ME 440 Intermediate Vibrations

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ME 440 Intermediate Vibrations April 15, 2017 ME 440 Intermediate Vibrations Tu, March 24, 2009 Chapter 4: Dynamic Load Factor + Response Spectrum M1051 ECB 2, 2hr EES seminars: 2-4 pm on Jan 20 4-6 pm on Jan 20 © Dan Negrut, 2009 ME440, UW-Madison

Before we get started… Last Time: April 15, 2017 Before we get started… Last Time: Response to an arbitrary excitation Convolution Integral (Duhamel’s Integral) Hints for HW due Th (hw is not trivial…): For 4.23 Draw on Example 4.11, your problem is tougher though since you have damping Note that you are required to come up with the relative motion (it’s simpler this way) For this problem, assume that the vehicle moves horizontally at constant velocity For 4.24 Draw on Example 4.10, your problem is slightly simpler Today: HW Assigned (due March 31): 4.32 and 4.35 Material Covered: Response to an arbitrary excitation: The total solution Dynamic Load Factor 2

April 15, 2017 Example [AO] Determine the response of a 1DOF system to the step function Work with an underdamped system 3

Alternate Solution Previous Example [AO] April 15, 2017 Alternate Solution Previous Example [AO] Determine the response of a 1DOF system to the step function Work with an underdamped system – alternate solution Consider now Start hunting for xp(t) (go back several slides and look at table) Note that xh(t) is very easy… 4

[Concluding Remarks] Determining the Total Response April 15, 2017 [Concluding Remarks] Determining the Total Response Direct Integration If you can find a particular solution xp(t) Rely on Duhamel’s Integral When the excitation force is wild… 5

Steps that need to be taken: April 15, 2017 [Concluding Remarks. Cntd.] Determining the Total Response: Direct Integration Steps that need to be taken: Step 1: Assume a solution for xp(t) Step 2: Substitute xp(t) back into the ODE to get unknown coefficients Step 3: Deal with xh(t). Choose one of the following two forms Step 4: Solve for A & B based on initial conditions associated with the IVP and the contribution of xp(t) component to the initial values Direct Integration: works when F(t), the forcing term, is one of the lucky scenarios in the Table discussed a couple of lectures ago. Otherwise, use convolution integral approach (next slide) 6

Steps that need to be taken: April 15, 2017 [Concluding Remarks. Cntd.] Determining the Total Response: Convolution Approach Steps that need to be taken: Step 1: Deal with xh(t). Chose one of the following two forms Step 2: Compute A and B based on ICs: Step 3: Produce the “Duhamel” component Use Convolution Approach: when F(t), the forcing term, is not one of the scenarios in Table discussed a couple of lectures ago. 7

Comments on the Convolution Approach April 15, 2017 Comments on the Convolution Approach What kind of initial conditions should you consider when solving for the homogeneous component in the Convolution Approach? You can answer if you know the initial conditions for the convolution component In other words, you need to figure out Going then back to the original question, you immediately have that 8

[Cntd] Comments on the Convolution Approach April 15, 2017 [Cntd] Comments on the Convolution Approach Recall that It is relatively easy to prove that The proof will use two things: Leibniz Integral Rule: Expression of the impulse response: 9

[New Topic] Dynamic Load Factor [DLF] April 15, 2017 [New Topic] Dynamic Load Factor [DLF] We’ve already discussed this concept for harmonic excitation Previously defined as Recall that defined in conjunction with external excitation of the form F0sin( t) Move beyond harmonic excitation, consider the DLF for other loading scenarios Start with undamped system and a step force Assume zero initial conditions Solution assumes form 10

[Cntd] Dynamic Load Factor [DLF] April 15, 2017 [Cntd] Dynamic Load Factor [DLF] The DLF is obtained as (note that it depends on time): If the ICs are not zero, the picture gets more complicated (with no good reason…), since Computing now DLF is not leading to something that looks pretty Forget about this, go back to the case when zero ICs… 11

DLF – Departing Thoughts April 15, 2017 DLF – Departing Thoughts DLF is : Nondimensional Independent of the magnitude of the load (again, we assume zero ICs) In many structural problems only the maximum value of the DLF is of interest For case just considered, max DLF is 2 All maximum displacements, forces and stresses due to the step input are twice the values if there was a static application of force F0 12

[New Topic] Response Spectrum April 15, 2017 [New Topic] Response Spectrum Framework Assume that you are dealing with a particular forcing function such as below Response spectrum: a graph showing how the maximum response (displacement, velocity, acceleration, force, etc.) changes with the natural frequency (or period) of a SDOF system 13

[Cntd] Response Spectrum April 15, 2017 [Cntd] Response Spectrum The RS graph basically presents the worst case scenario Widely used in earthquake engineering design Once we know the RS corresponding to a specified forcing function, we need to know just the natural frequency of the system to find its maximum response Example: 14

[Text] Example: Response Spectrum April 15, 2017 [Text] Example: Response Spectrum Find the undamped RS for the sinusoidal pulse force shown below. Assume zero initial conditions and F(t) as given below 15

[Text: 4.10, pp.323] Example: Triangular Load Pulse April 15, 2017 [Text: 4.10, pp.323] Example: Triangular Load Pulse Building frame modeled as undamped SDOF system. Find response of the frame if subjected to a blast loading represented by triangular pulse shown below. 16

April 15, 2017 [AO] Example 17

[Text: 4.8, pp.320] Example: Pulse Load April 15, 2017 [Text: 4.8, pp.320] Example: Pulse Load Determine the response of a suddenly applied constant load with a limited duration td as shown. System starts at rest, no damping present. 18

April 15, 2017 [AO] Example 19

End Chapter 4: Vibration Under General Forcing Conditions April 15, 2017 End Chapter 4: Vibration Under General Forcing Conditions Begin Chapter 5: Two Degree of Freedom Systems 20