amplitude as a function of time for plucked guitarsingle-particle radial wf (r) expand in harmonic...

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1 PRÁTICAS EDUCATIVAS NO CURSO INTEGRADO DE EDIFICAÇÕES: ESTUDO DE CASO SOBRE A PRESENÇA DE LADRILHO HIDRÁULICO NO CENTRO DA CIDADE DE LAGARTO/SE Bruna Fortes Santos ¹ Rosana Rocha Siqueira ² Tamires de Lima ³ Eixo: Educação, Sociedade e práticas educativas RESUMO Este artigo relata um estudo de caso baseado em uma prática educativa do Curso Integrado de Edificações do IFS- Instituto Federal de Educação Tecnológica no Campus Lagarto/SE. A partir da abordagem de um único material construtivo o “ladrilho hidráulico”, foi possível desenvolver com os alunos da equipe de estudo um novo olhar sobre o patrimônio material e imaterial contida no mesmo. Realizou-se pesquisa qualitativa e quantitativa cujo universo foi composto por 382 do centro da cidade, sendo a amostra de 8% destes imóveis, considerando as residências com presença de ladrilho hidráulico. Observou-se que a preservação do ladrilho hidráulico na área em estudo, não está sendo realizada. Percebe a importância de manter vivo este saber tradicional, que se traduz em patrimônio material e imaterial e que pode vir a ajudar a preservar a memória arquitetônica de várias regiões do Brasil. Palavras-chaves: Práticas educativas, edificações, ladrilho RESUMEN Este artículo presenta un estudio de caso sobre la base de una práctica educativa de las construcciones Curso Integrado de IFS-Instituto Federal de Educación Técnica Campus Lagarto / SE. Desde el enfoque de un único material de construcción " baldosa hidráulica, fue posible desarrollar equipo de los alumnos estudian una nueva mirada sobre el patrimonio material e inmaterial. Llevamos a cabo la investigación cuantitativa y cualitativa cuyo universo estuvo constituido por 382 del centro de la ciudad, con una muestra de 8% de estos edificios, teniendo en cuenta la presencia de hogares con baldosa hidráulica. Se observó que la preservación de baldosa hidráulica en el área de estudio, no se está realizando. Se da cuenta de la importancia de mantener vivo el conocimiento tradicional, que puede ayudar a preservar la arquitectura de memoria de varias regiones de Brasil.

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Page 1: Amplitude as a function of time for plucked guitarSingle-particle radial wf (r) Expand in harmonic oscillator wfs: N max (r) = NX max =0 c ˚ (r) Find c s by diagonalizing Hb = E Extend

Recasting a problem in Fourier space

Amplitude as a function of time for plucked guitar:

Same information is contained in amplitude of frequencies

Page 2: Amplitude as a function of time for plucked guitarSingle-particle radial wf (r) Expand in harmonic oscillator wfs: N max (r) = NX max =0 c ˚ (r) Find c s by diagonalizing Hb = E Extend
Page 3: Amplitude as a function of time for plucked guitarSingle-particle radial wf (r) Expand in harmonic oscillator wfs: N max (r) = NX max =0 c ˚ (r) Find c s by diagonalizing Hb = E Extend

Energy by adding up frequencies/wavelengths

Describe energy by where particle is and how fast it is movingor by adding up energy in each wavelength given thedistribution of wavelengths

Page 4: Amplitude as a function of time for plucked guitarSingle-particle radial wf (r) Expand in harmonic oscillator wfs: N max (r) = NX max =0 c ˚ (r) Find c s by diagonalizing Hb = E Extend

2D Fourier transforms of images

Page 5: Amplitude as a function of time for plucked guitarSingle-particle radial wf (r) Expand in harmonic oscillator wfs: N max (r) = NX max =0 c ˚ (r) Find c s by diagonalizing Hb = E Extend

Expanding wave functions in an HO basis

Single-particle radial wf ψ(r)

Expand in harmonic oscillator wfs:

ψNmax (r) =

Nmax∑α=0

cαφα(r)

Find cαs by diagonalizing HΨ = EΨ

Extend to many-body system

Out[532]=

0.5 1.0 1.5 2.0 2.5r

-5

5

10

15V@rD

Eexact'=')1.51'

ψexact(r), ψ0(r), 0.5 ∗ φ0 ψexact(r), ψ0(r), 0.5 ∗ φ0

Out[476]=

0.5 1.0 1.5 2.0 2.5r

-0.5

0.5

1.0

1.5

2.0

2.5

wf

0.5 1.0 1.5 2.0 2.5r

-0.5

0.5

1.0

1.5

2.0

2.5

wf

Nmax = 0, E0 = −1.30 Nmax = 0, E0 = +5.23

Page 6: Amplitude as a function of time for plucked guitarSingle-particle radial wf (r) Expand in harmonic oscillator wfs: N max (r) = NX max =0 c ˚ (r) Find c s by diagonalizing Hb = E Extend

