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April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
//// Sapienza and DTU workshopSapienza and DTU workshop ////
Sapienza University of RomeSapienza University of Rome,, School of EngineeringSchool of Engineering,, AprilApril 11 201511 2015
Structural optimization in parametricsStructural optimization in parametrics
Optimal lines on free-form surfacesOptimal lines on free-form surfaces
IntroductionIntroduction
Konstantinos GkoumasKonstantinos Gkoumas
StroNGER srl co-founder and partnerStroNGER srl co-founder and partner
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
THE UNIVERSITY
• Founded in 1303 by Pope Boniface
• 63 Departments
• 11 Faculties
• 2 University Hospitals
• 154 Bachelor courses
• 120 Master courses
• 243 Prof. Master courses
• 86 PhD courses
• 128,963 students
• 3997 Professors (including
assistant-associate)
• 914 International agreements
• 20 double degrees
• 100 visiting professors
• 183 FP7 programs in 2007-2013
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
THE FACULTY OF CIVIL AND INDUSTRIAL
ENGINEERING
• Founded in 1817
by Pope Pius VII
• In 1935, the
School became
the Faculty of
Engineering
• Nowadays:
“Faculty of Civil
and Industrial
Engineering”
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
THE ST. PETER IN CHAINS
BASILICA
• first rebuilt on
older foundations
in 432–440 to
house the relic of
the chains that
bound Saint Peter
• It houses
Michelangelo's
Moses statue
(completed in
1515)
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
THE ST. PETER IN CHAINS
BASILICA
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
THE CLOISTER
Giuliano da Sangallo
15th century
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
THE CLOISTER
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
THE CLOISTER
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
THE CLOISTER
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
THE GROUP OF STRUCTURAL ANALYSIS AND
DESIGN
Franco Bontempi, PhD
Prof. of Structural Analysis and Design
Sapienza University of Rome
Str
o N
GER
www.stronger2012.com
Academic research Industry research - R&D
University courses Professional courses
Big group Small group
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
THE GROUP OF STRUCTURAL ANALYSIS AND
DESIGN
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
THE TECHNICAL UNIVERSITY OF
DENMARK
• Founded in 1829
• Today ranked among
Europe's leading
engineering institutions
• Academic staff: 2,003
• Administrative staff: 1,540
• Students: 11,190
• Undergraduates: 6,803
• Doctoral students:1,200
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
VANKE PAVILION
RAMBOLL Computational Design
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
VANKE PAVILION
RAMBOLL Computational Design
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
VANKE PAVILION
RAMBOLL Computational Design
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
VANKE PAVILION
RAMBOLL Computational Design
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
WORKSHOP PROGRAM OUTLINE
09.15-09.45 Introduction: the Pierluigi Nervi inspiration Konstantinos
09.45-11.15 Grasshopper introduction and exercises Salma & Kareem
11.15-11.30 Morning break
11.30-13.00 Karamba introduction and exercises
•Simple beams (cantilever and simply supported), cross
sections, loads, materials, joints / truss elements
•Introduction to 2nd order analysis, buckling modes,
eigenfrequencies
•Mesh and shell elements (importance of good mesh
qualities and exercises in shell elements)
•Shell analysis tool (force-flow, principal stress, principal
bending)
Kristjan & Mariam
13.00-14.00 Lunch break
14.00-17.00 Design exercise
•Analyze existing structure(s)
•Design of new free-form shed covering the open space
over the Sapienza Engineering Faculty Cloister
17.00-18.00 Group presentations
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
isostatic lines – Nervi’s inspiration
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
Isostatic lines define the directions of principal stress to visualize the stress
trajectories in beams and other elements. In other words, they indicate by their
direction at any point, the direction of one of the principal stresses.
Beam with isostatic lines (thick
compression lines and thin tension lines)
isostatic lines – a brief recall
Cantilever beam
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
Lines of stress within a material subject to
compressive loading graphically describing the
isostatic lines around a hole – in the far right case
with a stiffer infill.
"Hole Force Lines" by Kaidor ‘Form and Forces’, by Edward
Allen and Waclaw Zalewski
isostatic lines – “force follows stiffness”
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
stress trajectory: a line showing the continuous
change in the orientation of a principal stress
throughout a body.
although trajectories may curve, their intersections
with other principal stresses remain perpendicular.
isostatic lines: stress trajectories in surfaces
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
isostatic lines: stress trajectories in surfaces
D'Aloisio, Righi, Modelli matematici per l’architettura e il calcolo numerico 2013  2014
Dr. Luca Sgambi, Politecnico di Milano
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
Considering (Arcangeli) that a 2D
continuous body subjected to normal
forces produces two families of
orthogonal curves (isostatics),
tangential to the principal bending
moment trajectories, along which
torsional moments are equal to zero.
