results and discussion (vibration s)

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  • 8/10/2019 Results and Discussion (Vibration s)

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    7.0 RESULTS AND DISCUSSION

    The graphs of Peak-to-Peak value, RMS value and crest factor were plotted against with the

    rotational speed of motor as below. We can observe the vibration waveform varies with time and

    the effect of adding bearings with and without unbalanced load by monitoring the change in the

    vibration response as to compare with the baseline data

    Experiment A: Baseline Vibration

    Graph 1- Experiment A : Baseline Vibration (Peak-to-Peak vs Speed of Motor)

    Graph 2- Experiment A : Baseline Vibration (RMS vs Speed of Motor)

    0

    0.0005

    0.001

    0.0015

    0.002

    630 810 1180 1320 1490

    Peak-t

    o-Peak(m)

    (rpm)

    Experiment A : Baseline Vibration

    (Peak-to-Peak vs Speed of Motor)

    0.00026

    0.00027

    0.00028

    0.00029

    0.0003

    0.00031

    630 810 1180 1320 1490

    RMS(m)

    (rpm)

    Experiment A : Baseline Vibration

    (RMS vs Speed of Motor)

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    Graph 3- Experiment A : Baseline Vibration (Crest Factor vs Speed of Motor)

    Experiment B1: Bearing Fault- without unbalanced mass

    Graph 4- Experiment B1: Bearing Fault- without unbalanced mass

    (Peak-to-Peak vs Speed of Motor)

    2

    2.2

    2.4

    2.6

    2.8

    3

    630 810 1180 1320 1490

    CrestFac

    tor

    (rpm)

    Experiment A : Baseline Vibration

    (Crest Factor vs Speed of Motor)

    0

    0.001

    0.002

    0.003

    0.004

    630 810 1180 1320 1490Pe

    ak-to-Peak(m)

    (rpm)

    Experiment B: Bearing Fault -without unbalance weight

    (Peak-to-Peak vs Speed of Motor)

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    Graph 5- Experiment B1: Bearing Fault- without unbalanced mass

    (RMS vs Speed of Motor)

    Graph 6- Experiment B1: Bearing Fault- without unbalanced mass

    (Crest Factor vs Speed of Motor)

    0

    0.0001

    0.0002

    0.0003

    0.0004

    630 810 1180 1320 1490

    RMS(m)

    (rpm)

    Experiment B: Bearing Fault -without unbalance weight

    (RMS vs Speed of Motor)

    0

    2

    4

    6

    630 810 1180 1320 1490

    CrestFactor

    (rpm)

    Experiment B: Bearing Fault -without unbalance weight

    (Crest Factor vs Speed of Motor)

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    Exercise B2: Bearing Fault -with unbalanced mass

    Graph 7- Experiment B2: Bearing Fault- with unbalanced mass

    (Peak-to-Peak vs Speed of Motor)

    Graph 8- Experiment B2: Bearing Fault- with unbalanced mass

    (RMS vs Speed of Motor)

    Graph 9- Experiment B1: Bearing Fault- with unbalanced mass

    (Crest Factor vs Speed of Motor)

    0

    0.001

    0.002

    0.003

    0.004

    630 810 1180 1320 1490Peak-to-Peak(m)

    (rpm)

    Experiment B: Bearing Fault - with unbalanced mass

    (Peak-to-Peak vs Speed of Motor)

    0

    0.0002

    0.0004

    0.0006

    630 810 1180 1320 1490

    RMS(m)

    (rpm)

    Experiment B: Bearing Fault - with unbalanced mass(RMS vs Speed of Motor)

    0

    1

    2

    3

    4

    5

    630 810 1180 1320 1490

    CrestFactor

    (rpm)

    Experiment B: Bearing Fault - with unbalanced mass

    (Crest Factor vs Speed of Motor)

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    Comparison between Experiment A with Experiment B1 and Experiment B2

    (a)Peak-to-Peak value

    By observing the results from Graph 1 for baseline vibration, we can conclude that with

    increasing speed, the peak-to-peak value increases and it reached a maximum amplitude of

    0.001695 m where the speed of motors, =1490 rpm. By observing the results from Graph 4 for

    bearing fault without unbalanced mass, the peak-to-peak value increases and reached a maximum

    amplitude of 0.002865 m where the speed of motors, =1320rpm and then it decreased. By

    observing the results from Graph 7 for bearing fault with unbalanced mass, the peak-to-peak

    value increases and reached maximum amplitude of 0.003074 m where the speed of motors,

    =1320rpm and decreases.

