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how to calculate the natural frequency of poles

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dcceecy

Structural
Oct 15, 2008
112
I try to find the wind load on a pole with ASCE-7.
I assume the pole is flexible structures so I need to calculate the Gust Effect Factor G. so I have to know the natural frequency of the pole.

In the code, the fundamental period of structures is calculated as Ct h^x in seismic section. but if I use this formula, the pole is rigid structure (f > 1 HZ).

I am wondering if I used the right equation or should I just calcualte the frequency using flexural rigidty (EI) of a cantilever beam (the pole).

any suggestions are welcome.
 
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Pretend the mass of the flagpole is acting laterally instead of vertically, and calc what the deflection is at the tip. The natural frequency is (approximately) 0.18*((g/deflection)^0.5), where g is 386 inches/second squared.
 
For finding frequency of pole you can use any FEM software and use eigen value solution.

If you want to do this by hand procedure is as follow :-
Here I have considered that there is mass lumped at the tip of the pole.
1) Calculate the deflection of pole with horizontal unit force at the tip of the pole.
2) Inverse the value which you have got, this is stiffness of the pole K.
3) You have mass lumped at the tip of the pole. Let's call it as M.
4) Circular frquency of vibration is given by
OMEGA = sqrt(k/m)
5) Frequency in Hz is given by
N = OMEGA / [2*pi()]

If there is no mass attached at the tip of the pole, and pole is self standing then frequency of pole is given by

OMEGA = [3.66/L^2] x sqrt[E x I / M]

L = Height of pole
E = Modulus of elasticity
I = Moment of inertia
M = Mass per unit length

Note - In above equation it is assumed that pole is considered as of uniform shape

Hope this will answer your querry
 
OMEGA = [3.66/L^2] x sqrt[E x I / M]

3.66/in^2 * sqrt(lb/in^2 * in^4 / (lb/in))

=3.66/in^2 * sqrt (in^3) ?

 
It is also assuming a fixed base - not entirely true. You need to add to the length above ground the depth to the point of fixity below ground to give a correct "L" value.

Mike McCann
MMC Engineering
Motto: KISS
Motivation: Don't ask
 
SEIT- no, that is wrong.

Cheers

Greg Locock

I rarely exceed 1.79 x 10^12 furlongs per fortnight
 
That's the procedure/equations used in DG #11 for vibrations.

What's wrong with it?
 
DG #11 says (on page 13) That the natural frequency of a cantilever can be approximated using Eq 3-3 to Eq 3-5, by substituting a different delta (namely delta for a cantilever beam). It doesn't matter if the pole is horizontal, vertical, or somewhere in between. The natural frequency is the natural frequency.

Is DG #11 wrong or I am reading something wrong?
 
The equation is based on a simple spring and a lumped mass. A cantilever will give the same result as that equation if you load it at its end with a lumped mass, if the beam's mass is negligible. That is not the case here. Admittedly a 12% error in this case probably won't kill anyone, but wrong is wrong. The reason the error is small is quite neat, see the usual beam example for Rayleigh's method.



Cheers

Greg Locock

I rarely exceed 1.79 x 10^12 furlongs per fortnight
 
The ASCE 7-05 commentary has equations for estimating the natural frequency of poles. See page 294.
 
from page 294 of ASCE-7
n = [0.56/L^2] x sqrt[E x I / M]
 
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