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    Chapter 3Forced Vibrations of SDOF

    Dr.-Ing. Azmi Mohamed Yusof

    Faculty of Mechanical Engineering

    At the end of this chapter students will be able to state, derive and apply

    the fundamental principle of vibration involving:-

    Forced vibration of undamped system with harmonic excitation

    Forced vibration of damped system with harmonic excitation

    Various applications, specifically the system with rotating unbalanced

    and method for vibration isolation

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    Course outcome

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    Undamped system with harmonic oscillation

    Consider the simplest vibrating system as shown infig. (a)

    The time varying external force is given by

    cos

    Applying Newtons second law for the FBD shown in

    fig. (b),

    cos

    or

    cos (1)

    Where is the natural frequency of the mass, while is the frequency of the external force

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    Forced Vibrations of SDOF

    =0

    =0

    The solution to this second order, linear, nonhomogeneous ODE containcomplementary solution , and particular solution

    ---- (2)

    The complementary solution :

    0

    cos sin ---- (3)

    Let assume the particular solution as :

    cos ---- (4)

    Obtaining the velocity and acceleration term for eqn. 4 gives

    cos

    sin

    cos

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    Substituting the above equations into eqn. (1)

    cos

    cos

    cos

    ;

    From eqn. (2), , the final solution gives

    cos sin

    cos

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    The complementary solution defines the freevibration (see figure (a)) and it will typically dampen

    out.

    Therefore xc is referred to as transient

    The particular solution describes the force vibration

    caused by the applied load (fig. (b))

    There resultant vibration is shown in fig. c

    As the free vibration will in time dampen out, the

    remaining vibration will be the force vibration

    Thus, is called steady state (see fig. (d)).

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    We need to determine the constant D & E by using

    initial conditions.

    Suppose 0 and 0 , then wehave

    and

    By substituting into equation 1

    cos

    sin

    cos

    If the static deflection of the mass due to force Fo is

    given by

    , the maximum amplitude can be

    written as,

    1

    1

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    The ratio, is known as the magnification factor

    (M)

    M The ratio of the amplitude of vibration to the

    amplitude of zero frequency deflection

    The plot

    or Magnification factorversus the

    frequency ratior

    is shown in fig. (a)

    The asymptote occurs at r =1, thus the system

    response can be of three types

    When 0 1

    When

    = 1

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    Case 1, when 0 natural frequency

    of forced vibration

    The amplitude of forced response > the static deflection

    The harmonic response of the system xp(t) is in phase with the external

    force. See the plots as shown in the figure

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    External force excitation System response

    Case 2, when > 1

    The natural frequency of the free vibration

    response < natural frequency of forced

    vibration

    cos , where

    and has opposite sign, 180o out ofphase

    When

    , then X 0 : the response at

    very high frequency is close to zero.

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    External force excitation

    System response

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    External force excitation

    System response

    Case 3, when

    = 1

    The condition when = n is called resonance

    Amplitude of oscillation increases linearly with

    time or infinite

    Undesirable condition which may harm overall

    system

    The equation of motion is

    The response of the system at resonance is:

    Example

    A weight of 50N is suspended from a spring of stiffness 5000 N/m and is

    subjected to a harmonic force of amplitude 40N and frequency of 4 Hz.

    Determine

    a) the extension of the spring due to suspended spring

    b) the static displacement of the spring due to the maximum applied

    force

    c) the amplitude of the forced motion of the weight

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    Solution

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    Example

    A 50 kg mass is hanging from a spring of stiffness 5 x 104 N/m. A

    harmonic force of magnitude 100 N and frequency 100 rad/s is applied to

    the system. Determine

    a) the amplitude of the forced response

    b) the natural frequency of the system

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    Solution

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    Example

    A reciprocating pump, having a mass of 68 kg, is mounted at the middle of a

    steel plate of thickness 1 cm, width 50 cm, and length 250 cm, clamped along

    two edges as shown in the figure below. During operation of the pump, the plate

    is subjected to a harmonic force, 220 cos62.832 N. Determine theamplitude of vibration of the plate. (Take the plate equivalent stiffness of the

    beam as

    , and Youngs modulus of the beam as 200 Gpa).

