This tutorial was created using ANSYS 7.0 The purpose of this tutorial is to show the steps involved to perform a simple transient analysis.
Transient dynamic analysis is a technique used to determine the dynamic response of a structure under a time-varying load.
The time frame for this type of analysis is such that inertia or damping effects of the structure are considered to be important. Cases where such effects play a major role are under step or impulse loading conditions, for example, where there is a sharp load change in a fraction of time.
If inertia effects are negligible for the loading conditions being considered, a static analysis may be used instead.
For our case, we will impact the end of the beam with an impulse force and view the response at the location of impact.
Since an ideal impulse force excites all modes of a structure, the response of the beam should contain all mode frequencies. However, we cannot produce an ideal impulse force numerically. We have to apply a load over a discrete amount of time dt.
After the application of the load, we track the response of the beam at discrete time points for as long as we like (depending on what it is that we are looking for in the response).
The size of the time step is governed by the maximum mode frequency of the structure we wish to capture. The smaller the time step, the higher the mode frequency we will capture. The rule of thumb in ANSYS is
time_step = 1 / 20f
where f is the highest mode frequency we wish to capture. In other words, we must resolve our step size such that we will have 20 discrete points per period of the highest mode frequency.
It should be noted that a transient analysis is more involved than a static or harmonic analysis. It requires a good understanding of the dynamic behavior of a structure. Therefore, a modal analysis of the structure should be initially performed to provide information about the structure's dynamic behavior.
In ANSYS, transient dynamic analysis can be carried out using 3 methods.
We will use the Reduced Method for conducting our transient analysis. Usually one need not go further than Reviewing the Reduced Results. However, if stresses and forces are of interest than, we would have to Expand the Reduced Solution.
finish
/clear
/TITLE, Dynamic Analysis
/FILNAME,Dynamic,0 ! This sets the jobname to 'Dynamic'
/PREP7 ! Enter preprocessor
K,1,0,0 ! Keypoints
K,2,1,0
L,1,2 ! Connect keypoints with line
ET,1,BEAM3 ! Element type
R,1,0.0001,8.33e-10,0.01 ! Real constants
MP,EX,1,2.068e11 ! Young's modulus
MP,PRXY,1,0.33 ! Poisson's ratio
MP,DENS,1,7830 ! Density
LESIZE,ALL,,,10 ! Element size
LMESH,1 ! Mesh the line
FINISH
/SOLU ! Enter solution phase
ANTYPE, TRANS ! Transient analysis
TRNOPT,REDUC, ! reduced solution method
DELTIM,0.001 ! Specifies the time step sizes
!At time equals 0s
NSEL,S,,,2,11, ! select nodes 2 - 11
M,All,UY, , , ! Define Master DOFs
NSEL,ALL ! Reselect all nodes
D,1,ALL ! Constrain left end
F,2,FY,-100 ! Load right end
!*
!At time equals 0.001s
TIME,0.001 ! Sets time to 0.001 seconds
KBC,0 ! Ramped load step
FDELE,2,ALL ! Delete the load at the end
!*
!At time equals 1s
TIME,1 ! Sets time to 1 second
KBC,0 ! Ramped load step
!*
LSSOLVE,1,3,1 ! solve multiple load steps
FINISH
/POST26 ! Enter time history
FILE,'Dynamic','rdsp','.' ! Calls the dynamic file
NSOL,2,2,U,Y, UY_2 ! Calls data for UY deflection at node 2
STORE,MERGE ! Stores the data
PLVAR,2, ! Plots vs. time
!Please note, if you are using a later version of ANSYS,
!you will probably have to issue the LSWRITE command at the
!end of each load step for the LSSOLVE command to function
!properly. In this case, replace the !* found in the code
!with LSWRITE and the problem should be solved.