GenericUser
Mechanical
- Dec 17, 2011
- 17
Hello,
I am trying to determine the stiffness of a part I simulated with enforced displacement. My first method was to use Hooke's law F=kx but applying an external non-pressure force was problematic in Abaqus. So I think I may have found a way using modal frequencies, but I have doubts if my method is sound.
Basically any continuous part has infinite number of natural modes. So w=sqrt(k/m) is only one of many frequencies. What I did is animate each mode until I found a mode shape that closely resembles the deformation pattern I am looking for and then calculating w using w=(2*pi*f) and then calculating the stiffness k by saying k = mw^2. Is this method correct or is it wrong to apply discrete vibration theory to a continuous part in this manner?
I am trying to determine the stiffness of a part I simulated with enforced displacement. My first method was to use Hooke's law F=kx but applying an external non-pressure force was problematic in Abaqus. So I think I may have found a way using modal frequencies, but I have doubts if my method is sound.
Basically any continuous part has infinite number of natural modes. So w=sqrt(k/m) is only one of many frequencies. What I did is animate each mode until I found a mode shape that closely resembles the deformation pattern I am looking for and then calculating w using w=(2*pi*f) and then calculating the stiffness k by saying k = mw^2. Is this method correct or is it wrong to apply discrete vibration theory to a continuous part in this manner?