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1. https://www.youtube.com/watch?v=FzCsDVfPQqk
2. https://videos.cern.ch/record/1753412
3. https://www.eso.org/public/videos/alma16-8mm-tafreshi/
4. https://www.ligo.caltech.edu/page/vibration-isolation
[K]
Carlo Zanoni, KES lecture
1. Role of Engineers
2. Basic Concepts
1. Elasticity and structures
2. Mechanisms
3. Vibrations
4. Heat Transfer
5. Manufacturing
3. Tools
4. Examples
Outline
3
Carlo Zanoni, KES lecture
Engineering
Engineering
Civil
Engineering
Mechanical
Engineering
Electrical
Engineering
Automotive
AerospaceStructures
….
Engineering is the use of scientific principles to design and build
machines, structures, and other things, including bridges, roads, vehicles,
and buildings.https://dictionary.cambridge.org/dictionary/english/ Cambridge Academic Content Dictionary © Cambridge University
4
Management
Carlo Zanoni, KES lecture
Mechanical Engineering
Engineering is the use of scientific principles to design and build
machines, structures, and other things, including bridges, roads, vehicles,
and buildings.https://dictionary.cambridge.org/dictionary/english/ Cambridge Academic Content Dictionary © Cambridge University
Mechanical Engineering is the study of objects and systems in motion.
The role of a Mechanical Engineer is to take a product from an idea to the
marketplace. To accomplish this, the Mechanical Engineer must be able
to determine the forces and thermal environment that a product will
encounter.https://me.columbia.edu/what-mechanical-engineering
5
DesignStructures, vibrations,
dynamics, heat transfer and thermodynamics,
electromagnetics, optics…
ManufacturingTesting AIV
Carlo Zanoni, KES lecture
❖Translate a scientific dream into a reality
Role of Engineers
1. Phase 0 Mission analysis and
identification
2. Phase A Feasibility
3. Phase B Preliminary Definition
4. Phase C Detailed Definition
5. Phase D Qualification and Production
6. Phase E Utilization
7. Phase F Disposal
[ESA mission lifetime cycle]
Scientific
requirements
Technical
requirements
Design
Manufacturing,
AIV,
Commissioning
7
Feasibility
check
Carlo Zanoni, KES lecture
ElasticityBasic
Concepts
𝐹 = 𝑘 ∆𝑥
𝐹 = 𝑘 ∆𝑥
𝜎 = 𝐸 𝜀
8
Carlo Zanoni, KES lecture
ElasticityBasic
Concepts
• 𝜎: stress [Pa]
• 𝜀: strain [-]
• 𝐸:Young’s modulus or Elastic modulus [Pa]
https://www.youtube.com/watch?v=4PbdRgyW0uI9
• 𝜎: stress [Pa]
• 𝜀: strain [-]
• 𝐸:Young’s modulus or Elastic modulus [Pa]
Carlo Zanoni, KES lecture
ElasticityBasic
Concepts
Slope = E
End of elastic regime (yield)
Plastic regime (deformation
is permanent)
W.D.Callister “Material Science and
Engineering: an Introduction” 2013
10
Carlo Zanoni, KES lecture
ElasticityBasic
Concepts
Elastic regime: deformation is not permanent and is recovered once
the load is removed. It mostly follows a linear behavior
Plastic regime: deformation is permanent, when a load is removed
the shape is different from the original one
Brittle → limited
deformation possible
Ductile → large
deformation possibleGlass
Steel
11
Carlo Zanoni, KES lecture
ElasticityBasic
Concepts
Reality is a bit more complex…
Stress is not a scalar value
Infinitesimal volumes have 9 components of stress
➢ 3×3 matrix
➢ Symmetric → 3 normal stresses, 𝜎, and 3 shear stresses, 𝜏
12
Is there a way to estimate an equivalent value from the 3×3 matrix?
Yes. There are theories that derive an equivalent stress from a tri-axial stress
state.
Most used is Von Mises:
Carlo Zanoni, KES lecture
ElasticityBasic
Concepts
13
What is an acceptable level of equivalent stress (aka strength) for a part?
It depends on the material.
For most applications, the strength is the elastic limit. This also assures the
problems can be solved with linear equations.