If this continuous body is replaced by
ribs oriented along the isostatics, then
the rib structure and the continuous
body would have identical structural
behavior under identical loading and
support conditions.
isostatic lines – Nervi’s inspiration
Isostatic inspiration for the rib patterns of Nervi’s floor systems
Isostatic Ribbed Floor Slab
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
Source: Nervi, P.L., Aesthetics and Technology in Building, Harvard University Press (1965).
Each 5m x 5m slab of the Gatti Wool
Factory is supported by a central column.
All slabs are monolithically joined along the
perimeter edges.
• red lines: primary isostatics, corresponding
to the maximum principal bending moments
• blue lines: represent the secondary
isostatics, corresponding to the minimum
principal bending moments.
Gatti Wool Factory floors
Design: Nervi, Arcangeli, Cesteli Guidi
ProjectNervi:AestheticsandTechnology,Dale
Clifford,CarnegieMellonUniversity
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
C.C. Guidi e P.L.
Nervi
Lanificio Gatti Roma
1951-53 solaio a
nervature isostatiche
Gatti Wool Factory floors
Design: Nervi, Arcangeli, Cesteli Guidi
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
Gatti Wool Factory floors
Design: Nervi, Arcangeli, Cesteli Guidi
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
Source: Nervi, P.L., Aesthetics and Technology
in Building, Harvard University Press (1965).
Each 10m x 10m slab is supported by columns at the four corners and the isostatic patterns
follow one-eighth symmetry
Palace of Labor (Palazzo del Lavoro), Turin
Design: Nervi, Arcangeli, Cesteli Guidi
Source: Project Nervi - Aesthetics and Technology,
Dale Clifford, Carnegie Mellon University
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
Analogy between natural and artificial forms: in nature there is a “natural reinforcement” along the most
stresses zones
A similarity in nature (?)
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
A similarity in nature (?)
left: Wolff’s Law traces bone growth along principle stress trajectories
right: cross section of a human femur
Wolff’s Law developed the theory that bone grows in response to stress or put
another way, the internal patterning of bone is transformable and responsive to
external loading from the environment. The converse is also true, that bone will
degenerate if not subject to loading.
‘OngrowthandForm,’D.Thompson,Dover
reprintof19422nded.(1sted.,1917)1992
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
Palazzetto dello Sport di Roma
A. Vitellozzi e
P.L. Nervi
Palazzetto dello Sport
Roma 1956-57
sezioni schematiche
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
A. Vitellozzi e P.L. Nervi
Palazzetto dello Sport
Roma 1956-57
particolare del pilastro a forcella
Palazzetto dello Sport di Roma
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
Palazzetto dello Sport di Roma
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
//// Sapienza and DTU workshopSapienza and DTU workshop ////
Sapienza University of RomeSapienza University of Rome,, School of EngineeringSchool of Engineering,, AprilApril 11 201511 2015
Structural optimization in parametricsStructural optimization in parametrics
Optimal lines on free-form surfacesOptimal lines on free-form surfaces
IntroductionIntroduction
Konstantinos GkoumasKonstantinos Gkoumas
StroNGER srl co-founder and partnerStroNGER srl co-founder and partner
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
Extra slides
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
curved surfaces – tangent plane
The tangent plane to a point on a given surface, is
the plane that goes through that point and that it is
tangent to the surface at that point.
Let F(x,y,z) define a surface that is differentiable at a
point (x0,y0,z0), then the tangent plane to F(x,y,z) at
(x0 ,y0 ,z0) is the plane with normal vector: Grad
F(x0,y0,z0) that passes through the point (x0,y0,z0).
In Particular the equation of the tangent plane is:
Grad F(x0,y0,z0) .
( x - x0 , y - y0 , z - z0) = 0
All tangent lines to a point p on a surface will fall on
the tangent plane to the surface at that point.
Any curve embedded in the surface that passes
through that point will have a tangent at that point
which falls in this tangent plane.
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
curved surfaces – normal plane, principal curvatures
A normal plane at point p is one that
contains the normal vector, and will
therefore also contain a unique direction
tangent to the surface and cut the surface
in a plane curve, called normal section.
