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The relationship between the buckling mode and fundamental natural mode is clearly displayed and studied in detail.
The buckling mode and fundamental natural mode are dependent on the graphite fiber orientation of the SMA reinforced angle-ply laminates.
To investigate the failure mode and fundamental mechanical behaviour of novel bolted connectors and to compare their shear performance with that of conventional welded headed studs, static push-out tests were implemented on four groups of bolted connector specimens and one group of welded stud specimens.
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The coupling properties between high-order waveguide modes and fundamental resonant modes are investigated.
We design and fabricate all-fiber mode-selective couplers (MSC), which perform mode conversion between the fundamental mode in single-mode fiber (SMF) and fundamental mode in MMF.
However, the s-polarized input light can only induce one peak among surface plasmon resonance places, which comes from the coupling between the core-guided mode and the fundamental SPP mode around the central hole surface.
It has been demonstrated that the p-polarized input light can induce two peaks among surface plasmon resonance places, which come from the coupling between the core-guided mode and the fundamental surface plasmon polariton (SPP) modes at the D-shaped surface and around the central hole surface.
Even if the frequency ranges are extended to higher frequencies, it is quite difficult to get a lot of (and even infinite) resonance bands having the high absorption coefficients, and typically only a maximum of two high-order resonance modes and a fundamental mode resonance can be achieved [40, 41, 47 49].
As excessive dynamic displacement affects the long-term safety, serviceability of the bridge and comfort of the passenger, hence, main focus of study is on the dynamic displacement and fundamental mode of vibration of the bridge.
The laser spectrum just above threshold indicates that the device operates on the fundamental mode and we can clearly get the stopband of the fundamental mode when the current is 285 mA.
Lower two panels show phase and group velocities of Rayleigh waves for Mode 1 and Mode 0 (fundamental): theoretical dispersion curves (Saito, 1988) were calculated using the 1-D velocity model above (solid and dashed lines), and velocities were estimated from the simulated waveforms (triangles).
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