Carlo Zanoni, KES lecture
ElasticityBasic
Concepts
Yield
@300 K
[MPa]
Rupture
@300 K
[MPa]
Steel, structural ASTM A36 steel 250 400–550
Steel S355 355 470-630
Steel, 2800 Maraging steel 2617 2693
Steel, high strength alloy ASTM A514 690 760
Polypropylene 4–369 9–80
Cast iron 4.5% C, ASTM A-48 130 200
Beryllium 99.9% Be 345 448
Aluminium alloy 2014-T6 414 483
Aluminium alloy 6061-T6 241 300
Copper 99.9% Cu 70 220
Brass 200 500
Tungsten 750 980
Titanium alloy, Ti-6Al-4V 880 900
J. Ekin “Experimental Techniques for Low -Temperature Measurements: Cryostat Design,
Material Properties and Superconductor Critical-Current Testing” 200614
Carlo Zanoni, KES lecture
Reality is even a bit more complex…
StructuresBasic
Concepts
Need of calculating everywhere in the
structure the stress due to various
loads:
• Gravity
• Earthquakes
• Wind
• Temperature
15
Carlo Zanoni, KES lecture
Idealization of structures, with ideal constraints blocking specific
degrees of freedom (dof):
StructuresBasic
Concepts
1 dof – y translation
2 dof – y translation
– x translation
2 dof – y translation
– rotation
3 dof – y translation
– x translation
– rotation
16
Carlo Zanoni, KES lecture
Idealization of structures, with ideal constraints blocking specific degrees
of freedom (dof)
Equilibrium equations (σ𝐹 = 0 and σ𝑀 = 0) for the whole structure and
single beams allow the calculations of internal actions everywhere.• Solution of 3D complex structures relies on the use of computer codes.
Euler-Bernoulli equation relates local bending moment (𝑀) to
displacements (𝑤):
𝑑2𝑤
𝑑𝑥2= −
𝑀(𝑥)
𝐸𝐼
StructuresBasic
Concepts
17
Reality is even more complex than this…
Carlo Zanoni, KES lecture
MechanismsBasic
Concepts
For a mechanism, stress is not a
sufficient design quantity.
Need of calculating multiplication
of displacements/rotations and of
forces/moments.
This is done by means of properly
derived equations of motion, so
called kinematic chains, the
principle of virtual work and other
tools.
18
M2 Hexapod
➢ The Hexapod or Stewart platform is the mechanism supporting most of mirrors
that need rigid body motion
Carlo Zanoni, KES lecture
MechanismsExample
19
METIS chopper mechanism
Carlo Zanoni, KES lecture
MechanismsExample
20
Carlo Zanoni, KES lecture
▪ All mechanical systems vibrate (they are elastic and have mass) due to seismic
noise of the ground, wind, motion of mechanisms…
• Small vibrations → displacements and deformations, reduction of life of components• Displacement and deformations of mirrors is a killer for a telescope
• Large vibrations (e.g. earthquake) → rupture
▪ Vibrations are analyzed in the frequency domain
VibrationsBasic
Concepts
𝑚 ሷ𝑥 = 𝑘 𝑦 − 𝑥 + 𝑐( ሶ𝑦 − ሶ𝑥)𝑚 ሷ𝑥 + 𝑐 ሶ𝑥 + 𝑘𝑥 = 𝑐 ሶ𝑦 + 𝑘𝑦
⋮𝑋(𝜔)
𝑌(𝜔)=
𝑐 𝑖𝜔 + 𝑘
−𝑚 𝜔2 + 𝑐 𝑖𝜔 + 𝑘
=2𝜁𝜔𝑛 𝑖𝜔 + 𝜔𝑛
2
−𝜔2 + 2𝜁𝜔𝑛 𝑖𝜔 + 𝜔𝑛2
1. Make a model of the system 2. Write motion equations(for complex cases numerical models
are used)
3. Derive transfer function(for verification purposes: measure)
S.S. Rao “Mechanical Vibrations” 2010 21
Pre-focal Station (PFS)
➢ Distributes the optical beam to the
instruments
➢ Contains sky metrology used by the
active optics of the telescope
Carlo Zanoni, KES lecture
VibrationsExample
M6N
M6C22
The PFS is required to provide a focal
position with M6N and M6C with a stability
better than 1 μm in [1,100] Hz
Seismic noise, wind and mechanisms
motion shake the structure
Transfer Functions are optimized to
minimize resonance effects
➢ Use of isolators/dampers if needed
Carlo Zanoni, KES lecture
VibrationsExample
23
Carlo Zanoni, KES lecture
Heat TransferBasic
Concepts
Conductivity
𝑞 = −𝜆∇𝑇
𝜆 thermal conductivity [W m-1 K-1]
𝑞 heat flux [W m-2]
∇𝑇 temperature gradient [K m-1]
0
300
600
900
1200
1500
1800
0 50 100 150 200 250 300
λ [W
m-1
K-1
]
T [K]
Conductivity (Cu)
Convection
𝑞 = ℎ𝐴(𝑇𝑓 − 𝑇)
ℎ convection coefficient [W m-2 K-1]
𝑞 heat flux [W m-2]
A area [m2]
𝑇 local surface temperature [K]
𝑇𝑓 fluid temperature [K]
Estimation of the convection coefficient
is very hard as it depends strongly on
the specific problem.