This curve will in general have different
curvatures for different normal planes at p.
The principal curvatures at p, denoted k1
and k2, are the maximum and minimum
values of this curvature, and they measure
the maximum and minimum “bending” of
the surface at that point. They are the
eigenvalues of the Hessian
The lines of curvature are curves which are
always tangent to a principal direction (they
are integral curves for the principal
direction fields).
Eigenvalues of H: k1 k2
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
curved surfaces – mean and Gaussian curvature
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
Surfaces with zero mean curvature are called
minimal surfaces.
Minimal surfaces tend to be saddle-like since
principal curvatures have equal magnitude but
opposite sign.
The saddle is also a good example of a surface with
negative Gaussian curvature.
curved surfaces – specific cases
Surfaces with zero Gaussian curvature are called
developable surfaces because they can be
“developed” or flattened out into the plane without
any stretching or tearing.
For instance, any piece of a cylinder is developable
since one of the principal curvatures is zero.
The hemisphere is one example of a
surface with positive Gaussian curvature
April 11 2015April 11 2015
Sapienza University of RomeSapienza University of Rome
School of EngineeringSchool of Engineering
curved surfaces – Gaussian curvature example surfaces
From left to right:
•a surface of negative
Gaussian curvature
(hyperboloid);
•a surface of zero
Gaussian curvature
(cylinder), and;
•a surface of positive
Gaussian curvature
(sphere).
"Gaussian curvature" by Jhausauer - English wikipedia,. Licensed under Public Domain via Wikimedia Commons -
http://commons.wikimedia.org/wiki/File:Gaussian_curvature.PNG#/media/File:Gaussian_curvature.PNG

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S[tr/c]u[c/lp]ture workshop Sapienza 11 04 2015 intro

  • 1. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering //// Sapienza and DTU workshopSapienza and DTU workshop //// Sapienza University of RomeSapienza University of Rome,, School of EngineeringSchool of Engineering,, AprilApril 11 201511 2015 Structural optimization in parametricsStructural optimization in parametrics Optimal lines on free-form surfacesOptimal lines on free-form surfaces IntroductionIntroduction Konstantinos GkoumasKonstantinos Gkoumas StroNGER srl co-founder and partnerStroNGER srl co-founder and partner
  • 2. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering
  • 3. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering THE UNIVERSITY • Founded in 1303 by Pope Boniface • 63 Departments • 11 Faculties • 2 University Hospitals • 154 Bachelor courses • 120 Master courses • 243 Prof. Master courses • 86 PhD courses • 128,963 students • 3997 Professors (including assistant-associate) • 914 International agreements • 20 double degrees • 100 visiting professors • 183 FP7 programs in 2007-2013
  • 4. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering THE FACULTY OF CIVIL AND INDUSTRIAL ENGINEERING • Founded in 1817 by Pope Pius VII • In 1935, the School became the Faculty of Engineering • Nowadays: “Faculty of Civil and Industrial Engineering”
  • 5. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering THE ST. PETER IN CHAINS BASILICA • first rebuilt on older foundations in 432–440 to house the relic of the chains that bound Saint Peter • It houses Michelangelo's Moses statue (completed in 1515)
  • 6. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering THE ST. PETER IN CHAINS BASILICA
  • 7. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering THE CLOISTER Giuliano da Sangallo 15th century
  • 8. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering THE CLOISTER
  • 9. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering THE CLOISTER
  • 10. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering THE CLOISTER
  • 11. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering THE GROUP OF STRUCTURAL ANALYSIS AND DESIGN Franco Bontempi, PhD Prof. of Structural Analysis and Design Sapienza University of Rome Str o N GER www.stronger2012.com Academic research Industry research - R&D University courses Professional courses Big group Small group
  • 12. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering THE GROUP OF STRUCTURAL ANALYSIS AND DESIGN
  • 13. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering THE TECHNICAL UNIVERSITY OF DENMARK • Founded in 1829 • Today ranked among Europe's leading engineering institutions • Academic staff: 2,003 • Administrative staff: 1,540 • Students: 11,190 • Undergraduates: 6,803 • Doctoral students:1,200
  • 14. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering VANKE PAVILION RAMBOLL Computational Design
  • 15. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering VANKE PAVILION RAMBOLL Computational Design
