Presentation_1.ppt2. Critical Point
Input Energy
Damped Energy
Amplitude
Energy
per
cycle
Time
Amplitud
e
Classifications of Vibrations
Free Vibration
Forced Vibration
Self excited Vibration
4. Equipment Details
01 Piezoelectric accelerometer, DYTRAN: 3145AG
02 Impact hammer, DYTRAN: 5800B4
03 Electro dynamic Shaker, MB dynamics: 50A
04 Data Acquisition System, NI: 9234
05 Data Acquisition System, PHOTON+
03
02
05
04
01
Impact hammer
Accelerometer
specimen
Clamping Mechanism
8. Logarithmic decrement method
20
10
0
-10
-20
0 50 100 150 200
Acceleration,
g
Time ms
0 200 400 600 800 1000
0.8
0.6
0.4
0.2
0
Amplitude,
g
Time ms
0 50 100 150 200
40
20
0
-20
-40
Acceleration,
g
0 200 400 600 800 1000
1.8
1.2
0.6
0
Amplitude,
g
Frequency, Hz
Frequency, Hz
i) Time domain signal
i) Time domain signal
ii) Frequency domain signal ii) Frequency domain signal
680Hz
666Hz
680Hz
678Hz
664Hz
642Hz
10. 200 250 300 350 400
0.0
-1.0
-2.0
-3.0
-4.0
-5.0
A1=4.23, 294 Hz
Frequency, Hz
Imaginary
part
,
m/N
x10
-5
a) Without Excitation current
i) Real part
FRF
m/N
(10
-6
) 12
8
4
0
-4
-8
-12
Frequency Hz
400 500 600 700 800
FRF from shaker excitation test
---- Eqn (3)
---- Eqn (4)
---- Eqn (5)
---- Eqn (6)
15. To find the roots of the equation, ω1 &ω2, the
determinant of the mass-stiffness is equated to zero.
&
17. Semi Definite Systems
To find the roots of the equation, ω1 & ω2,
the determinant of the mass-stiffness is equated to zero.
m1
k
m2
X(1) X(2)