Title: Linear Motor Electromechanical Brake System Design and Actuation ENS 491492
1 Linear Motor Electromechanical Brake System
Design and ActuationENS 491/492
- Ömer Taner Sarper , 9325
- Mustafa Hakan Çakmakci , 8283
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2Outline
- Linear Motor Elevator Systems
- Aim of the Project
- Old Brake Design
- New Brake System Design
- Experimental Analysis Results
- Manufacturing Implimentation
- Conclusion
3What is Linear Motor Elevator?
- Linear Motor Elevator is mounted system in a
manner permitting motion of the entire linear
motor, including stator, through the hoistway.
4Linear Motor Elevator consists of...
- Mover
- Stator Assembly
- Magnet Assembly
- Motor Coils
- Brake Actuator
5History of Linear Motors
- 1840s, to the work of Charles Wheatstone at
King's College in London , too inefficient - US patent 1905 - inventor Alfred Zehden of
Frankfurt am Main , for driving trains or lifts - Late 1940s, professor Eric Laithwaite of
Imperial College in London, development of
thefirst full-size working model - 1980s British engineer HughPeter Kelly designed
the firsttubular linear motor - Recent Developments
6Applications of Linear Motors
- Usage with conventional rails
- Usage with monorails
- Usage with magnetic levitation
- Usage with Elevators
7Aim of the project
- To research and build a linear motor
multicar elevator - Design and manufacturing of the brake mechanism
and actuator including analysis of itself
8Old Brake Design
9Old Brake Design
10Old Brake System
- Because of the not directly grasping the
stators head of shoes, it doesnt work. - The force, which would be expected to be
conveyed to shoes entire surface, would now be
exerted on only one line on each of the this
makes the pressure on the shoes skyrocket.
11Reshaping of Old Brake System
- Modificated model of old designis grasping the
stators headdirectly hence the pressure
will be dispersed on the surface of the brake
shoes.
12New Brake System
- The bell crank consists of an Lpivoted
wherethe two arms of the Lmeet and it is used
toconvert the direction of reciprocating
movement. - Changing the length of the arms changes
the mechanical advantage (MA).
13New Brake System
14New Brake System
- The magnet attached parts caused a little
reverse and the magnet position should be
thought as between movers.
15New Brake System
16New Brake System
- Before manufacturing the Brake
- Brake grabbing 2.30 Brake releasing 4.60
- Distance the magnet can travel on linear bearing
14 - Gain 14/ (4.60-2.30) 6.087
17New Brake System
18Experimental Analysis of Brake
- FEA of the Brake Shoe (1) - Design
- FEA of the Brake Shoe (2) - Results
- FEA of the Brake Shoe (3) - Discussion
- Experimental Analysis of Shoe Link
19FEA of the Brake Shoe (1) Design
- Strength analysis of the brake shoe is done with
Finite Element Method. - Material 7075 Aluminum alloy
- Properties Yield Strength 145 MPa
Youngs Modulus 71.7 GPa Poissons Ratio
0.33 - Load on the surface is 10000 N.
Load on the part
20FEA of the Brake Shoe (2) - Results
- The results converged for 2mm-sized elements.
- The maximum stress is 12.588 MPa
- Yield strength was 145 MPa.
- Only elastic deformation.
- No fracture.
von Mises stress analysis
21FEA of the Brake Shoe (3) - Discussion
- Maximum elastic deformation 3.8 µm
- So small, can be ignored.
Displacement analysis
22Experimental Analysis of Shoe Link
- The critical part, Shoe Link,has come out of
the analysis,chosen material as AISI
304Steel and it result as minimumsafety factor
4.244.
Shoe Link
23Analysis of New Stator
- Back EMF Measurements (1) - Circuits
- Back EMF Measurements (2) Programs
- Back EMF Measurements (3) Results
- Resistance and Inductance Measurement
24Back EMF Measurements (1) - Circuits
- The Back-EMF is measured for three different
cases. - Circuit 1 and 2 are when the motor is being
driven. - Circuit 3 is when all the coils are open.
Circuit 1
Circuit 3
25Back EMF Measurements (2) - Programs
- DSpace and MATLABs Simulink were used.
DSpace interface
Simulink Model
26Back EMF Measurements (3) - Results
- The results were normal and expected.
- The shifts betweenthe coils are clear.
Results
27Resistance and Inductance Measurement
28New Stator Measurements
- For the new stator, the coils are not
totally linear and for the electromagnetic
force analysis it is needed to be calculated - Aim to know how much clearance the new
statorscoils have and the minimaand maxima
point of thesurface levels
29New Stator Measurements (1)
30New Stator Measurements(2)
31New Stator Measurements(3)
32New Stator Measurements(4)
33Manufacturing Implimentation
34Manufacturing Implimentation
35Manufacturing Implimentation
- Gain Report (Real)
- Distance Between Shoes
- Open 7.85 mm
- Closed 3.07 mm
- Moves 4.78 mm
- Magnet Set (66)
- Open 88.38 mm
- Closed 104.02 mm
- Moves 15.64 mm
- Gain 15.64/4.78 mm
- Gain 3.272
36Manufacturing Implimentation
- Weight Report
- Total 7 Movers 30 Assembly_Parts
Brake_System - Weight
- 1 Mover 5500 gr
- 1 Assembly_Part 65 gr
- Volume
- Brake_System 1037962 mm3 1037.962 cm3
- Density
- Al 7075 2.796 gr/cm3
- Steel 8.01 gr/cm3
- Weight
- Brake_System w/o Steel Parts 2902.14 gr
- Brake_System 2950 gr
- Total 43400 gr 43.4 kg
37Conclusion
- The system gives expected outcomes, as
designed logically and with simulation. The
brake shoes grab the steel plate and with the
help of the magnetic force it releases.
38References
- Bell crank. (2009, March 11). In Wikipedia, The
Free Encyclopedia. Retrieved 2028, April 10,
2009, from http//en.wikipedia.org/w/index.php?tit
leBell_crankoldid276485040 - Sandor Markon Yasuhiro Komatsu, Akitomo Yamanaka,
Ahmet Onat, Ender Kazan, Linear Motor Coils as
Brake Actuators for Multi-Car Elevators,
ICEMS07, CDROM bildiri kitabi, 2007 - http//www.fujitec.co.jp/
39Questions?