investigation of the potential of different lubrication...
TRANSCRIPT
Faculty of Mechanical Science and Engineering Institute of Fluid Power
Investigation of the Potential of Different
Cooling System Structures for Machine Tools
1
Axis drives 1503 kJ (45%)
Cooling system 389 kJ (12%)
Cooling lubricant system 532 kJ (16%)
Lubrication system409 kJ (12%)
Hydraulic system 126 kJ (4%)
Other 369 kJ (11%)
SFB/Transregio 96Thermo-energetic Design
of Machine Tools
QH
Q̇E
Electrical cabinet
Rotary table
Main drive
• Introduction
• Cooling system structure design
• System modelling and validation
• Potential analysis of cooling structures
• Summary & outlook
Linart ShabiInstitute of Fluid Power (IFD)
Dresden
Shabi, Linart3/19/2018
Introduction
2
Thermo-energetic Design of Machine Toolswww.transregio96.de
QualityProductivity
Efficiency
Production processes (energy losses) thermal energy
Different generated heat temperature fluctuation
Temperature variation thermo-elastic deformation
Displacement of TCP reduction of machine accuracy
Challenges
Motivation
Thermal behavior of cooling systems not analyzed in detail
Energy demand of cooling system inadequate information
Previous projects efficient components & control strategies
Main goal uniform temperature, minimal energy demand
Shabi, Linart3/19/2018
Cooling system structure design
Cooling system of DBF630
Cooling system cools three components
Centrally fixed displacement pump
Rotary table & main drive cooled directly
Cooling unit (heat sink) in the return flow
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Schematic representation of cooling system of DBF630
Shabi, Linart3/19/2018
Cooling system structure design
Cooling system of DBF630
Cooling system cools three components
Centrally fixed displacement pump
Rotary table & main drive cooled directly
Cooling unit (heat sink) in the return flow
Cooling system of DMU80
Cooling systems cools 13 components
Cooling unit (heat sink) bypass cooling
Electrical cabinet separate cooling unit
3-Way valve used as diverting valve
4
Schematic representation of cooling system of DMU80
Shabi, Linart3/19/2018
p1 p3p2 p2
Heat flow
T1
T2
T2
p2, T2
Ch, Cth
Thermal resistance:
Throttle equation:
Pressurizing equation : Temperature equation:
System modelling and validation
Methodology of the model development thermo-hydraulic network modelling
Hydraulic & thermodynamic domain laws of electrical engineering (Kirchhoff’s circuit)
5
𝛼𝑖𝑛𝑠𝑖𝑑𝑒
Thermo-hydraulic network modelling
Shabi, Linart3/19/2018
System modelling and validation
Methodology of the model development thermo-hydraulic network modelling
Hydraulic & thermodynamic domain laws of electrical engineering (Kirchhoff’s circuit)
Heat transfer at the hoses is considered
6
𝑅𝑒 =𝐷𝐻 ∙ 𝑉
𝜈 ∙ 𝐴
𝑃𝑟 =𝑐𝑓𝑙𝑢𝑖𝑑 ∙ 𝜌 ∙ 𝜈
𝜆𝑓𝑙𝑢𝑖𝑑
𝑁𝑢 = 0.0235 ∙ 𝑅𝑒0.8 − 230 ∙ 1.8 ∙ 𝑃𝑟0.3 − 0.8 ∙ [1 +𝑑𝑖
𝑙
23
]
𝛼𝑖𝑛𝑠𝑖𝑑𝑒 =𝜆𝑓𝑙𝑢𝑖𝑑 ∙ 𝑁𝑢
𝐿𝐸𝑛𝑓𝑜𝑟𝑐𝑒𝑑 𝑐𝑜𝑛𝑣𝑒𝑐𝑡𝑖𝑜𝑛
𝛼𝑐𝑜𝑛. =2 ∙ 𝜆𝑐𝑜𝑛.
