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Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

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Page 1: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Analysis of the effects of different types of loads on a Thermo-Acoustic Engine

Chitta Saha, Paul Riley and Mark Johnson

Page 2: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Presentation Outline

- Construction of the tested Thermo-acoustic Engine (TAE)

- Design issues of the low cost Alternator

- Different electrical loads with the TAE

- Power analysis for different load conditions

- Measured results

- Conclusions

Page 3: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Propane Burner TAE

• TAE consists of - Stainless steel bulge (HHX) - 30 layers stainless steel wire mesh regenerator ( 95 µm, 250 µm) - Car radiator (AHX)

• 5.5 kW propane burner, 4 inch pipe and B & C 6PS38 speaker.

• Each engine could be connected in series/parallel or independently.

Radiator

Hot buffer

tube

BulgeInsulation

Page 4: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Requirements of LA for SCORE project

• Alternator design : low cost ( £4/unit ) high efficiency and resonant frequency operation.

• Ultimate goals - Supply 12 V lead acid battery. - Generate 150 W dc power

• Small magnet constrains : (BL)2/Rc

• Meet the output power and cost : frequency & displacement

Page 5: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Limitations of Commercial low cost loudspeakers

• High suspension loss and limited mechanical stability.

• Operate over a large frequency range, LA needs to operate a fixed frequency.

• Lower efficiency and larger weight.

Cone

Voice Coil

Yoke pole pieces

Front suspension

Rear suspension

Magnet

Vent holes

Schematic of a loudspeaker type alternator

Page 6: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

SCORE Alternator : Halbach array

• Alternator can be constructed without back iron material, no yoke piece is required.

• Smaller pumping loss due to large hole.

• High Efficiency and high air-gap reversal flux density.

Page 7: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Load power and efficiency with battery circuit for 1 mm gap between coils

0

130

260

390

520

650

0 0.2 0.4 0.6 0.8 1

Ratio : Vbattery/Vp

Av

era

ge

loa

d p

ow

er

(W)

0

20

40

60

80

100E

lec

tric

al e

ffic

ien

cy

(%

)

Power : 9 mm coilPower: 7.5 mm coilPower : 6.5 mm coilPower : 5 mm coilPower : 2 mm coilEfficiency : 9 mm coil

Performance of Alternator with Battery

M

L

N

W

Double coil case 2 mm height 10 coils case

p

L

p

L

p

L

p

L

c

Leout V

V

V

V

V

V

V

V

R

VP 1

222

, cos12

• Battery with rectifier circuit :

• Electrical efficiency for dual coils : 80 % for 125 W when Vbattery/Vp = 0.73, 76 % for 150 W when Vbattery/Vp=0.7

• Max. power : Vbattery/Vp = 0.39

Page 8: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Tested prototype : Halbach array

0

1

2

3

4

5

6

7

8

0 1 2 3

Displacement (mm)

Op

en C

ircu

it p

eak

volt

age

(V)

Measured

Simulated

0

15

30

45

60

0 7 14 21 28 35Load resistance (ohm)

Eff

icie

ncy

(%

)

Acoustic-electrical efficiency

Calculated acoustic-electrical efficiency

• Measured and simulated voltages agree well.

• Discrepancy between measured and calculated efficiency appears due to cracking in the suspension.

Page 9: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Alternator power analysis

RL

Rc

+

Sin

D1

D4

D3

D2

+

Sin

Rc

+-C RL

rmsrms

T

Lc

pps IVdt

RR

tVtV

TP

)

sin)(sin(

2 2/

0

L

LLrmsL R

VRIP

2

22

- Resistive load, source power and load power :

-Battery load can be considered as a RC load when C becomes very large. - Source power and load power for battery rectifier circuit

avgbatterydcLL IVIVP **

))](sin2

1(2

[1 1

22

p

LL

Lp

cavg V

VV

VV

RI

frmsrms

LpL

p

Lp

cs

IV

VVV

V

VV

RP

])(sin1

2

1([

1 2212

Page 10: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Measured results

• Pressure and temperature has been measured using NI DAQ module.• Voltage and power has been measured using PPA2530.• Electrical power is almost proportionally varied with the square pressure.

