24
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Identification of the Rijke Tube
Rijke Tube
-k1k2
speaker micpre-amp/
variable amppower amp
w PK+w y
Identify Stabilized Closed Loop T :=PK
1− PK, K ∈ [Kmin,Kmax]
calculate P = KT
1 + TK is uncalibrated → can determined poles and zeros of P, but not OL gain
() SpongFest, Nov ’12 7 / 24
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Identification of the Rijke Tube (cont.)
Validating a frequency-fitted, finite-dimensional, open-loop Rijke Tube model
Unstable fundamental, stable higher harmonic modes
Parabolic root pattern characteristic of wave equation with Kelvin-Voigt damping
OL zero locations depend on mic location, OL poles do not
() SpongFest, Nov ’12 8 / 24
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Identification of the Rijke Tube (cont.)
Further validation: which harmonic is predicted to go unstable at high gain?
Identified model must predict particular higher harmonic instability
Changing mic location allows for repeat experimentsmicrophone position
position 4: +1 inposition 3: +1/2 inposition 2: 0 inposition 1: -1/2 in
top end of Rijke tube
() SpongFest, Nov ’12 9 / 24
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Identification of the Rijke Tube (cont.)
Further validation: which harmonic is predicted to go unstable at high gain?
Identified model must predict particular higher harmonic instability
Changing mic location allows for repeat experimentsmicrophone position
position 4: +1 inposition 3: +1/2 inposition 2: 0 inposition 1: -1/2 in
top end of Rijke tube
() SpongFest, Nov ’12 9 / 24
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The Rijke Tube as a Controls Laboratory Experiment
A versatile experiment to illustrate many important controls conceptsEasy/cheap to buildVery rich and deep (see analysis section)
cf. upcoming Control Systems Magazine article (with K. Åstörm)
() SpongFest, Nov ’12 10 / 24
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THERMOACOUSTIC ENERGY CONVERSION
() SpongFest, Nov ’12 11 / 24
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Basic Physics of the ThermoAcoustic Instability
vp
v
qqv =
Acoustic mode: standing wave1/2 wavelength = L
q: Heat release from coildepends on velocity fluctuations v
(convective heat transfer)
Acoustic Dynamics Coil Heat Releasev
q
TheromAcoustic Instabilities are caused by an unstable feedback betweenAcoustic Dynamics and a Flow-Dependent Heat Release Process
() SpongFest, Nov ’12 12 / 24
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ThermoAcoustic Engines and Heat Pumps
Stack-based systems:Temperature gradients inside acoustic cavities acoustic wave
() SpongFest, Nov ’12 13 / 24
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ThermoAcoustic Engines and Heat Pumps
Similar principle as “pulse-tube refrigerators”
() SpongFest, Nov ’12 13 / 24
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ThermoAcoustic Engines and Heat Pumps
A heat-powered refrigerator with no moving parts!
+
acoustic wave
engine heat pump
+
() SpongFest, Nov ’12 13 / 24
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ThermoAcoustic Engines and Heat Pumps
Vision:Replace traditional piston/crank/turbines with pressure/displacement waves
“The power of sound”, Garrett & Backhaus, American Scientist, 2000
Why is this not more widely known? Why hasn’t there been more progress?
() SpongFest, Nov ’12 13 / 24
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ThermoAcoustic Engines and Heat Pumps
Vision:Replace traditional piston/crank/turbines with pressure/displacement waves
“The power of sound”, Garrett & Backhaus, American Scientist, 2000
Why is this not more widely known? Why hasn’t there been more progress?
The Los Alamos Prototype:
Acoustic impedances and couplingsvery carefully designed!
Mechanical design is forone operating point!
() SpongFest, Nov ’12 13 / 24
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ThermoAcoustic Engines and Heat Pumps
Vision:Replace traditional piston/crank/turbines with pressure/displacement waves
“The power of sound”, Garrett & Backhaus, American Scientist, 2000
Why is this not more widely known? Why hasn’t there been more progress?
Acoustics need to adapt to changes in operating conditions
A delicate dance between pressure, displacement and solid/gas heat transfer with nokinematics to enforce timing
Answer: Active Control is needed!
