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Building Design and Construction Handbook - Merritt - Ventech!

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5.158 SECTION FIVE<br />

2W� 2W� kW<br />

c � � � 2 (5.291)<br />

g g g<br />

d �<br />

Damping sometimes is expressed as a percent of critical (� as a percent of �).<br />

For small amounts of viscous damping, the damped natural frequency is approximately<br />

equal to the undamped natural frequency minus 1 ⁄2� 2 /�. For example,<br />

for 10% critical damping (� � 0.1�), � d � �[1 � 1 ⁄2(0.1) 2 ] � 0.995�. Hence, the<br />

decrease in natural frequency due to small amounts of damping generally can be<br />

ignored.<br />

Damping sometimes is measured by logarithmic decrement, the logarithm of<br />

the ratio of two consecutive peak amplitudes during free vibration.<br />

2��<br />

Logarithmic decrement � (5.292)<br />

�<br />

For example, for 10% critical damping, the logarithmic decrement equals 0.2�.<br />

0.2�<br />

Hence, the ratio of a peak to the following peak amplitude is e � 1.87.<br />

The complete solution of Eq. (5.288) with initial displacement y o <strong>and</strong> velocity<br />

v o is<br />

� d o d�<br />

vo � �y<br />

��t<br />

o<br />

y � e sin � t � y cos � t<br />

� d<br />

2 �<br />

t<br />

��(t��)<br />

�d 0<br />

� e� � ƒ(�)e sin � (t � �) d� (5.293)<br />

where e� is the deflection that the applied force would produce under static loading.<br />

Equation (5.293) is identical to Eq. (5.274) when � � 0.<br />

Unbalanced rotating parts of machines produce pulsating forces that may be<br />

represented by functions of the form F o sin �t. If such a force is applied to an<br />

undamped one-degree system. Eq. (5.274) indicates that if the system starts at rest<br />

the response will be<br />

� �� �<br />

Fg o<br />

2 1/� �<br />

2 2<br />

y � sin �t � sin �t (5.294)<br />

W 1 � � /� �<br />

And since the static deflection would be F o/k � F og/W� 2 , the dynamic load factor<br />

is<br />

� �<br />

1 �<br />

D � sin �t � sin �t (5.295)<br />

2 2 1 � � /� �<br />

If � is small relative to �, maximum D is nearly unity; thus, the system is practically<br />

statically loaded. If � is very large compared with �, D is very small; thus, the<br />

mass cannot follow the rapid fluctuations in load <strong>and</strong> remains practically stationary.<br />

Therefore, when � differs appreciably from �, the effects of unbalanced rotating<br />

parts are not too serious. But if � � �, resonance occurs; D increases with time.<br />

Hence, to prevent structural damage, measures must be taken to correct the unbalanced<br />

parts to change �, or to change the natural frequency of the vibrating mass,<br />

or damping must be provided.<br />

The response as given by Eq. (5.294) consists of two parts, the free vibration<br />

<strong>and</strong> the forced part. When damping is present, the free vibration is of the form of<br />

d

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