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Integrity, Professionalism, & Entrepreneurship Pertemuan - 3 Single Degree of Freedom System Forced Vibration Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa Kegempaan Kode : CIV - 308 SKS : 3 SKS

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Page 1: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Pertemuan - 3

Single Degree of Freedom System Forced Vibration

Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa Kegempaan

Kode : CIV - 308

SKS : 3 SKS

Page 2: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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TIU : Mahasiswa dapat menjelaskan tentang teori dinamika struktur.

Mahasiswa dapat membuat model matematik dari masalah teknis yang

ada serta mencari solusinya.

TIK : Mahasiswa mampu menghitung respon struktur dengan eksitasi

harmonik dan eksitasi periodik

Page 3: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Sub Pokok Bahasan :

Eksitasi Harmonik

Eksitasi Periodik

Page 4: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Undamped SDoF Harmonic Loading The impressed force p(t) acting on the simple oscillator in

the figure is assumed to be harmonic and equal to Fo sin wt ,

where Fo is the amplitude or maximum value of the force

and its frequency w is called the exciting frequency or forcing

frequency.

k m

u(t)

p(t) = Fo sin wt

fS = ku

u(t)

Fo sin wt fI(t) = mü

Page 5: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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The differential equation obtained by summing all the forces

in the Free Body Diagram, is :

The solution can be expresses as :

tsinFkuum o w (1)

tututu pc

Complementary Solution

uc(t)= A cos wnt + B sin wnt

Particular Solution

up(t) = U sin wt

(2)

(3.a) (3.b)

Page 6: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Substituting Eq. (3.b) into Eq. (1) gives :

Or :

Which b represents the ratio of the applied

forced frequency to the natural frequency of

vibration of the system :

oFkUUm 2w

22 1 bw

kF

mk

FU oo

nw

wb (5)

(4)

Page 7: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Combining Eq. (3.a & b) and (4) with Eq. (2) yields :

With initial conditions :

tsinkF

tsinBtcosAtu onn w

bww

21 (6)

00 uuuu

tsinkF

tsinkFu

tcosutu on

o

n

n wb

wb

b

ww

22 11

00

Transient Response Steady State Response

(7)

Page 8: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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-3

-2

-1

0

1

2

3

0 0,5 1 1,5 2 2,5 3 3,5 4

Total Response Steady State Response Transient Response

k/F

tu

o

200

0 and 00

,

k/Fuu

n

on

ww

w

Page 9: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Steady state response present because of the applied force, no matter what the initial conditions.

Transient response depends on the initial displacement and velocity.

Transient response exists even if

In which Eq. (7) specializes to

It can be seen that when the forcing frequency is equal to natural frequency (b = 1), the amplitude of the motion becomes infinitely large.

A system acted upon by an external excitation of frequency coinciding with the natural frequency is said to be at resonance.

00 0 uu

tsintsinkF

tu no wbwb

21

(8)

Page 10: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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If w = wn (b = 1), the solution of Eq. (1) becomes :

tsintcostk

Ftu nnn

o www 2

1(9)

-40

-30

-20

-10

0

10

20

30

40

0 0,5 1 1,5 2 2,5 3 3,5

p

k/F

tu

o

Page 11: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Assignment 3 If system in the figure have initial condition

And subjected to harmonic loading p(t) = 5000 sin (wt)

Plot a time history of displacement response of the system,

for t = 0 s until t = 5 s, if ξ = 0%, and :

b = 0,1 ; 0,25 ; 0,60 ; 0,90; 1,00; 1,25 & 1,75

cm/s 20 0 cm 30 u&u

40x4

0 c

m2

E= 23.500 MPa

(b)

EI ∞

W = 2,5 tons

3 m

Page 12: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Damped SDoF Harmonic Loading Including viscous damping the differential equation governing

the response of SDoF systems to harmonic loading is :

c

k

m

u(t)

p(t)

fD(t) = cú

fS(t) = ku

u(t)

Fo sin wt fI(t) = mü

tsinFkuucum o w (10)

Page 13: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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The complementary solution of Eq. (9) is :

The particular solution of Eq. (9) is :

Where :

tsinBtcosAetu DD

t

cn www

tcosDtsinCtu p ww

222

222

2

21

2

21

1

bb

b

bb

b

k

FD

k

FC

o

o

(11)

(12)

(13.a)

(13.b)

Page 14: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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The complete solution of Eq. (9) is :

tcosDtsinCtsinBtcosAetu DD

t

cn wwwww

(14)

Transient Response Steady State Response

502222

22

222

121

12

21

2

,

o

o

k

FB

k

FA

bb

bb

bb

b

Page 15: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Response of damped

system to harmonic

force with

b = 0,2,

= 0,05,

u(0) = 0,

ú(0) = wnFo/k

Page 16: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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The total response is shown by the solid line and

the steady state response by the dashed line.

The difference between the two is the transient

response, which decays exponentially with time

at a rate depending on b and .

After awhile, essentially the forced response

remains, and called steady state response

The largest deformation peak may occur before

the system has reached steady state.

Page 17: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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If w = wn (b = 1), the solution of Eq. (10) becomes :

tcostsintcose

k

Ftu nDD

to n ww

w

w

212

1 (15)

Page 18: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Considering only the steady state response, Eq. (12) & Eq.

(13.a, b), can be rewritten as :

Where :

Ratio of the steady state amplitude, U to the static deflection

ust (=Fo/k) is known as the dynamic magnification factor, D :

w tsinUtu

222 21 bb

kF

U o

21

2

b

b

tan

(16)

(17)

222 21

1

bb

stu

UD (18)

Page 19: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Page 20: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Exercise The steel frame in the figure supports

a rotating machine that exerts a

horizontal force at the girder level p(t)

= 100 sin 4 t kg. Assuming 5% of

critical damping, determine : (a) the

steady-state amplitude of vibration and

(b) the maximum dynamic stress in the

columns. Assume the girder is rigid (b)

EI ∞

W = 6,8 tons

4,5 m WF 250.125

I = 4,050 cm4

E = 205.000 MPa

Page 21: Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa ...ocw.upj.ac.id/files/Slide-CIV-308-DinamikaStr-PengRekGempa-CIV-308... · Mata Kuliah : Dinamika Struktur & Pengantar Rekayasa

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Assignment 4 If system in the figure have initial condition

And subjected to harmonic loading p(t) = 5000 sin (wt)

Plot a time history of displacement response of the system,

for t = 0 s until t = 5 s, if : ξ = 5%

cm/s 20 0 cm 30 u&u

40x40 cm2

E= 23.500 MPa

(b)

EI ∞

W = 2,5 tons

3 m

b = 0,1 ; 0,25 ; 0,60 ; 0,90; 1,00; 1,25

& 1,75