Expanding wave functions in an HO basis

Single-particle radial wf ψ(r)

Expand in harmonic oscillator wfs:

ψNmax (r) =

Nmax∑α=0

cαφα(r)

Find cαs by diagonalizing HΨ = EΨ

Extend to many-body system

Out[532]=

0.5 1.0 1.5 2.0 2.5r

-5

5

10

15V@rD

Eexact'=')1.51'

ψexact(r), ψ2(r), 0.5 ∗ φ2 ψexact(r), ψ2(r), 0.5 ∗ φ2

Out[480]=

0.5 1.0 1.5 2.0 2.5r

-0.5

0.5

1.0

1.5

2.0

2.5

wf

0.5 1.0 1.5 2.0 2.5r

-0.5

0.5

1.0

1.5

2.0

2.5

wf

Nmax = 2, E2 = −1.46 Nmax = 2, E2 = −0.87

Page 7: Amplitude as a function of time for plucked guitarSingle-particle radial wf (r) Expand in harmonic oscillator wfs: N max (r) = NX max =0 c ˚ (r) Find c s by diagonalizing Hb = E Extend

Expanding wave functions in an HO basis

Single-particle radial wf ψ(r)

Expand in harmonic oscillator wfs:

ψNmax (r) =

Nmax∑α=0

cαφα(r)

Find cαs by diagonalizing HΨ = EΨ

Extend to many-body system

Out[532]=

0.5 1.0 1.5 2.0 2.5r

-5

5

10

15V@rD

Eexact'=')1.51'

ψexact(r), ψ4(r), 0.2 ∗ φ4 ψexact(r), ψ4(r), 0.2 ∗ φ4

Out[485]=

0.5 1.0 1.5 2.0 2.5r

-0.5

0.5

1.0

1.5

2.0

2.5

wf

0.5 1.0 1.5 2.0 2.5r

-0.5

0.5

1.0

1.5

2.0

2.5

wf

Nmax = 4, E4 = −1.46 Nmax = 4, E4 = −1.04

Page 8: Amplitude as a function of time for plucked guitarSingle-particle radial wf (r) Expand in harmonic oscillator wfs: N max (r) = NX max =0 c ˚ (r) Find c s by diagonalizing Hb = E Extend

Expanding wave functions in an HO basis

Single-particle radial wf ψ(r)

Expand in harmonic oscillator wfs:

ψNmax (r) =

Nmax∑α=0

cαφα(r)

Find cαs by diagonalizing HΨ = EΨ

Extend to many-body system

Out[532]=

0.5 1.0 1.5 2.0 2.5r

-5

5

10

15V@rD

Eexact'=')1.51'

ψexact(r), ψ6(r), 0.2 ∗ φ6 ψexact(r), ψ6(r), 0.2 ∗ φ6

Out[489]=

0.5 1.0 1.5 2.0 2.5r

-0.5

0.5

1.0

1.5

2.0

2.5

wf

0.5 1.0 1.5 2.0 2.5r

-0.5

0.5

1.0

1.5

2.0

2.5

wf

Nmax = 6, E6 = −1.50 Nmax = 6, E6 = −1.40

Page 9: Amplitude as a function of time for plucked guitarSingle-particle radial wf (r) Expand in harmonic oscillator wfs: N max (r) = NX max =0 c ˚ (r) Find c s by diagonalizing Hb = E Extend

Expanding wave functions in an HO basis

Single-particle radial wf ψ(r)

Expand in harmonic oscillator wfs:

ψNmax (r) =

Nmax∑α=0

cαφα(r)

Find cαs by diagonalizing HΨ = EΨ

Extend to many-body system

Out[532]=

0.5 1.0 1.5 2.0 2.5r

-5

5

10

15V@rD

Eexact'=')1.51'

ψexact(r), ψ8(r), 0.2 ∗ φ8 ψexact(r), ψ8(r), 0.2 ∗ φ8

Out[493]=

0.5 1.0 1.5 2.0 2.5r

-0.5

0.5

1.0

1.5

2.0

2.5

wf

0.5 1.0 1.5 2.0 2.5r

-0.5

0.5

1.0

1.5

2.0

2.5

wf

Nmax = 8, E8 = −1.50 Nmax = 8, E8 = −1.43