𝑑𝑜 ∙ 𝑙𝑛𝑑𝑜𝑑𝑖
𝑓𝑜𝑟 𝑐𝑦𝑙𝑖𝑛𝑑𝑒𝑟 𝑠ℎ𝑎𝑝𝑒
𝛼𝑖𝑛𝑠𝑖𝑑𝑒Fluid
𝛼𝑐𝑜𝑛𝑑𝑢𝑐𝑡𝑖𝑜𝑛
𝛼𝑖𝑛𝑠𝑖𝑑𝑒 𝛼𝑐𝑜𝑛𝑑𝑢𝑐𝑡𝑖𝑜𝑛
Heat transfer mechanisms at the hose
Shabi, Linart3/19/2018
System modelling and validation
Methodology of the model development thermo-hydraulic network modelling
Hydraulic & thermodynamic domain laws of electrical engineering (Kirchhoff’s circuit)
Heat transfer at the hoses is considered
7
𝛼𝑖𝑛𝑠𝑖𝑑𝑒Fluid
𝛼𝑐𝑜𝑛𝑑𝑢𝑐𝑡𝑖𝑜𝑛
𝛼𝑖𝑛𝑠𝑖𝑑𝑒 𝛼𝑐𝑜𝑛𝑑𝑢𝑐𝑡𝑖𝑜𝑛
Heat transfer mechanisms at the hose
𝛽 =1
𝑇∞
𝐺𝑟 = 𝛽 ∙ 𝑔 ∙ 𝐷3 ∙ (𝑇𝑤 − 𝑇∞
𝜈2
𝑅𝑎 = 𝐺𝑟 ∙ 𝑃𝑟
𝑁𝑢 = 0.6 +0.387 ∙ 𝑅𝑎 1 6
1 + 0.559 𝑃 𝑟 9 16 8 27
2
𝑓𝑜𝑟 10−5 < 𝑅𝑎 < 1012
𝑎𝑛𝑑 0 < 𝑃𝑟 < ∞
𝛼𝑜𝑢𝑡𝑠𝑖𝑑𝑒 =𝜆𝑎𝑖𝑟 ∙ 𝑁𝑢
𝐿
𝛼𝑜𝑢𝑡𝑠𝑖𝑑𝑒
𝛼𝑜𝑢𝑡𝑠𝑖𝑑𝑒
Shabi, Linart3/19/2018
System modelling and validation
Methodology of the model development thermo-hydraulic network modelling
Hydraulic & thermodynamic domain laws of electrical engineering (Kirchhoff’s circuit)
Heat transfer at the hoses is considered
Developing Simulation model of the current cooling system
8
𝛼𝑖𝑛𝑠𝑖𝑑𝑒 𝛼𝑐𝑜𝑛𝑑𝑢𝑐𝑡𝑖𝑜𝑛 𝛼𝑜𝑢𝑡𝑠𝑖𝑑𝑒
Model development of cooling system in the simulation software
exemplified by DMU80Model parameters for the simulation model
Shabi, Linart3/19/2018
System modelling and validation
Measurement on the machine tools different operating processes
Validation the simulation model high accuracy of the thermal and hydraulic quantities
9
Comparison of temperature development simulation and measurement
in the idle process of DMU80
0 166 332 498 664 830
Time in s
23
24
25
26
27
Te
mp
era
ture
in
°C
0 166 332 498 664 830
Time in s
23
24
25
26
27
Te
mp
era
ture
in
°C
0 166 332 498 664 830
Time in s
27
26
25
24
23
Te
mp
era
ture
in
°C
0 166 332 498 664 830
Time in s
27
26
25
24
23
Te
mp
era
ture
in
°C
Outlet temperature measurement
Inlet temperature measurement
Outlet temperature simulation
Inlet temperature simulation
Motor spindle Drive B axis
Spindle nut Z axis Rail secondary part X axisa
b
c
d
xY
ZB
C
f
e
Inlet temperature
Outlet temperature
a) Motor spindle
b) Drives B axis
c) Spindle nut Z axis
d) Secondary part X axis
e) Pump
f) Tank
Shabi, Linart3/19/2018
Comparison of temperature development simulation and measurement
in the manufacturing process of DMU80
Outlet temperature measurement
Inlet temperature measurement
Outlet temperature simulation
Inlet temperature simulation
Motor spindle Drive B axis
Spindle nut Z axis Rail secondary part X axis
0 176 352 528 704 880
Time in s
24
25
26
27
28
Te
mp
era
ture
in
°C
0 176 352 528 704 880
Time in s
24
25
26
27
28
Te
mp
era
ture
in
°C
0 176 352 528 704 880
Time in s
24
25
26
27
28
Te
mp
era
ture
in
°C
0 176 352 528 704 880
Time in s
24
25
26
27
28
Te
mp
era
ture
in
°C
System modelling and validation
Measurement on the machine tools different operating processes
Validation the simulation model high accuracy of the thermal and hydraulic quantities
10
a
b
c
d
xY
ZB
C
f
e
Inlet temperature
Outlet temperature
a) Motor spindle
b) Drives B axis
c) Spindle nut Z axis
d) Secondary part X axis
e) Pump
f) Tank
Shabi, Linart3/19/2018
System modelling and validation
Measurement on the machine tools different operating processes
Validation the simulation model high accuracy of the thermal and hydraulic quantities