  • 16. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering VANKE PAVILION RAMBOLL Computational Design
  • 17. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering VANKE PAVILION RAMBOLL Computational Design
  • 18. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering WORKSHOP PROGRAM OUTLINE 09.15-09.45 Introduction: the Pierluigi Nervi inspiration Konstantinos 09.45-11.15 Grasshopper introduction and exercises Salma & Kareem 11.15-11.30 Morning break 11.30-13.00 Karamba introduction and exercises •Simple beams (cantilever and simply supported), cross sections, loads, materials, joints / truss elements •Introduction to 2nd order analysis, buckling modes, eigenfrequencies •Mesh and shell elements (importance of good mesh qualities and exercises in shell elements) •Shell analysis tool (force-flow, principal stress, principal bending) Kristjan & Mariam 13.00-14.00 Lunch break 14.00-17.00 Design exercise •Analyze existing structure(s) •Design of new free-form shed covering the open space over the Sapienza Engineering Faculty Cloister 17.00-18.00 Group presentations
  • 19. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering isostatic lines – Nervi’s inspiration
  • 20. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering Isostatic lines define the directions of principal stress to visualize the stress trajectories in beams and other elements. In other words, they indicate by their direction at any point, the direction of one of the principal stresses. Beam with isostatic lines (thick compression lines and thin tension lines) isostatic lines – a brief recall Cantilever beam
  • 21. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering Lines of stress within a material subject to compressive loading graphically describing the isostatic lines around a hole – in the far right case with a stiffer infill. "Hole Force Lines" by Kaidor ‘Form and Forces’, by Edward Allen and Waclaw Zalewski isostatic lines – “force follows stiffness”
  • 22. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering stress trajectory: a line showing the continuous change in the orientation of a principal stress throughout a body. although trajectories may curve, their intersections with other principal stresses remain perpendicular. isostatic lines: stress trajectories in surfaces
  • 23. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering isostatic lines: stress trajectories in surfaces D'Aloisio, Righi, Modelli matematici per l’architettura e il calcolo numerico 2013 2014 Dr. Luca Sgambi, Politecnico di Milano
  • 24. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering Considering (Arcangeli) that a 2D continuous body subjected to normal forces produces two families of orthogonal curves (isostatics), tangential to the principal bending moment trajectories, along which torsional moments are equal to zero. If this continuous body is replaced by ribs oriented along the isostatics, then the rib structure and the continuous body would have identical structural behavior under identical loading and support conditions. isostatic lines – Nervi’s inspiration Isostatic inspiration for the rib patterns of Nervi’s floor systems Isostatic Ribbed Floor Slab
  • 25. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering Source: Nervi, P.L., Aesthetics and Technology in Building, Harvard University Press (1965). Each 5m x 5m slab of the Gatti Wool Factory is supported by a central column. All slabs are monolithically joined along the perimeter edges. • red lines: primary isostatics, corresponding to the maximum principal bending moments • blue lines: represent the secondary isostatics, corresponding to the minimum principal bending moments. Gatti Wool Factory floors Design: Nervi, Arcangeli, Cesteli Guidi ProjectNervi:AestheticsandTechnology,Dale Clifford,CarnegieMellonUniversity
  • 26. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering C.C. Guidi e P.L. Nervi Lanificio Gatti Roma 1951-53 solaio a nervature isostatiche Gatti Wool Factory floors Design: Nervi, Arcangeli, Cesteli Guidi
  • 27. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering Gatti Wool Factory floors Design: Nervi, Arcangeli, Cesteli Guidi
  • 28. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering Source: Nervi, P.L., Aesthetics and Technology in Building, Harvard University Press (1965). Each 10m x 10m slab is supported by columns at the four corners and the isostatic patterns follow one-eighth symmetry Palace of Labor (Palazzo del Lavoro), Turin Design: Nervi, Arcangeli, Cesteli Guidi Source: Project Nervi - Aesthetics and Technology, Dale Clifford, Carnegie Mellon University
  • 29. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering Analogy between natural and artificial forms: in nature there is a “natural reinforcement” along the most stresses zones A similarity in nature (?)
