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The application of partial treatment could also alter the deflection pattern of the beam, particularly the location of the peak deflection.
Determination of the inertial torque components, too, necessitates the knowledge of the crank angle-time function, θ(t), since both the angular acceleration pattern of the beam, d2 θ b/dt 2, and the angular acceleration of the crankshaft, d2 θ/dt 2, change with the variation of the crank angle.
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Open image in new window Fig. 4 Crack pattern of the beams at bond failure.
Open image in new window Fig. 3 Crack pattern of the beams at shear failure.
When following the flexural mode, a major failure pattern of the beams, the structures demonstrated a very interesting feature – linearized deflection curves.
On the other hand, the strength and cracking pattern of the beams with stirrups are not affected when exposed to temperatures as low as −40 °C.
With the height increase of vertical direction of explosion, the failure patterns of the beam are changed from bending shear to tensile bending.
All impairments will affect the shape of the beam pattern and antenna gain.
Additionally, in order to provide a restriction on the shape of the beam pattern, a similarity constraint is enforced at the design stage.
In order to provide a control on the shape of the beam pattern, we can formulate the similarity constraint as {{{left|{mathbf{w}}-{{mathbf{w}}_{q}}right|}^{2}}le{{xi }^{2}}} (17).
The source grating provides a spatially coherent X-ray beam, the phase grating generates an interference pattern downstream of the beam and the analyser grating detects changes of the latter, when a specimen is introduced into the beam, by which retrieval of phase- and dark-field contrast is practicable.
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Justyna Jupowicz-Kozak
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