    (b)RMS value

    By observing the results from Graph 2 for baseline vibration, we can conclude that with

    increasing speed, the RMS value increases but decreased at the speed of motors, =1320rpm andincreased and reached a maximum amplitude of 0.000307348 m at the speed of motors, =1490

    rpm. By observing the results from Graph 5 for bearing fault without unbalanced mass, the RMS

    value increased and reached a maximum 0.000359 m at the speed of motors, =1320rpm before

    it decreased. By observing the results from Graph 8 for bearing fault with unbalanced mass, the

    RMS value increased and reached a maximum 0.000383 m at the speed of motors, =1320rpm

    before it decreased.

    (c) Crest Factor

    By observing the results from Graph 3 for baseline vibration, with increasing speed, the

    crest factor increases and reached a maximum of 2.811149 at the speed of motors, =1490rpm .

    By observing the results from Graph 6 for bearing fault without unbalanced mass, the crest factor

    increased but decreased at the speed of motor, =810rpm but it was then increased to maximum

    of 4.31621 at the speed of motor, =1320rpm before it decreased again. By observing the results

    from Graph 9 for bearing fault with unbalanced mass, the crest factor increased and reached a

    maximum 3.982582 at the speed of motors, =1320rpm before it decreased.

    Effects of Motor Speed on Experiment A

    By observing the results from Graph 1 for baseline vibration, we can conclude that with

    the speed of motor increases, peak-to-peak value also increases as until =1490rpm where themaximum peak-to-peak value is observed. This represent that at this speed, the amount of lateral

    movement of machine is the highest and vibrates the most. For RMS value as it has a directly

    proportional relationship between peak-to-peak and RMS values, where highest RMS is found at

    about =1320 rpm which tell us that the vibration energy is at the maximum at this speed.

    Meanwhile for the crest factor, at =1320rpm, maximum impact is exerted on the machine

    because of the highest crest factor obtained.

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    Effects of Bearing Fault Without and With Unbalance Mass on Vibration Response

    When the bearing fault is mounted, the overall peak-to-peak value seems to be higher for

    all the motor speed compare to the baseline vibration of Experiment A. The vibration is

    intensified because of the unsuitable alignment between the abnormal bearing and the shaft when

    the faulty bearing is mounted on the shaft. Hence, it results in more lateral movement of themachine. However, for bearing fault with unbalanced mass, this only occurs at small speed.

    When the bearing fault is mounted, the overall RMS value is increased for all the motor

    speed compare to the baseline vibration of Experiment A because of the unsuitable alignment

    between bearing and shaft and caused it to vibrate with higher energy and intensity. It generates

    noisier operating sounds as a result of the vibration during the experiment. But when a screw is

    mounted to the rotor, the RMS value drops to a lower speed but it becomes even higher at higher

    speed.

    When the bearing fault is mounted, the overall crest factor is smaller compared to the

    baseline vibration at low motor speed. However, the crest factor is increased when the speed of

    the motor is increased as the impact wear is intensified at high speed for the vibration of bearing

    fault without the unbalanced mass. When an unbalanced mass is mounted, the crest factor

    decreased for almost all motor speed this means that the screw is effective in minimizing the

    impact of wear on the bearing due to the oscillating waveform.

    Exercise C: Resonance Test

    Effect of Rotor Location on Critical Speed

    The critical motor speed for the occurrence of resonance increased to =2335 rpm whenthe rotors were shifted to the left side of the shaft. There is a decrease in the speed required to

    result in resonance compared to =2160 rpm if the rotor were to be placed in the middle because

    of the imbalance position of the rotor increases the equivalent mass of the system. We can also

    observe that with lower natural frequency will lead to lower critical speed for resonance.

    Effect of Unbalanced Mass on Resonance

    The critical speed for the occurrence of resonance decreased to =2120 rpm when the

    unbalanced mass (a screw) was added to the rotor. There is a decrease in the speed required to

    result in resonance when compared to =2160rpm without the adding of unbalanced mass. This

    is because the unbalanced force induced on the rotor, acting as resistance to the shaft rotation.

    Hence, higher operating speed was applied in order to have resonance effect since some of the

    speed had been converted to cancel out the unbalanced force.

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    Damaging Effect of Resonance and Possible Remedial Actions

    Resonance has a great impact on the amplitude of oscillation of a system. Therefore it produces

    more vibration when the system is subjected to a speed equivalent to its natural frequency.

    Among the undesirable effects of resonance include:

    Machines failure due to unaccounted fatigue load

    Undesirable wear of machines parts

    Undesirable noises generated

    In order to cut down the effect of resonance, we can introduce a damper system to dissipate the

    energy generated from a system such as springy material or absorber. The damping system will

    be able to dissipate the amplitude of vibration. Since natural frequency, n= , we can alsomodify the natural frequency of the system by increasing the spring constant (k) of the system in

    order to increase its natural frequency to avoid disturbance due to external excitation that might

    cause to resonance.