Page 11: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Loads effect on a Thermo-Acoustic Engine

Load Condition TAE parameters Alternator

HHX (oC) HHX- AHX (oC) Pressure (mBar)

Ac voltage (Vrms)

Ac power (W)

Total power (VA)

Idc (A)(Into 12V lead acid battery)

Load power* (W)

12 V battery + capacitor +

rectifier

413 347 38 13.12 8.96 11.35 0.43 5.59

Capacitor + 30 Ω resistance +

rectifier

411 346 39 13.57 8.89 11.36 0.49 6.85

20 Ω resistance 403 343 37 13.2 8.65 8.65 - 8.65

• Bridge rectifier required a fixed load resistance to generate the same amount of real power with battery.

• No effect on pressure and temperature when the real power is constant.

• Load power is less than generated power due to losses in the rectifier.

Page 12: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Conclusions

• The construction of dual loop 30 layers stainless steel regenerator SCORE TAE is introduced.

• Design issues of SCORE LA and advantages of double Halbach array are discussed.

• Voltage/power measurement issues of the alternator with linear and non-linear load with the full wave rectifier circuit are discussed.

• Variations of the measured pressure and temperature of the engine as well as electrical power are shown.

• Measured results show, no effect on the pressure and temperature with the changing the load condition.

Page 13: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Acknowledgment

The Score project www.score.uk.com is funded by EPSRC, the UK Engineering and Physical Research Council.

Page 14: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson
Page 15: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

Specification of the regeneratorWire diameter 95 umWire spacing 250 umVolumetric Porosity: σ 0.783Solid fraction: (1-σ) 0.217Hydraulic radius 86 umRegenerator width 155 mmRegenerator length 180 mmRegenerator thickness 9 mm

𝑄𝑡ℎ𝑒𝑟𝑚𝑎𝑙 ℎ𝑒𝑎𝑡 = 𝑄𝑏𝑢𝑟𝑛𝑒𝑟 − 𝑄𝑝𝑎𝑛1+𝑝𝑎𝑛2 − 𝑄𝑐ℎ𝑖𝑚𝑛𝑒𝑦 − 𝑄ℎ𝑜𝑢𝑠𝑖𝑛𝑔 𝑊𝑎𝑐𝑜𝑢𝑠𝑡𝑖𝑐 (ℎ𝑒𝑎𝑡) = 𝑄𝑡ℎ𝑒𝑟𝑚𝑎𝑙 ℎ𝑒𝑎𝑡 − 𝑄𝑟𝑒𝑗𝑒𝑐𝑡𝑒𝑑 ℎ𝑒𝑎𝑡 − 𝑄𝑇𝐵𝑇

𝜂𝑆𝑡𝑜𝑣𝑒 = 𝑄𝑝𝑎𝑛 1+𝑝𝑎𝑛 2𝑄𝑏𝑢𝑟𝑛𝑒𝑟 × 100%

𝜂𝑇𝐴𝐸(𝑒𝑙𝑒𝑐𝑡𝑟𝑖𝑐𝑎𝑙 ) = 𝑊𝑒𝑙𝑒𝑐𝑡𝑟𝑖𝑐𝑖𝑡𝑦𝑊𝑎𝑐𝑜𝑢𝑠𝑡𝑖𝑐 (ℎ𝑒𝑎𝑡 ) × 100%

𝜂𝑇𝐴𝐸(ℎ𝑒𝑎𝑡) = 𝑊𝑎𝑐𝑜𝑢𝑠𝑡𝑖𝑐 (ℎ𝑒𝑎𝑡 ) 𝑄𝑡ℎ𝑒𝑟𝑚𝑎𝑙 ℎ𝑒𝑎𝑡 × 100%

Page 16: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson

General power/losses summary of the system

Burner (net power) 4657.71 W Rejected Heat1807.39

WEngine housing losses

519.24 W Acoustic power (Heat) 460.65 W

Heat to the Pans 1170.69 W Electricity power 15 WChimney losses 430.00 W Stove efficiency 25.13%

Heat to the TAE 2537.78 WTAE Efficiency (Heat to Acoustic power(Heat))

18.15%

TBT losses 269.74 WTAE and Generator Efficiency (Acoustic power (Heat) to Electrical power)

3.2%

Page 17: Analysis of the effects of different types of loads on a Thermo-Acoustic Engine Chitta Saha, Paul Riley and Mark Johnson