Differences between analytic and Radioss solutions in modal transient dynamic analysis
Hey,
we have a mass applied to a spring, which is clamped on the other side. At the mass we apply a Cosinus load [ F*COS(OMEGA*t) ]
F = 500 N
OMEGA = 1 1/s
t = 0 - 8 s [DT 0.01]
Now we do a modal transient dynamic analysis and look at the history of displacements with the help of Hyperview.
The screenshot shows the result in HyperView.
Now the problem is, that the analytic results are not the same.
Our sping has a rate (k) of 500 N/m and the apllied mass has a weigth (m) of 10 kg.
So we calculate with the following equations:
omega=sqrt(k/m)
set-up ratio: eta=OMEGA/omega
magnification function: V=sqrt(1/(1-eta^2)^2)
The whole system is undamped.
The equation for the displacement is:
x(t)=(F/k)*V*cos(OMEGA*t)
for the maximum amplitude: cos(OMEGA*t)=1.
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Hi,
the red triangle is a DAREA load with a value of -500N. In the collector Tabled there is the cosine profile of this force.
In the Load Collector TLoad we combine the DAREA Force with the cosine profile to a dynamic load, which excites the mass at the end of the spring.
But the problem is, that we don't get equal solutions with Hyperworks and the manual calculation.
Thanks and regards.
Hi,
The omega= sqrt(K/m) holds good for angular frequency, it is not what are you interested, I guess. So it should be the dynamic analysis is natural frequency (rad/time)
to the omega should be (2* pi / T = 2 * Pi * f) where f= 1 / 2*pi ( (sqrt (K/M)).
could you please check the above?
Also, could you give us any reference of the calculation (formula) from which you calculated the displacement?
Hi,
can you confirm if the force applied is a dynamic load?
Assuming the mass is in Kgs, the modelled CONM2 is 10Kgs (which is 98.1 N ~100N) which is a static load and a dynamic load factor of 500 will make the dynamic load or force to 100*500= 5*E4.