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    Solution

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    Forced vibration with viscous damping

    Consider a viscously damped SDOF spring-mass

    system as shown in fig. (a).

    Suppose the external force applied is in the form of

    sin

    Using Newtons second law of motion for FBD shown in

    fig. (b),

    cos or

    cos

    The particular solution can be assumed in the form

    cos sin The velocity and acceleration terms become,

    sin

    cos

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    Substitute these results into equation 1,

    cos sin cos

    Extracting the algebraic equation involving term A and B,

    and 0

    Dividing both equations with k

    1 2 and 2 1 0

    Where

    ,

    and

    Solve the above equation for A and B yield,

    ,

    The result for a steady state equation

    1 21 cos 2 sin

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    It can also be written in a generalized form

    Introducing the magnification factor M,

    Where the phase angle is:

    The plot for M versus r, and versus r are shown in the figure

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    Finally, The complete solution is given by

    cos cos

    and can be determined from the initial conditions 0 0

    See textbook page 275 for complete solution (long equation).

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    Example

    A SDOF spring-mass-damper system is subjected to a harmonic force.The amplitude is found to be 25 mm at resonance and 10 mm at a

    frequency 0.75 times the resonant frequency. Determine the damping

    ratio for the system.

    Solution

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    Example

    A SDOF damped system is composed of a mass of 10 kg, a spring

    having a constant of 2000 N/m, and a dashpot with damping constant of

    50 Ns/m. The mass of the system is acted on by a harmonic force F = Fo

    sin t having a maximum value of 250 N and a frequency of 5 Hz.

    Determine the complete solution for the motion of the mass.

    Solution

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    Example

    A 25 kg mass is mounted on an oscillator pad whose stiffness is 5 x 105

    N/m. When the system is subjected to a harmonic excitation of

    magnitude 300 N and frequency 100 rad/s, the phase different between

    the excitation and the steady state response is 25o. Determine:

    a) the damping ratio of the isolator pad

    b) the isolator pads maximum deflection due to this excitation

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    Response due to harmonic motion ofthe base/support motion

    Sometime the base or support of a

    spring-mass-damper-system undergoes

    harmonic motion.

    Example of this situation is the car

    moving on bumpy road as shown in the

    figure.

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    Forced Vibrations of SDOF

    Let y(t) denote the displacement of the base and x(t) the displacement of

    the mass

    The system is simplified in the figure shown. The subsequent analysis is

    based on the FBD shown. The net elongation of the spring is

    The relative velocity between two ends of the damper is

    The equation of motion according to the FBD is obtained as:

    k 0

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    Rearrange the equation

    If sin, then cos sin

    If sin and - and substitute into eqn. 1 then sin

    where , and

    Recall our steady state response for a spring-mass-damper system

    sin

    sin

    Therefore,

    sin

    sin

    Where

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    The amplitude of oscillation is obtained as

    or

    Rearrange the equation,

    If Z is the relative displacement between the mass and the base, then

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    The maximum force transmitted to the base is given by

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    Example

    The simple model of motor vehicle

    is shown in the figure, that can

    vibrate in the vertical direction

    while traveling over a rough road.

    The vehicle has a mass of 1200

    kg. The suspension system has a

    spring constant of 400 kN/m and a

    damping ratio of 0.5. If the vehicle

    speed is 20 km/h, determine the

    displacement amplitude of the

    vehicle. The road surface varies

    sinusoidally with an amplitude of Y= 0.05m and a wavelength of 6m.

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    Solution

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    Class exercise

    A 50 kg mass is attached to the base through a spring in parallel with a

    damper as shown in fig. below. The base undergoes a harmonic

    excitation of y(t) = 0.20 sin 30t. The stiffness of the spring is 30000 N/m

    and the damping constant is 200 Ns/m. Determine a) the amplitude of the

    masss absolute displacement, b) the amplitude of its displacement

    relative to its base [ans: a) 0.38m; b) 0.56m]

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    m

    k c

    y(t) = 0.20 sin 30t

    x(t)

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    Solution

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    Class exercise

    A racing car is modeled as a SDOF damped system vibrating in the

    vertical direction. The elevation of the road is assumed to vary

    sinusoidally. The distance from peak to through is 0.2 m and the distance

    between peaks is 70m. The natural frequency of the system is 2 Hz and

    the damping ratio of the damper is 0.15. Determine the amplitude of

    vibration of the racing car at a speed of 120 km/h. [ans: 1.06 m]

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    Solution

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    Rotating unbalanced

    Unbalanced forces in many rotating

    mechanism is the common sources of

    vibration excitation.

