Two-degree-of-freedom System with Translation & Rotation

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Presentation transcript:

Two-degree-of-freedom System with Translation & Rotation Unit 45 Vibrationdata Two-degree-of-freedom System with Translation & Rotation

Introduction Vibrationdata Rotational degree-of-freedom dynamic problem requires mass moment of inertia Measure, calculate, or estimate MOI

Measure Inertia via Bifilar Pendulum Vibrationdata

Two-Plane Spin Balance Vibrationdata

Inertia & Radius of Gyration Vibrationdata

Rectangular Prism Vibrationdata Y c a b Z X

Vibrationdata Inertia & Radius of Gyration m is the mass The mass moment of inertia J m is the mass r is the radius of gyration - The distance from an axis at which the mass of a body may be assumed to be concentrated and at which the moment of inertia will be equal to the moment of inertia of the actual mass about the axis, equal to the square root of the quotient of the moment of inertia and the mass.

Vibrationdata Avionics Component What is mass moment of inertia? Seldom if ever have measurements Could treat as solid block with constant mass density Or just estimate radius of gyration

Vibrationdata Two DOF Example  x L1 L2 m mass J m, J k 1 L1 k 2 L2 x m mass J mass moment of inertia about the C.G. k spring stiffness L length from spring attachment to C.G.

Vibrationdata Free Body Diagram L2 L1 x k2 (x+L2) k1 (x-L1) Reference k2 (x+L2) k1 (x-L1) L1 L2  Derive two equations of motion

Vibrationdata Equations of Motion Assemble equation into matrix form. The vibration modes have translation and rotation which will be coupled if The natural frequencies are found via the eigenvalue problem:

Vibrationdata Sample Values Variable Value m 3200 lbm - L1 4.5 ft 54 in L2 5.5 ft 66 in k1 2400 lbf / ft 200 lbf/in k2 2600 lbf / ft 217 lbf/in R 4.0 ft 48 in From Thomson, Theory of Vibration with Applications

Vibrationdata vibrationdata > Structural Dynamics > Two-DOF System Natural Frequencies

Vibrationdata

Vibrationdata Natural Frequency Results mass matrix 8.29 0 0 1.91e+04 8.29 0 0 1.91e+04 stiffness matrix 417 1482 1482 1.504e+06 Natural Frequencies No. f(Hz) 1. 1.1234 2. 1.4166 Modes Shapes (column format) 0.3445 0.0444 -0.0009 0.0072

Vibrationdata C.G. Combined rotation and translation

Vibrationdata C.G. Combined rotation and translation

Vibrationdata Apply Base Excitation The corresponding base excitation problem is complicated because the base motion directly couples with each of the two different degree-of-freedom types Thus use an “enforced motion” approach Must add a base mass for this method Motion will then be enforced on the base degree-of-freedom The mass value of the base is arbitrary

Three Dof System Vibrationdata  m2, J k 1 L1 k 2 L2 x2 m1 x1

Vibrationdata Free Body Diagram L2 L1  k2 (x2+L2 - x1)

Derive Equation of Motion Vibrationdata Homogeneous for now

Vibrationdata Avionics Component Partition the matrices and vectors as follows where the displacement vector is Subscripts d is driven f is free

Vibrationdata Transformation Matrix I is the identify matrix where I is the identify matrix

Vibrationdata Decoupling via Transformation Matrix Let Intermediate goal is to decouple the partition-wise stiffness matrix. Let Substitute transformed displacement and pre-multiply mass and stiffness matrices by T as follows

Apply Transformation Matrix Vibrationdata

Vibrationdata Avionics Component The equation of motion is thus Non-homogenous term due to enforce acceleration The final displacement are found via The equation of motion can solved either in the frequency or time domain.

Vibrationdata Reference Too many equations for a Webinar! Further details given in: T. Irvine, Spring-Mass System Subjected to Enforced Motion, Vibrationdata, 2015 Similar to Craig-Bampton modeling Damping can be applied later as modal damping

Vibrationdata Sample Avionics Box with C.G. Offset Variable Value m 5 lbm L1 3 in L2 5 in k1 2000 lbf/in k2 R 2 in Calculate natural frequencies, modes, shapes and frequency response functions for base excitation Q= 10 for both modes

Vibrationdata vibrationdata > Structural Dynamics > Two-DOF System Base Excitation

Avionics Component Vibrationdata Next Enter Uniform Damping Q=10

Vibrationdata Natural Frequency Results mass matrix 0.01295 0 0.01295 0 0 0.05181 stiffness matrix 4000 4000 4000 6.8e+04 Natural Frequencies No. f(Hz) 1. 85.052 2. 183.93 Modes Shapes (column format) 8.6887 1.3065 -0.6532 4.3443

Vibrationdata

Transmissibility Vibrationdata

Translational Acceleration Transmissibility Vibrationdata

Rotational Acceleration Transmissibility Vibrationdata

Relative Displacement Transmissibility Vibrationdata

Angular Displacement Transmissibility Vibrationdata

Vibrationdata Import: SRS 2000G Acceleration & NAVMAT PSD Specification

Vibrationdata Apply the Navmat PSD as the base input.

Angular Displacement Transmissibility Vibrationdata

Vibrationdata

Vibrationdata

Angular Displacement Transmissibility Vibrationdata

Angular Displacement Transmissibility Vibrationdata

Angular Displacement Transmissibility Vibrationdata

Angular Displacement Transmissibility Vibrationdata