Sentence examples for mode of bulk from inspiring English sources

The most efficient mode of bulk transport for petroleum is the network of pipelines that are now found all over the world.

The Raman spectra of both nanowire and bulk InAs have been normalized with respect to the intensity of the TO phonon mode of bulk InAs for easy comparison.

In addition, the TO mode of InAs NWs exhibits a downshift of about 2 to 3 comparedpared to the TO mode of bulk ZB InAs.

Recently, the size dependence of mechanical behaviors, particularly the yield strength and plastic deformation mode, of bulk metallic glasses (BMG) has created a great deal of interest.

The first-order Raman scattering of the Γ-point mode of bulk silicon gives a line at 521 cm−1, and as Figure 2 shows, the LH aerogel composites show a line close to this position (with a Lorentzian lineshape, centre at 522 cm−1, FWHM 12 to 14 cm−14.

A theory for heterogeneous flame propagation in the self-propagating, high-temperature synthesis (SHS) process that proceeds in multi-layer foils consisting of alternating layers of constituents has been formulated, describing a pre-mixed mode of bulk flame propagation supported by a non-pre-mixed reaction that proceeds at the layer surface of a constituent with higher melting point.

In particular, we study the effect of squeezed-film damping on the behaviour of high frequency, higher order resonant modes of bulk resonators.

For bulk InAs materials, two Raman peaks are clearly observed: one is located around 241.0 cm-1, the other around 218.7 cm-1, which can be attributed to the LO and TO phonon modes of bulk InAs.

After nanocatalyst preparation, the wavenumber is shifted from 610 to 640 cm−1 and of sharp bands at 636 and 1609 cm−1, corresponding to Si O stretching modes of bulk sulphates, mainly MnSO4, in agreement with data from XRD Fig. 2.

A typical Raman spectrum of as-achieved SiC nanochains is shown in Figure 7. Two feature peaks at around 783 and 930 cm-1 could be assigned to the TO and LO phonon peaks of cubic SiC crystal, respectively, and a shift of 13 cm-1 and 42 cm-1 are observed comparing with the modes of bulk SiC [32, 33].

We show that a practical way to achieve this imperative is to consider the radial mode of actuation of bulk PZT elements.