  • 30. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering A similarity in nature (?) left: Wolff’s Law traces bone growth along principle stress trajectories right: cross section of a human femur Wolff’s Law developed the theory that bone grows in response to stress or put another way, the internal patterning of bone is transformable and responsive to external loading from the environment. The converse is also true, that bone will degenerate if not subject to loading. ‘OngrowthandForm,’D.Thompson,Dover reprintof19422nded.(1sted.,1917)1992
  • 31. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering Palazzetto dello Sport di Roma A. Vitellozzi e P.L. Nervi Palazzetto dello Sport Roma 1956-57 sezioni schematiche
  • 32. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering A. Vitellozzi e P.L. Nervi Palazzetto dello Sport Roma 1956-57 particolare del pilastro a forcella Palazzetto dello Sport di Roma
  • 33. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering Palazzetto dello Sport di Roma
  • 34. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering //// Sapienza and DTU workshopSapienza and DTU workshop //// Sapienza University of RomeSapienza University of Rome,, School of EngineeringSchool of Engineering,, AprilApril 11 201511 2015 Structural optimization in parametricsStructural optimization in parametrics Optimal lines on free-form surfacesOptimal lines on free-form surfaces IntroductionIntroduction Konstantinos GkoumasKonstantinos Gkoumas StroNGER srl co-founder and partnerStroNGER srl co-founder and partner
  • 35. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering Extra slides
  • 36. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering curved surfaces – tangent plane The tangent plane to a point on a given surface, is the plane that goes through that point and that it is tangent to the surface at that point. Let F(x,y,z) define a surface that is differentiable at a point (x0,y0,z0), then the tangent plane to F(x,y,z) at (x0 ,y0 ,z0) is the plane with normal vector: Grad F(x0,y0,z0) that passes through the point (x0,y0,z0). In Particular the equation of the tangent plane is: Grad F(x0,y0,z0) . ( x - x0 , y - y0 , z - z0) = 0 All tangent lines to a point p on a surface will fall on the tangent plane to the surface at that point. Any curve embedded in the surface that passes through that point will have a tangent at that point which falls in this tangent plane.
  • 37. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering curved surfaces – normal plane, principal curvatures A normal plane at point p is one that contains the normal vector, and will therefore also contain a unique direction tangent to the surface and cut the surface in a plane curve, called normal section. This curve will in general have different curvatures for different normal planes at p. The principal curvatures at p, denoted k1 and k2, are the maximum and minimum values of this curvature, and they measure the maximum and minimum “bending” of the surface at that point. They are the eigenvalues of the Hessian The lines of curvature are curves which are always tangent to a principal direction (they are integral curves for the principal direction fields). Eigenvalues of H: k1 k2
  • 38. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering curved surfaces – mean and Gaussian curvature
  • 39. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering Surfaces with zero mean curvature are called minimal surfaces. Minimal surfaces tend to be saddle-like since principal curvatures have equal magnitude but opposite sign. The saddle is also a good example of a surface with negative Gaussian curvature. curved surfaces – specific cases Surfaces with zero Gaussian curvature are called developable surfaces because they can be “developed” or flattened out into the plane without any stretching or tearing. For instance, any piece of a cylinder is developable since one of the principal curvatures is zero. The hemisphere is one example of a surface with positive Gaussian curvature
  • 40. April 11 2015April 11 2015 Sapienza University of RomeSapienza University of Rome School of EngineeringSchool of Engineering curved surfaces – Gaussian curvature example surfaces From left to right: •a surface of negative Gaussian curvature (hyperboloid); •a surface of zero Gaussian curvature (cylinder), and; •a surface of positive Gaussian curvature (sphere). "Gaussian curvature" by Jhausauer - English wikipedia,. Licensed under Public Domain via Wikimedia Commons - http://commons.wikimedia.org/wiki/File:Gaussian_curvature.PNG#/media/File:Gaussian_curvature.PNG

Editor's Notes

  1. Giuliano da Sangallo 15th century Adjacent St Peter in Chains Basilica
  2. Giuliano da Sangallo 15th century Adjacent St Peter in Chains Basilica
  3. Giuliano da Sangallo 15th century Adjacent St Peter in Chains Basilica
  4. Daniel Liebskind Twisted surface
  5. The workshop focuses on space structures, and is greatly inspired by structural forms for roofs and floors by Pierluigi Nervi. In particular the way Nervi used
  6. A simple recal on isostatic lines. Focusing on the stresses in a structural element, in this case a simple supported beam, or a cantilever, Isostatic lines define the direction of the principal stresses.
  7. A simple recal on isostatic lines. Focusing on the stresses in a structural element, in this case a simple supported beam, or a cantilever, Isostatic lines define the direction of the principal stresses.
  8. Nervi laid out it’s concrete ribs along isostatic lines, which put the greatest bending resistance at the point of maximum moment while visually expressing the flow of forces through the slab and toward the column.
  9. Grad: vector with first partial derivates