- •Главная
- •1.1 Напряжений и концентраторы
- •1.1.3 Концентраторы напряжения
- •1.3 Stress concentration factor
- •1.7 Elastic-plastic stress concentration
- •1.8 Joints: bolts and welds
- •3. Механические свойства конструкционных материалов
- •3.1 Напряженности испытания
- •3.2 Stress - strain diagram
- •3.3 Testing schemes
- •3.4 Strength
- •4 Прочность материалов
- •4.1 Tension and compression
- •4.2 Shear and torsion
- •4.3 Stress-strain state
- •4.4 Bending: force and moment diagrams
- •4.5 Geometrical characteristics of sections
- •4.6 Bending: stress and deformation
- •4.7 Mixed mode loading
- •4.8 Buckling
- •4.9 Statically indeterminate systems
- •4.10 Three-dimensional structures
- •References
- •5. Theory of elasticity
- •5.1 Deformation
- •5.2 Stress
- •5.3 Hooke's law
- •5.4 Plane problems
- •5.5 Torsion
- •5.6 Bending
- •5.7 Polar coordinates
- •5.8 Plates
- •5.9 Shells
- •5.10 Contact stresses
- •6.2 Distribution functions
- •6.3 Structural models of reliability
- •6.4 Limiting state
- •6.5 Dispersion
- •6.6 Durabilty
- •6.7 Design by reliability criterion
- •6.8 Risk
- •6.9 Safety classes
- •6.10 Risk : structural and social
- •References
- •7 Materials science
- •7.1 Crystalline solids
- •7.2 Mechanical properties
- •7.3 Failure
- •7.4 Phase diagrams
- •7.5 Heat treatment of metals and alloys
- •7.6 Corrosion of metals and alloys
- •7.7 Casting
- •7.8 Polymers
- •7.9 Composites
- •7.10 Forming of metals
- •8.2 Mechanical properties
- •8.3 Stress concentration
- •8.4 Defects
- •8.5 Residual Stress
- •8.6 Strength
- •8.7 Fatigue strength
- •8.8 Fracture
- •8.9 Weldability
- •References
- •9 Composites
- •9.1 Structure of composites
- •9.2 Fibers
- •9.3 Rigidity
- •9.4 Strength
- •9.5 Crack resistance
- •9.6 Optimization
- •9.7 Fatigue and temperature effect
- •9.8 Reliability
- •9.9 Joints
- •9.10 Material selection
- •References
- •10 Finite element analysis
- •10.1 Finite element method
- •10.2 Finite elements
- •10.3 Meshing
- •10.4 Boundary conditions
- •10.5 Deformation
- •10.6 Accuracy
- •10.7 Heat transfer analysis
- •10.8 Dynamics
- •10.9 Computational fluid dynamics
- •10.10 Design analysis
- •References
10.8 Dynamics
Modal
Analysis. Understanding the natural frequencies and corresponding
modes of engineering structures can help improve performance and
guarantee safety. Changing the external forces causes dynamic
effects. For example, vibrations are generated in vehicles from
motors or road conditions, in ships from waves, in airplane wings due
to turbulence, etc. The maximum stresses resulting from the vibration
are considered in engineering analysis. The stresses define the
lifetime of a structure.
Vibration
involves repetitive motion. Frequency is defined as the number of
cycles in a given time period. 10 Hertz is the same as 10 cycles per
second.
The dynamic magnification factor D is equal to
the ratio of amplitude at a given frequency to amplitude of the
static response.
The number of characteristic frequencies
of the model is equal to number of DOF in the FE model. The most
important results are within the first few natural frequencies. The
coincidence of the external vibration with the first (and smallest)
fundamental frequency results in the maximum deflection of the
structure.
The first frequency is a property of
structure. It does not change if the number of FE in the model
increases. FEM solves the eigenvalue problem with better
approximation for low frequencies. The higher the frequency, the
smaller the correspondence between the FE model and the real
situation. There is no need to predict all high frequencies for a
structure. It is possible to identify one structure from another by
the set of natural frequencies, the "finger prints" of a
structure.
The
most serious consequences occur when a power-driven device produces a
frequency at which an attached structure naturally vibrates. This
effect is called "resonance". If sufficient power is
applied, the structure can be destroyed. The major purpose of the
modal analysis is to avoid resonance. Ideally, the first mode must
have a frequency higher than any potential driving frequencies.
In
the example, the membrane of a load cell is compressed with variable
external pressure. External pressure is applied to the membrane with
a frequency of 1 / (time period) = 1 / 0.2 = 5 Hz. If the FEA shows
that the natural frequency of the membrane is about 5 Hz resonance
will take place. The load cell cannot correctly reflect the pressure
values. It is recommended to use the cell with lower frequency
external pressure. If this is not possible then the cell design must
be changed.
An increase of the modulus of elasticity E can
increase the fundamental frequency w1.
Natural frequency decreases for heavier material.
The
following linear eigenvalue problem is solved to calculate the
natural frequencies and associated mode shape of a finite element
model. Here
[K] is the structural stiffness matrix;
[M] is
the mass matrix;
wi
is the ith
natural frequency;
{Di}
is the ith
mode shape or eigenvector.
Natural frequencies and mode
shapes are the results of modal analysis. They do not depend on
static loading schemes. The force vector is a zero-element vector.
Predicting
the effects of impacts are the most common use of transient dynamics.
The second formula given shows the dependence of dynamic response on
applied force. Stiffness matrix relates forces and displacements.
Inertia is described by point accelerations. Damping effect is
defined by the velocity of the body.
Analysis of dynamic
response by FEM is shown in the example. The solutions were obtained
for a time interval Dt. The smaller the time interval the smaller the
errors.
There is a critical value Dtcritical
above which the step-by-step integration leads to significant error.
The value of Dtcritical
depends on the highest frequency of the model.
In
the example a static load had caused tensile stress to reach the
yield strength in the low-carbon steel thin plate. The dynamic
response problem of the weight dropped onto the plate from a height
of 0.5 meter is solved with nonlinear dynamic analysis. There are
damping vibrations. The dynamic magnification factor is much larger
than 1. This means that at dynamic loading the stress exceeds the
yield strength of the material and there is a residual deformation in
plate that is larger than the static one.
