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 EXPT NO: NAME: DATE: ROLL NO: WHIRLING OF SHAFT AIM To study the whirling phenomenon of the given shafts and to compare the theoretical and experimental values of critical speeds of whirling. APPARATUS Apparatus consists of a frame to support the driving motor with speed control unit to vary the speed and two bearing blocks and to support the holding chuck. Chuck supports the free end of the shaft. Shafts of different diameters (d1, d2, and d3), tachometer, Vernier calipers and spanner are also needed. THEORY AND PRINCIPLE When a shaft rotates it will go into transverse oscillations if the shaft is out of balance due to eccentricity of CG and neutral axis of the shaft, e . The resulting centrifugal force will induce the shaft to vibrate. When shaft rotates at speed equal to natural frequency of transverse oscillations this vibration becomes large and shows up as whirling of shaft. It also occurs at multiples of resonant speed. a- Mode 1  b- Mode 2 c- Mode 3

Whirling of Shaft

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  • EXPT NO: NAME:

    DATE: ROLL NO:

    WHIRLING OF SHAFT

    AIM

    To study the whirling phenomenon of the given shafts and to compare the theoretical and

    experimental values of critical speeds of whirling.

    APPARATUS

    Apparatus consists of a frame to support the driving motor with speed control unit to vary the

    speed and two bearing blocks and to support the holding chuck. Chuck supports the free end of

    the shaft. Shafts of different diameters (d1, d2, and d3), tachometer, Vernier calipers and spanner

    are also needed.

    THEORY AND PRINCIPLE

    When a shaft rotates it will go into transverse oscillations if the shaft is out of balance due to

    eccentricity of CG and neutral axis of the shaft, e. The resulting centrifugal force will induce

    the shaft to vibrate. When shaft rotates at speed equal to natural frequency of transverse

    oscillations this vibration becomes large and shows up as whirling of shaft. It also occurs at

    multiples of resonant speed.

    a- Mode 1

    b- Mode 2

    c- Mode 3

  • When the shaft of mass M rotates, the centrifugal force will force it to bend out. Let the

    deflection of the shaft due to centrifugal force be r. The distance of CG is then r+e. Let the

    shaft rotates at rad/s and trasverse stiffness of the shaft be Kt .

    The centrifugal force is M2(r+e)

    Equating force we have Kt r = M2(r+e)

    Kt/M=n, so r = e / (1-(/n)2)

    If =n then r = infinity. So the shaft will whirl at its natural frequency.

    PROCEDURE

    1. The given rod is held between holding chuck and bearing.

    2. The motor is switched on and speed is to be increased to certain value at which violent

    vibration of rod occurs.

    3. The shaft deflects like a single bow or like a skipping rope.

    4. The speed is measured with tachometer.

    5. The speed is increased further to a value at which double bow is formed.

    6. This speed is also measured and above procedure is repeated for three different shaft

    diameters.

  • TABULAR COLUMN

    Sl

    No

    Diameter

    of shaft

    (m)

    Area of

    shaft

    (m2)

    M.I. of

    shaft

    (m4)

    UDL

    (N/m)

    Static

    deflection

    (m)

    Mode Theoretical

    critical

    speed

    Actual

    critical

    speed

    1

    2

    1

    2

    1

    2

    OBSERVATIONS AND SAMPLE CALCULATIONS FOR SET NO:__________

    d- diameter of the shaft= m

    A -Cross section area of the shaft, (/4) d2= = m2

    - density of the shaft material= 8000 Kg/m3

    g- acceleration due to gravity= 9.81 m/s

    W - uniformly distributed load on the shaft, g A= N/m

    Static deflection of the shaft (both ends fixed) due to self weight is given by

    = 1/384 (WL4/EI) m

    L length of the shaft = m

  • E Youngs modulus of the shaft= 2.1 x 1011 N/m2

    I - Moment of inertia of the shaft about the horizontal,

    (/64) d4= = m4

    The lowest critical speed is:

    Theoretical critical speed at node 1 = = rpm

    Theoretical critical speed at node 2 = = rpm

    RESULTS

    The experiment on whirling of shaft is done and following results are obtained.

    For shaft 1 (d = m);

    Theoretical critical speed at node 1 =________rpm

    Theoretical critical speed at node 2 =________rpm

    Experimental critical speed at node 1= ________rpm

    Experimental critical speed at node 2= ________rpm

  • For shaft 2 (d = m);

    Theoretical critical speed at node 1 =________rpm

    Theoretical critical speed at node 2 =________rpm

    Experimental critical speed at node 1= ________rpm

    Experimental critical speed at node 2= ________rpm

    For shaft 3 (d = m);

    Theoretical critical speed at node 1 =________rpm

    Theoretical critical speed at node 2 =________rpm

    Experimental critical speed at node 1= ________rpm

    Experimental critical speed at node 2= ________rpm

    INFERENCE