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Lecture 5

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36 views24 pages

Lecture 5

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s.eleslam122
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© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
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Mechanical Vibrations

(MED 343)
Lecture 5: Forced vibration of SDOF systems
(Harmonically Excited Vibration)
Dr. Mahmoud Atef
Department of Mechanical Design and Production
Engineering
2
Physical model of SDoF system

The basic components of a mechanical system are:

1- Inertia components store kinetic energy


2- Stiffness components store potential energy
3- Damping components dissipate energy
4- Energy sources provide energy to the system

11/10/2024 Mahmoud Abdalhamed.


3
Forced vibration system

• Forced vibration occurs when external energy is supplied to the system


during vibration.
• External energy can be supplied through :
1- Force excitation.
2- Displacement excitation (Base excitation).

11/10/2024 Mahmoud Abdalhamed.


4
Forced vibration system

• External Excitation can vary in nature:


1- Harmonic excitation:
• A regular, repeating force or displacement, often sinusoidal.
• The system’s response to such excitation is known as the harmonic response.

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5
Forced vibration system

• External Excitation can vary in nature:


2- Nonharmonic but periodic excitation:
Repetitive, non-sinusoidal forces or displacements that recur at regular
intervals.

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6
Forced vibration system

• External Excitation can vary in nature:


3- Nonperiodic excitation:
Irregular, one-time or intermittent forces or displacements.

F(t) F(t) F(t)

t t t
Step force Ramp force impulse force

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Forced vibration system
• External Excitation can vary in nature:
Nonperiodic excitations vary in duration and can be classified based on their
impact on the system:
➢ Long Duration Excitation: A sustained, continuous excitation that acts over
an extended period, significantly influencing the system’s behaviour through
prolonged energy input.
➢ Short Duration Excitation (Shock or Impulse): A brief, intense excitation
with a duration much shorter than the system’s natural period, delivering a
sudden energy surge and causing a rapid transient response

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8
Forced vibration system
• External Excitation can vary in nature:
3- Random excitation
• It refers to external forces or displacements that vary unpredictably over time,
lacking any regular or periodic pattern.
• Random excitation is commonly encountered in real-world situations where
forces arise from complex, uncontrollable sources.
Real examples of random excitation are:
➢ Earthquake ground motion
➢ Wind turbulence
➢ Vehicle vibrations
11/10/2024 Mahmoud Abdalhamed.
Harmonically Excited Vibration
10
Force excited vibration system

• Harmonic Excitation in Engineering: it commonly arises from rotational


unbalance in machinery, producing a sinusoidal force or displacement.
• Importance for Analysis: Understanding harmonic response helps predict system
behaviour under more complex excitations, aiding in resonance and stability
assessments.
• Harmonic excitation may be in the form of a force or displacement of some point
in the system.
𝑡 = 𝐹𝑜 sin(𝜔𝑡)
𝑌 𝑡 = 𝑌𝑜 sin(𝜔𝑡)

11/10/2024 Mahmoud Abdalhamed.


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Force excitated Mass-spring- damper system
Equation of motion Vibration response

c k

k.x

m
m.x
𝑥(𝑡) = 𝑥ℎ𝑜𝑚𝑜𝑔𝑒𝑛𝑜𝑢𝑠 + 𝑥𝑝𝑎𝑟𝑡𝑖𝑐𝑢𝑙𝑎𝑟

𝐹(𝑡) = 𝐹𝑜 sin 𝜔 𝑡
11/10/2024 Mahmoud Abdalhamed.
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Force excited Mass-spring- damper system
Vibration response 𝑥(𝑡) = 𝑥ℎ𝑜𝑚𝑜𝑔𝑒𝑛𝑜𝑢𝑠 + 𝑥𝑝𝑎𝑟𝑡𝑖𝑐𝑢𝑙𝑎𝑟

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Force excited Mass-spring- damper system
P𝑎𝑟𝑡𝑖𝑐𝑢𝑙𝑎𝑟 Solution (steady state response)
x(t ) = X sin(t −  ) m.x + cx + kx = Fo sin t
x (t ) = X cos(t −  ) = X sin(t −  +  / 2)
x(t ) = − 2 X sin(t −  )
−𝑚𝜔2 𝑋 sin( 𝜔𝑡 − 𝜑) + 𝑐𝑋𝜔 sin( 𝜔𝑡 − 𝜑 + 𝜋/2) + 𝑘𝑋 sin( 𝜔𝑡 − 𝜑) − 𝐹𝑜 sin 𝜔 𝑡 = 0
m 2 X sin(t −  ) − cX sin(t −  +  / 2) − kX sin(t −  ) + Fo sin t = 0
kX Fo sin t

cX  X sin(t −  )
t
m 2 X
11/10/2024 Mahmoud Abdalhamed.
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Force excited Mass-spring- damper system
P𝑎𝑟𝑡𝑖𝑐𝑢𝑙𝑎𝑟 Solution (steady state response)

F 2 = (cX ) 2 + (kX − m 2 X ) 2

Fo
X=
(k − m 2 ) 2 + (c ) 2

kX Fo sin t

cX  X sin(t −  )
t
m 2 X
11/10/2024 Mahmoud Abdalhamed.
15
Force excited Mass-spring- damper system
P𝑎𝑟𝑡𝑖𝑐𝑢𝑙𝑎𝑟 Solution (steady state response)
Non- dimensional form

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Force excited Mass-spring- damper system
P𝑎𝑟𝑡𝑖𝑐𝑢𝑙𝑎𝑟 Solution (steady-state response)

11/10/2024 Mahmoud Abdalhamed.


17
Force excited Mass-spring- damper system
P𝑎𝑟𝑡𝑖𝑐𝑢𝑙𝑎𝑟 Solution (steady-state response)

11/10/2024 Mahmoud Abdalhamed.


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Force excited Mass-spring- damper system
General response of forced vibration
Standard form

Steady state response

Transient response

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Quality Factor and Bandwidth

Quality Factor
• It is the value of the amplitude ratio at
resonance frequency.
• It is a measure of a system's resonant
sharpness.
• A high Q factor means low energy loss and
a narrow, sharp resonance peak.

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20
Quality Factor and Bandwidth
Bandwidth
• It is the range of frequencies over which the
system's response remains significant, typically
around the resonant frequency.
• Bandwidth is the frequency range where the
amplitude falls to 70.7% of the peak value.
• High Q has narrow bandwidth, and low Q has
wider bandwidth.

• Q and bandwidth determine the frequency


response and damping characteristics of a
system

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Example

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Example

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Example

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