موضوع: VIBRATION SOURCES الأحد 15 مايو 2011 - 23:21
<p dir="RTL" style="text-align:left;mso-pagination:widow-orphan lines-together; direction:rtl;unicode-bidi:embed" align="left">4.1. What Is Diagnosis?
<p dir="RTL" style="text-align:left;mso-pagination:widow-orphan lines-together; direction:rtl;unicode-bidi:embed" align="left"> From a general perspective, including both the medical and technical case, diagnosis can be explained as follows. For a process there are observed variables or behaviors for which there is knowledge of what is expected or normal. The task of diagnosis is to, from the observations and the knowledge, generate a diagnosis, i.e. to decide whether there is a fault or not and also to identify the fault. The following picture shows the information flow including a process and a diagnosis system.
<p class="MsoNormal" style="text-align:justify;mso-layout-grid-align:none; text-autospace:none;direction:ltr;unicode-bidi:embed" align="left"> All machinery with moving parts generates mechanical forces during normal operation. As the mechanical condition of the machine changes because of wear, changes in the operating environment, load variations, and so on, so do these forces. Understanding machinery dynamics and how forces create unique vibration frequency components is the key to understanding vibration sources.
<p class="MsoNormal" style="text-align:justify;mso-layout-grid-align:none; text-autospace:none;direction:ltr;unicode-bidi:embed" align="left"> Vibration does not just happen. There is a physical cause, referred to as a forcing function, and each component of a vibration signature has its own forcing function. The components that make up a signature are reflected as discrete peaks in the FFT or frequency-domain plot.
The vibration profile that results from motion is the result of a force imbalance. By definition, balance occurs in moving systems when all forces generated by, and acting on, the machine are in a state of equilibrium. In real-world applications, however, there is always some level of imbalance, and all machines vibrate to some extent. This section discusses the more common sources of vibration for rotating machinery, as well as for machinery undergoing reciprocating and/or linear motion.
<p class="MsoNormal" style="text-align:justify;mso-pagination:widow-orphan lines-together; tab-stops:right 18.0pt;mso-layout-grid-align:none;text-autospace:none; direction:ltr;unicode-bidi:embed" align="left"> Vibration due to unbalance of a rotor is probably the most common machinery defect. It is luckily also very easy to detect and rectify. The International Standards Organisation (ISO) define unbalance as: That condition, which exists in a rotor when vibratory, force or motion is imparted toits bearings as a result of centrifugal forces. It may also be defined as: The uneven distribution of mass about a rotor’s rotating centerline. There are two new terminologies used: one is rotating centerline and the other is geometric centerline. The rotating centerline is defined as the axis about which the rotor would rotate if not constrained by its bearings (also called the principle inertia axis or PIA). The geometric centerline (GCL) is the physical centerline of the rotor. When the two centerlines are coincident, then the rotor will be in a state of balance. When they are apart, the rotor will be unbalanced. There are three types of unbalance that can be encountered on machines, and these are:
<p class="MsoNormal" style="text-align:justify;mso-pagination:widow-orphan lines-together; mso-layout-grid-align:none;text-autospace:none;direction:ltr;unicode-bidi:embed" align="left">1. Static unbalance (PIA and GCL are parallel) figure (4-2)
<p class="MsoNormal" style="text-align:justify;mso-pagination:widow-orphan lines-together; mso-layout-grid-align:none;text-autospace:none;direction:ltr;unicode-bidi:embed" align="left">2. Couple unbalance (PIA and GCL intersect in the center) figure (4-3)
<p class="MsoNormal" style="text-align:justify;mso-pagination:widow-orphan lines-together; mso-layout-grid-align:none;text-autospace:none;direction:ltr;unicode-bidi:embed" align="left">3. Dynamic unbalance (PIA and GCL do not touch or coincide).
For all types of unbalance, the FFT spectrum will show a predominant 1× rpm frequency of vibration. Vibration amplitude at the 1× rpm frequency will vary proportional to the square of the rotational speed.
<p class="MsoNormal" style="text-align:justify;mso-pagination:widow-orphan lines-together; mso-layout-grid-align:none;text-autospace:none;direction:ltr;unicode-bidi:embed" align="left"> Misalignment, just like unbalance, is a major cause of machinery vibration. Some machines have been incorporated with self-aligning bearings and flexible couplings that can take quite a bit of misalignment. However, despite these, it is not uncommon to come across high vibrations due to misalignment.