    Consider the rotating component is

    mounted in bearing and rotates

    counterclockwise.

    Variables:

    M = total mass of the system

    m = eccentric mass located at e from the

    center of rotation.

    x = the displacement of the machine in

    vertical direction

    = angular speed

    t = time

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    The component of the displacement of the eccentric mass in vertical

    direction is given by:

    sin

    the acceleration is obtained as

    sin

    The total inertia forces of the machine

    Applying Newtons second law of motion

    and using equation 3 yield,

    sin

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    Comparing this equation with fundamental equation

    We obtain that

    Recall the steady state solution for the system

    sin , where

    ,

    and

    Finally the steady state response is obtained as:

    /

    1 2

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    Basic damped forced equation Equation 4

    sin

    sin

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    This equation can also be written as

    1 2sin

    Thus the amplitude of vibration is obtained as

    1 2

    Peak deflection of the mass M at resonance is given from

    ; thus

    The force transmitted to the base

    1 2

    1 2sin

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    Forced Vibrations of SDOF - Applications

    Example

    An electric generator weighing 981 N and operating at 600 rpm is

    mounted on four parallel springs of stiffness 5000 N/m each. Determine

    the maximum permissible unbalance in order to limit the steady state

    deflection to 6 mm peak-to-peak.

    Solution

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    Example

    An electric motor of mass M, mounted on an elastic

    foundation, is found to vibrate with a deflection of

    0.15 m at resonance. It is known that the unbalanced

    mass of the motor is 8% of the mass of the rotor due

    to manufacturing tolerances used, and the damping

    ratio of the foundation is 0.025, Determine:

    a) the eccentricity or radial location of the

    unbalanced mass (e).

    b) the peak deflection of the motor when the

    frequency ratio varies from resonance

    c) the additional mass to be added uniformly to the

    motor if the deflection of the motor is to be reduced

    to 0.1 m.

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    Solution

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    Vibration isolation and force transmissibility

    To minimize excessive vibration excitation that may

    contribute to system failure, an isolator is installed to

    support the structure

    The vibration isolator is typically designed on the

    machine with flexible support

    Good isolator design must consider proper selection of

    the stiffness and damping coefficients.

    Consider a spring-mass- damper system (fig.(a)) with

    external force applied in the form of sin

    The FBD for the system and the velocity triangle isshown in fig. (b) and (c).

    The force transmitted to the support can be written as

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    sin

    sin

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    Transmissibility, is defined as the ratio of the transmitted force to thatof the disturbing force

    When the damping is negligible, then

    1

    1

    To reduce the amplitude X without changing Td,

    Isolated mass m can be mounted on larger mass M

    The stiffness k must be increased to keep the ratio

    constant

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    M

    mk

    The plot Td versus r is shown in the figure below

    At region Td >1 for r < 1.41, the amplitude of transmitted force is greater

    than the amplitude of applied force.

    For r < 1.41, the transmitted force to the support can be reduced by

    increasing the damping factor.

    Vibration isolation is best accomplished by an isolator composed only of

    spring elements for which r > 1.41 with no damping element used in the

    system.

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    Transmiss

    ibility,

    Td

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    Example

    A machine of mass 100 kg is mounted on springs anddamper as shown in the figure. The total spring stiffness is

    50,000 N/m and the damping factor is 0.20. A harmonic

    force, F = 200 sin 13.2t acts on the mass. Determine:-

    a) the amplitude of the motion of the machine

    b) its phase with respect to the existing force

    c) the transmissibility

    d) the maximum dynamic force transmitted to the foundation

    e) the maximum velocity of the motion

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    Solution

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