Heat transport through the hydraulic pipe 1% of cooling unit performance (4.5 kW)
11
a
b
c
d
xY
ZB
C
f
e
Inlet temperature
Outlet temperature
a) Motor spindle
b) Drives B axis
c) Spindle nut Z axis
d) Secondary part X axis
e) Pump
f) Tank
Total heat transport through the hydraulic
hoses of the DMU80
0 166 332 498 664 83042
44
46
48
He
at
flo
w in
W
Time in s
Shabi, Linart3/19/2018
Potential analysis of cooling structures
Deficit of the current cooling system structures
High energy consumption 12% DBF630, 26% DMU80 /4,12/
Investigation of cooling systems ineffectively cooling
Supplied cooling medium does not match the component demand
Pump performance does not match to thermal load
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central, variable speed drive
unit with proportional valves
1
Structure 1
Decentralized, variable
speed drive units without
flow control valves
1
Structure 2
Decentralized, variable
speed drive units, tanks
and cooling units
1
Structure 3
Developing new
cooling system
structures
Cold fluid Hot fluid Mixed fluid with predefined temperature
fixed drive unit with
constant flow valves
Current structure
Shabi, Linart3/19/2018
Potential analysis of cooling structures
Design of the new cooling system structures
Individually component-specific supply (pump or proportional valve)
Controlled cooling volume flow minimizing energy demand
Precise temperature control homogenous temperature field at the component
Reducing of displacement of TCP enhance the machine accuracy
The control compares Tactual with Tset
controlling of cooling volume flow
Each component is supplied with a different
demand-oriented cooling volume flow
Inactive pump or valve Component’s temperature
doesn’t exceed predefined limits
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Control strategy of structure 1
sensor signal
control signal
pump
actual temperature
Regelung
Electrical cabinet Rotary table
Motor spindle
Controlling
TSet
thermal connection
hydraulic connection
heat input / heat output
Thermal resistance
heat capacity
hydraulic capacity
adjusting valve
tank
Shabi, Linart3/19/2018
Structure 1Current structure Structure 2 Structure 3Structure 3
Simulation results of new cooling structures in comparison to the
current cooling structure
1500 2000 2500 3000
Heat input in W
25
26
27
28
29
Te
mp
era
ture
in
°C
150 180 210 240 270 300
Heat input in W
25
26
27
28
29
Te
mp
era
ture
in
°C
150 180 210 240 270 300
Heat input in W
25
26
27
28
29
Te
mp
era
ture
in
°C
Electrical cabinet (EC) Rotary table (RT)
Main drive (MS)
1800 2400 3000 3600
Total heat input in W
0
4
8
12
16
20
Vo
lum
e f
low
in
l/m
in
Temperature current system
system structure 1, 2, 3
system structure 1, 2, 3
system structure 1, 2, 3
current system
current system
system structure 1, 2, 3
system structure 1, 2, 3
Flow rate developments
Potential analysis of cooling structures
Potential analysis structure 1, 2, 3
Stationary behavior of cooling system
Average equivalent heat flow
New cooling structures
Different Tset
Tactual constant
Volume flow control
Lower hydraulic power
Current cooling structures
No Tset possible
Tacutal depends from heat input
Uncontrolled volume flow
Higher hydraulic power