Very little work has been done in this area“[tunable thermoacoustic cooler]", Li, Rotea, Chiu, Mongeau, Paek, ’05
() SpongFest, Nov ’12 13 / 24
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THERMOACOUSTIC DYNAMICS & CONTROL
() SpongFest, Nov ’12 14 / 24
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Acoustic & Thermal Dynamics
vp
v
qqv =
Acoustic Dynamics Velocity-dependentheat release
Acoustic Dynamics Coil Heat Releasev
q
() SpongFest, Nov ’12 15 / 24
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1d Gas Dynamics
x1 x2
Ap(x1) p(x2)
v(x2)v(x1)
x
q
Pressure form: (there’s an equivalent Temperature form)
∂
∂t
ρvp
= −
v ρ 00 v 1
ρ
0 γp v
∂xρ∂xv∂xp
+
0β v
ρ
γq
:
mass conservationmomentum balance
energy balance
A PDE in the Hamilton-Jacobi form with q as source term
Linearizations behave like Wave Equation
Point-to-point Transfer Function (non-dimensionalized)
1cosh(s/2)
q v
() SpongFest, Nov ’12 16 / 24
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1d Gas Dynamics
x1 x2
Ap(x1) p(x2)
v(x2)v(x1)
x
q
Pressure form: (there’s an equivalent Temperature form)
∂
∂t
ρvp
= −
v ρ 00 v 1
ρ
0 γp v
∂xρ∂xv∂xp
+
0β v
ρ
γq
:
mass conservationmomentum balance
energy balance
A PDE in the Hamilton-Jacobi form with q as source term
Linearizations behave like Wave Equation
Point-to-point Transfer Function (non-dimensionalized)
1cosh(s/2)
q v
() SpongFest, Nov ’12 16 / 24
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Convective Heat Transfer
Hot-wire in cross flow
qe = (Ts−T)(κd + κv
√|v|)
=: (Ts−T) f (v),
v
v
f(v)
“King’s Law” (for steady flow)
() SpongFest, Nov ’12 17 / 24
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Convective Heat Transfer (unsteady)
Hot-wire in fluctuating cross flow
Frequency response
vthermal boundary layer
Lighthill ’53
The Royal Society is collaborating with JSTOR to digitize, preserve, and extend access toProceedings of the Royal Society of London. Series A, Mathematical and Physical Sciences.
www.jstor.org®
on August 28, 2012rspa.royalsocietypublishing.orgDownloaded from
() SpongFest, Nov ’12 18 / 24
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Convective Heat Transfer (unsteady)
Hot-wire in fluctuating cross flow
Frequency response
vthermal boundary layer
Lighthill ’53Calculation of the frequency response (matched asymptotic expansions)
on August 28, 2012rspa.royalsocietypublishing.orgDownloaded from
() SpongFest, Nov ’12 18 / 24
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Convective Heat Transfer (unsteady)
Hot-wire in fluctuating cross flow
Frequency response
vthermal boundary layer
Lighthill ’53Approximate first-order lag with time delay
() SpongFest, Nov ’12 18 / 24
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Convective Heat Transfer (a simple model)
Use King’s law for heat transfer into a thermalboundary layer
Conductive heat transfer from thermal boundarylayer to bulk flow
This introduces a “thermal inertia” around wire Ts
Tb
T
Qs→bQb→f
v
Tube Wall
Thus:
1s/↵+1
f(.)qv
v
f(v)
v
() SpongFest, Nov ’12 19 / 24
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Predicting the ThermoAcoustic Instability
1cosh(s/2)
1s/↵+1
f(.)
Correct prediction of the unstable fundamental mode
() SpongFest, Nov ’12 20 / 24
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OPTIMAL PERIODIC CONTROL
() SpongFest, Nov ’12 21 / 24
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Control to Enhance Heat-to-Acoustic Power Conversion
Design control to enhance heat-to-acoustic powerconversion
Trade off control effort
Design of an engine’s “optimal limit cycle”
Details of heat transfer are probably important
Similar to problems in (periodic) motion planningWALKING ROBOTS ↔ HUMMING ENGINES
Controller
() SpongFest, Nov ’12 22 / 24
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Optimal Periodic Control
More popular in days past (’70s)(is cycling (periodic) operation better than steady (constant) operation? )
ApproachesI Periodic Boundary Value ProblemsI Flatness-based
Our current approach:Frequency domain and flatness-based method for PDE systems
Example:non-sinusoidal operation may be optimal
(“A frequency domain method for optimal periodic control”, Epperline, BB, ACC ’12)
() SpongFest, Nov ’12 23 / 24
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Optimal Periodic Control
More popular in days past (’70s)(is cycling (periodic) operation better than steady (constant) operation? )
ApproachesI Periodic Boundary Value ProblemsI Flatness-based
Our current approach:Frequency domain and flatness-based method for PDE systems
Example:non-sinusoidal operation may be optimal
(“A frequency domain method for optimal periodic control”, Epperline, BB, ACC ’12)
() SpongFest, Nov ’12 23 / 24
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Concluding Thoughts
# of times the word “thermoacoustic” appears in the ACC or CDCproceedings (all PDF files) in the past 2 years?
≈ 2-3This area deserves more attention
() SpongFest, Nov ’12 24 / 24