9 natural frequency

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    Introduction to Natural Frequency Testing

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    INTRODUCTION

    Every mechanical system has a series of natural frequencies, each of which has its

    own damping characteristics. These natural frequencies will liedormantin a

    system until they are excited by some external influence or forcing function.

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    The vibration can be greatly amplified if a forcing function, such as unbalance or a

    blade pass frequency (# blades X RPM) happens to be within the range of a

    natural frequency. When such forcing frequencies coincide with (or closely

    approach) a natural frequency, this is the condition known as resonance.

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    DIFFERENCE BETWEEN NATURAL FREQUENCY, RESONANCE AND

    CRITICAL SPEED

    The termsnatural frequency, resonanceandcritical speedare often used

    interchangeably, even by experienced vibration analysts. However, there are

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    . ,operating at a resonant frequency, but this may or may not be a critical speed. It is

    hoped the following definitions will help clarify the differences between each of these

    important terms.

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    a. Natural Frequency:

    Reference 2 defines a natural frequency as The frequency of free vibration of a

    system. The frequency at which an undamped system with a single degree of

    freedom will oscillate upon momentary displacement from its rest position.In

    addition, for a multiple degree-of-freedom system, the natural frequencies are

    the frequencies of the normal modes of vibration. All machines and all

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    structures have a number of natural frequencies. If forced to vibrate at one or

    more of these natural frequencies, dynamic stresses of 10 to 100X higher

    than those are inducedcompared to those which would be generated if these

    same forces were input at other frequencies lower or higher than these

    natural frequencies.

    This only becomes a problem if they are excited(seeresonancebelow). For

    example, when we perform impulse tests, we are not looking for resonant

    frequencies, but for natural frequencies which the machine must avoid so that it

    may not encounter resonance.

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    Natural Frequency

    Every machine will be vibrating at its natural frequency when it is exciting

    by external force:

    = 1/2

    =

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    2Pi 2PiFn = natural frequency , cpm

    Gc = Gravity of earth , m/s2

    K = Stiffness Kg/metreM = Mass , Kg/m/s2

    Delta = Deflection, m

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    b. Resonance:

    Resonance is the condition which occurs when such forcing frequencies do in fact

    coincide with one or more natural frequencies. These may be a natural frequencies

    of the rotor, but often can be a natural frequency of the support frame, foundation or

    even of drive belts. The piping on compressors can be a problem if they resonate.

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    Forcing frequencies include those from sources such as unbalance, misalignment,

    looseness, bearing defects, gear defects, belt wear, etc.

    Therefore, it is important to point out resonances can be encountered not only at 1X

    RPM,but at series of frequencies including 1X RPM, 2X RPM, 3X RPM, etc.

    Reference 2 defines resonance as the condition of vibration amplitude and phase

    change response caused by a corresponding system sensitivity to a particularforcing frequency. A resonance is typically identified by a substantial amplitude

    increase, and related phase shift.

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    Resonance - Characteristics

    1. Lack of response to balance attempts: thus it is almost impossible to

    balance the rotor having resonance problem. It is necessary to change

    natural frequency or speed.

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    . ,resonant direction be 5 to 15 times higher than other direction.

    3. Phase Behavior in the resonant measuring direction: 90 degree change

    of phase with almost 180 degree through resonant

    4. Probable phase difference in measuring direction perpendicular to resonant

    measuring direction: Noticeable phase difference else than 90 degreewhen measurement in horizontal compare to vertical direction.

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    5. Frequencies at which resonance can occur:

    Resonant Vibration = Forcing frequency vibration x Q

    6. Resonance can suddenly occur on a long running machine never before

    subjected to it:

    For exam le bearin wear or sim le sleeve bearin re lacement which can

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    cause a change in natural frequency. One can simply solve this type of

    problem by proper installation of the bearings and checking for required

    clearance specifications.

    7. Possible effect of coupling changes:

    Coupling changes can sometimes result in a different torsional natural

    frequency, particularly if a different diameter coupling is used, or differenttype. Significant vibration occur in bearings on either side of the coupling.

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    c. Critical Speed:

    Reference 3 points out that critical speeds are a special case of resonance in

    which the vibrating forces are caused by the rotation of the rotor. He also adds that

    critical speed testing is often more complicated than resonance testing because

    the natural frequencies encountered are functions of stiffness and mass which may

    be dependent on machine speed. For example,in the case of a machine with an

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    extended overhung rotor or in the case of general sleeve bearing machines, critical

    speeds can change their frequency location due to changes in stiffness and/or

    gyroscopic motion (unlike resonant frequencies for frames, foundations and rolling

    element bearing machines which have fixed natural frequencies independent of

    operating speed).

    Similarly, Reference 1 defines critical speeds as in general, any rotating speed

    which is associated with high vibration amplitude. Often, the rotor speeds whichcorrespond to natural frequencies of the system.Generally, good design practices

    mandate that a machine should be designed not to operate within 20% of a critical

    speed(not20% of any natural frequency).

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    Critical Speed

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    typically 20% or greater

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    fn

    fhfl

    Q (amplification factor) = fn / (fh-fl)

    Damping factor = 1

    2Q

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    = 0.707 An

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