ℎ~𝑁𝑢 𝜆
𝐿𝑁𝑢 = 0.023 𝑅𝑒0.8𝑃𝑟0.4
Where Re and Pr are a-dimensional
numbers (Reynolds, Prandtl)
Thermal Radiation
𝑞 = 𝜀 𝜎 𝐴(𝑇14 − 𝑇2
4)
𝜎 Boltzmann constant,
5.67038×10-8 [W m-2 K-4]
𝜀 emissivity
𝑞 heat flux [W m-2]
A area [m2]
𝑇1 temperature ambient [K]
𝑇2 temperature surface [K]
When heat is exchanged between two
surfaces, the above relationship
becomes more complex because of the
view factors between the surfaces.
Emissivity, 𝜀, is very dependent on the
surface quality of the material, which
makes it hard to estimate a priori.
24
Thermal Contact Resistance
[W/K]
Key for estimating temperature distribution and power needed to keep cool/warm
Carlo Zanoni, KES lecture
ManufacturingBasic
Concepts
Forging
27
https://www.youtube.com/watch?v=Lqf-vJKs-28
Carlo Zanoni, KES lecture
ManufacturingBasic
Concepts
Turning
28
https://www.youtube.com/watch?v=MwgobIVj4fU
Carlo Zanoni, KES lecture
ManufacturingBasic
Concepts
Milling
29
https://www.youtube.com/watch?v=h74HO5ltd_o
Carlo Zanoni, KES lecture
ManufacturingBasic
Concepts
Each manufacturing process has a typical range of tolerances (i.e. dimensional and geometrical
deviations from nominal geometry). These tolerances are key aspects when drafting realistic
scientific and technical requirements.
forging→
30
http://www2.mae.ufl.edu/designlab/Lab%20Assignments/EML2322L-Tolerances.pdf
Example
MESH:
Deformation:
(enhanced)
Stress:
Carlo Zanoni, KES lecture
Finite ElementsTools
31
Motivation & Principle
• Problems often complex due to their
uniqueness (e.g. geometry)
• Analytical techniques available only
for simple cases
• Numerical tools developed (and now
implemented in professional very
expensive software packages)
• The PDE of the elastic
theory/Fourier law/… are substituted
by a set of algebraic equations
elements nodes
Carlo Zanoni, KES lecture
StandardsTools
Loads and material properties have a statistical distribution
➢ Material could be weaker than expected
➢ Loads could be higher than planned
32
Failures can cause deaths, injuries and/or
economic losses (that includes a stop to an experiment)
The loads are multiplied by certain factors and
the material strength is divided. Margin
Factors
For common applications margin factors are
prescribed by National or International norms.
In some cases, norms have the status of laws
EN 13445-8:
Unfired pressure vessels - Part 8:Additional requirements for pressurevessels of aluminium and aluminium
alloys
Carlo Zanoni, KES lecture
RF Crab CavitiesExamples
33
https://videos.cern.ch/record/2621681
Carlo Zanoni, KES lecture
RF Crab Cavities
34
RF equipment has very tight requirements (pressure,
magnetic fields, thermal losses, vibrations…)
On top of that, fabricating such a shape is very
challenging:
• tolerances requested are ~100 μm
• hard to access the inside volume
• Niobium (not a widely used material)
• maximum cleanliness
→ test program to be able to fabricate with the
required tolerance
Process called
deep drawing
Courtesy of A. Amorim Carvalho, CERN
Examples
Carlo Zanoni, KES lecture
RF Crab CavitiesExamples
35
Subjects touched:
• Elasticity and materials
• Structural mechanics
• Mechanisms
• Vibrations
• Heat Transfer
• Manufacturing
• Finite Elements
• Standards
Time for questions…!