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Cold fluid Hot fluid Mixed fluid with predefined temperature
Shabi, Linart3/19/2018
Comparison of the pumps performance in the current cooling
structure and in the new cooling structures
Current structure Structure 1 Structure 2 Structure 3
Potential analysis of cooling structures
Potential analysis structure 1, 2, 3
Stationary behavior of cooling system
Average equivalent heat flow
New cooling structures
Different Tset
Tactual constant
Volume flow control
Lower hydraulic power
Current cooling structures
No Tset possible
Tacutal depends from heat input
Uncontrolled volume flow
Higher hydraulic power
15
Cold fluid Hot fluid Mixed fluid with predefined temperature
Phydr. DBF 630 Phydr. DMU80
Phydr. Structure 1 / DBF630
Phydr. Structure 2 / DBF630
Phydr. Structure 3 / DBF630
1800 2400 3000 3600
Total heat input in W
0
80
160
240
320
400
To
tal h
yd
rau
lic p
ow
er
in W
Shabi, Linart3/19/2018
Summary and outlook
Motivation and main goal
Reducing of thermo-elastic deformation enhancing of machine accuracy
Demand-oriented cooling system uniform temperature, minimal Energy demand
Deficits of current cooling structures
Cooling systems high energy consumption (12% to 26%)
Non-matching supplied cooling medium temperature fluctuation (ΔT= 3 to 5K)
Fixed speed drive high hydraulic energy
Benefits of new cooling structures
Controlled cooling medium flow minimization of energy demand
Matching supplied cooling medium temperature difference (ΔT= 0.2 to 0.4 K)
Variable speed drive lower hydraulic energy (53% to 70.5%)
16
Shabi, Linart3/19/2018
Summary and outlook
Extension of simulation models
E-Motor, Frequency converter, etc.
Energetic evaluation of the overall system
Calculation of efficiency
Showing the energy flow paths
17
Shabi, Linart3/19/2018
Summary and outlook
Extension of simulation models
E-Motor, Frequency converter, etc.
Energetic evaluation of the overall system
Calculation of efficiency
Showing the energy flow paths
18
Shabi, Linart3/19/2018
Summary and outlook
Extension of simulation models
E-Motor, Frequency converter, etc.
Energetic evaluation of the overall system
Calculation of efficiency
Showing the energy flow paths
Development of a test rig
Practice investigation of cooling structures
Demonstrate the benefit of the structures
Experimentally sound statement
19
Shabi, Linart3/19/2018
Summary and outlook
Extension of simulation models
E-Motor, Frequency converter, etc.
Energetic evaluation of the overall system
Calculation of efficiency
Showing the energy flow paths
Development of a test rig
Practice investigation of cooling structures
Demonstrate the benefit of the structures
Experimentally sound statement
Coupling with a demonstration machine,
measurement TCP displacement
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Technische Universität Dresden | Institute of Fluid Power | Chair of Fluid-Mechatronic Systems
Prof. Dr.-Ing. J. Weber | Tel. 0351- 463 33559 | [email protected]
Faculty of Mechanical Science and Engineering Institute of Fluid Power
21
Linart Shabi - [email protected]
Supported by:
SFB/Transregio 96Thermo-energetic Design
of Machine Tools
Thank you for your attention