<p class="MsoNormal" style="text-align:justify;text-indent:18.0pt;mso-pagination: widow-orphan lines-together;mso-layout-grid-align:none;text-autospace:none; direction:ltr;unicode-bidi:embed" align="left">There are basically two types of misalignment:
<p class="MsoNormal" style="text-align:justify;mso-pagination:widow-orphan lines-together; mso-layout-grid-align:none;text-autospace:none;direction:ltr;unicode-bidi:embed" align="left">1. Angular misalignment: the shaft centerline of the two shafts meets at angle with each other
<p class="MsoNormal" style="text-align:justify;mso-pagination:widow-orphan lines-together; mso-layout-grid-align:none;text-autospace:none;direction:ltr;unicode-bidi:embed" align="left">2. Parallel misalignment: the shaft centerline of the two machines is parallel to each other and have an offset.
Misalignment primarily subjects the driver and driven machine shafts to axial vibrations at the 1× rpm frequency. The figure is an exaggerated and simplistic single-pin representation, but a pure angular misalignment on a machine is rare. Thus, misalignment is rarely seen just as 1× rpm peak. Typically, there will be high axial vibration with both 1× and 2× rpm. However, it is not unusual for 1×, 2× or 3× to dominate. These symptoms may also indicate coupling problems
Eccentricity occurs when the center of rotation is at an offset from the geometric centerline of a sheave, gear, bearing, motor armature or any other rotor. The maximum amplitude occurs at 1× rpm of the eccentric component in a direction through the centers of the two rotors. Here the amplitude varies with the load even at constant speeds In a normal unbalance defect, when the pickup is moved from the vertical to the horizontal direction, a phase shift of 90° will be observed. However in eccentricity, the phase readings differ by 0 or 180° (each indicates straight-line motion) when measured in the horizontal and vertical directions. Attempts to balance an eccentric rotor often result in reducing the vibration in one direction, but increasing it in the other radial direction (depending on the severity of the eccentricity)
<p class="MsoNormal" style="text-align:justify;mso-pagination:widow-orphan lines-together; mso-layout-grid-align:none;text-autospace:none;direction:ltr;unicode-bidi:embed" align="left">4.2.4. Bent shaft
<p class="MsoNormal" style="text-align:justify;mso-pagination:widow-orphan lines-together; mso-layout-grid-align:none;text-autospace:none;direction:ltr;unicode-bidi:embed" align="left"> When a bent shaft is encountered, the vibrations in the radial as well as in the axial direction will be high. Axial vibrations may be higher than the radial vibrations. The FFT will normally have 1× and 2× components. If the:
<p class="MsoNormal" style="text-align:justify;mso-pagination:widow-orphan lines-together; mso-layout-grid-align:none;text-autospace:none;direction:ltr;unicode-bidi:embed" align="left">1• Amplitude of 1× rpm is dominant then the bend is near the shaft center figure (4-14)
<p class="MsoNormal" style="text-align:justify;mso-pagination:widow-orphan lines-together; mso-layout-grid-align:none;text-autospace:none;direction:ltr;unicode-bidi:embed" align="left">2• Amplitude of 2× rpm is dominant then the bend is near the shaft end.
<p class="MsoNormal" style="text-align:justify;mso-pagination:widow-orphan lines-together; mso-layout-grid-align:none;text-autospace:none;direction:ltr;unicode-bidi:embed" align="left">4.2.5. Rolling element bearings
A rolling element bearing comprises of inner and outer races, a cage and rolling elements. Defects can occur in any of the parts of the bearing and will cause high-frequency vibrations. In fact, the severity of the wear keeps changing the vibration pattern. In most cases, it is possible to identify the component of the bearing that is defective due to the specific vibration frequencies that are excited. Raceways and rolling element defects are easily detected. However, the same cannot be said for the defects that crop up in bearing cages. Though there are many techniques available to detect where defects are occurring, there are no established techniques to predict when the bearing defect will turn into a functional failure. In an earlier topic dealing with enveloping/demodulation, we saw how bearing defects generate both the bearing defect frequency and the ringing random vibrations that are the resonant frequencies of the bearing components. Bearing defect frequencies are not integrally harmonic to running speed. However, the following formulas are used to determine bearing defect frequencies. There is also a bearing database available in the form of commercial software that readily provides the values upon entering the requisite bearing number.
A gearbox is a piece of rotating equipment that can cause the normal low-frequency harmonics in the vibration spectrum, but also show a lot of activity in the high frequency region due to gear teeth and bearing impacts. The spectrum of any gearbox shows the 1× and 2× rpm, along with the gear mesh frequency (GMF). The GMF is calculated by the product of the number of teeth of a pinion or a gear, and its respective running speed