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Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan [email protected] IREM of Toulouse Time 2012 July 10/14 2012 Tartu, ESTONIA
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Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan [email protected] IREM of Toulouse Time 2012 July 10/14 2012.

Dec 13, 2015

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Page 1: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

Representations of Solids and Surfaces Within the TI N’Spire

Environment

Jean-Jacques [email protected]

IREM of Toulouse

Time 2012 July 10/14 2012

Tartu, ESTONIA

Page 2: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

INTRODUCTION

Representing 3D objects in 2D with two parallel perspectives

Page 3: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

The « cavaliere » and the « military » perspectives

« Cavaliere » perspective « Military » perspective

PC.cg3 PM.cg3

Page 4: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

Theses perspectives with dynamic numbers in the « Geometry » application of TI

N’Spire

Paper1 problem 1

Page 5: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

An example of representation Circles in base planes

Paper1 problem 1

Page 6: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

Another example using dynamic numbers: Dynamic coordinates for movable points

Paper 1 problem 2

Page 7: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

PART 1 CYLINDERS and CONES

Their representations in« cavaliere » and « military »

perspectives

Page 8: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

With traces and loci

Paper1 problems 3, 4

Page 9: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

PART 2FOLDING and UNFOLDING

In « military » perspective

Page 10: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

Folding and unfolding cylindersin « military » perspective

Page 11: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

The technique

Paper1 problems 5

Page 12: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

The result

Paper1 problems 5

Page 13: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

Folding and unfolding conesin « military » perspective

Page 14: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

The model

Paper2 problem 1

Page 15: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

PART 3The experimental process of discovery with technology

Two conjectures obtained with the model of unfolding a

cone and their proofs

Page 16: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

Unfolding a cone onto half a disk

Paper2 problems 2

Page 17: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

Formal proof

Page 18: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

Evaluation of a limit of a ratio (between two angles)

Paper2 problem 3

Page 19: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

Formal proof

Page 20: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

PART 4SURFACES z = f(x,y)

Two possible approaches

Page 21: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

With the « Graphs » application of TI N’Spire

Page 22: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

Paper3 problem1

Page 23: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

Paper3 problem 2

Page 24: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

With the « 3D Graphing » tool of TI N’Spire

Page 25: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

z = sin(x)+cos(y)

z = 0

Paper3 problem 3

Page 26: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

z = sin(x)+cos(y)

z = 0

Paper3 problem 4

Page 27: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

CONCLUSIONas a new title

Dynamic numbers for a dynamic approach of 3D analytic geometry

Page 28: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

z = sin(x)- k.cos(y)

Paper3 problem 5

Page 29: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

[email protected] YouTube channel

Page 30: Representations of Solids and Surfaces Within the TI N’Spire Environment Jean-Jacques Dahan jjdahan@wanadoo.fr IREM of Toulouse Time 2012 July 10/14 2012.

I recommand you the work of:

Oysten Nordvik (Norway)About

Representations in central perspective with TI N’Spire

Go to his website