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Tunnels and Tunnelling

Geology is the most important factor that determines the nature, form and cost of a tunnel. For example, the route, design and construction of a tunnel are largely dependent on geological considerations. Estimating the cost of tunnel construction, particularly in areas of geological complexity, is uncertain. [Pg.470]

A pilot tunnel is probably the best method of exploring tunnel locations and should be used if a major-sized tunnel is to be constructed in ground that is known to have critical geological conditions. It also drains the rock ahead of the main excavation. If the inflow of water is excessive, the rock can be grouted from the pilot tunnel before the main excavation reaches the water-bearing zone. [Pg.470]

Large pianar surfaces form most of the roof in a formation that is not inciined at a high angle and strikes more or iess paraiiei to the axis of a tunnei. in tunneis in which jointed strata dip into the side at 30° or more, the up-dip side may be unstabie. Joints that are paraiiei to the axis of a tunnel and that dip at more than 45° may prove especially treacherous, leading to slabbing of the walls and fallouts from the roof. The effect of joint orientation in relation to the axis of a tunnel is given in Table 9.3. [Pg.471]

Overbreak in thinly bedded horizontal strata with joints. Ultimate overbreak occurs if no support is installed. 472 [Pg.472]

Movements along major active faults in certain parts of the world can disrupt a tunnel lining and even lead to a tunnel being offset. As a consequence, it is best to shift the alignment to avoid the fault, or, if possible, to use open cut within the active fault. [Pg.474]


Comparison between Electrochemical Electron Tunneling and Tunneling between Two Metals... [Pg.254]

Typical energy-level schemes for dipolarly unstable systems with indications of the allowed rotational, tunneling, and tunneling-rotational transitions in two limit cases, when the rotational frequency is larger than the tunneling one and when the inverse inequality takes place, are presented in Figs. 1 and 2. The expected pure rotational spectra for three concrete sets of parameter values are shown in Figs. 3 to 5. If A = 0 (or... [Pg.15]

The approach to the Rock Mechanics Site Descriptive Model was tested by predicting the rock mechanics properties of a 600 m x 180 m x 120 m rock volume at the Aspb Hard Rock Laboratory (HRL) in Sweden using limited borehole data of the type typically obtained during a site investigation (Hudson, 2002). These predicted properties were then compared with best estimate properties obtained from a study of the test rock volume using additional tunnel and tunnel borehole data. This exercise was known as the Test Case, and directly indicates how some of the input required for modelling can be specified and tested. [Pg.443]

Tunnels and tunnelling are rather specialised engineering projects that require advanced technology and know-how. Investigations for tunnels are targeted towards the determination and classification... [Pg.233]

Several factors influence the choice of a specific venous access device length and frequency of therapy patient comfort or activity ability to care for the device personal preference (physician, nurse, home health care and patient). Devices suitable for intermediate lengths of treatment (weeks to months) include PICCs, non-tunneled, and tunneled chest wall catheters. Longer therapies (months to years) favor tunneled external chest wall catheters and subcutaneous ports. Daily access would favor an external... [Pg.135]

Tunnels and Tunnelling International (1369-3999) http //www.tunnelsonline.info/ (accessed September 3, 2010). World Market Intelligence monthly. International in coverage, T T publishes technical profiles of ongoing and completed tunnels, including rail, vehicular, and pipeline projects. Covers techniques and methods, equipment, geologic conditions, safety, and environmental issues. [Pg.516]

On the other hand, spillage into underground tunnels and tunnel networks, like sewage systems, is extremely hazardous and must never be allowed to happen. [Pg.128]

IK Iskandar and FH Sayles 1997, Ground Freezing for Containment of Haz. Waste Engineering Aspects. Int. Symp. on Phys., Chem. and Ecol. of Seasonally Frozen Soils, Fairbanks Alaska 1997. IK Iskandar et al. eds. CRREL Sp Rpt 97-10, 361-369. Jones, M.B., 1982. Ground Freezing Technology Advances with Speed. Tunnels and Tunneling, December. [Pg.250]

Jones MB 1982. Ground freezing technology advances with speed. Tunnels and tunneling 14, 31. [Pg.250]

Tunnel dryers are shown in Fig. 3.15a. Wet material on trays or a conveyor belt is passed through a tunnel, and drying takes place by hot air. The airflow can be countercurrent, cocurrent, or a mixture of both. This method is usually used when the product is not free flowing. [Pg.89]

The development of scanning probe microscopies and x-ray reflectivity (see Chapter VIII) has allowed molecular-level characterization of the structure of the electrode surface after electrochemical reactions [145]. In particular, the important role of adsorbates in determining the state of an electrode surface is illustrated by scanning tunneling microscopic (STM) images of gold (III) surfaces in the presence and absence of chloride ions [153]. Electrodeposition of one metal on another can also be measured via x-ray diffraction [154]. [Pg.203]

The ability to control the position of a fine tip in order to scan surfaces with subatomic resolution has brought scanning probe microscopies to the forefront in surface imaging techniques. We discuss the two primary techniques, scanning tunneling microscopy (STM) and atomic force microscopy (AFM) the interested reader is referred to comprehensive reviews [9, 17, 18]. [Pg.294]

Since scanning tunneling microscopy requires flat conducting surfaces, it is not surprising that most of its early application was to study inorganic materials [17, 19, 20, 29-34]. These studies include investigations of catalytic metal surfaces [24, 35-37], silicon and other oxides [21], superconductors [38], gold... [Pg.294]

Fig. VIII-1. Schematic illustration of the scanning tunneling microscope (STM) and atomic force microscope (AFM). (From Ref. 9.)... Fig. VIII-1. Schematic illustration of the scanning tunneling microscope (STM) and atomic force microscope (AFM). (From Ref. 9.)...
Fig. VIII-2. Scanning tunneling microscopy images illustrating the capabilities of the technique (a) a 10-nm-square scan of a silicon(lll) crystal showing defects and terraces from Ref. 21 (b) the surface of an Ag-Au alloy electrode being electrochemically roughened at 0.2 V and 2 and 42 min after reaching 0.70 V (from Ref. 22) (c) an island of CO molecules on a platinum surface formed by sliding the molecules along the surface with the STM tip (from Ref. 41). Fig. VIII-2. Scanning tunneling microscopy images illustrating the capabilities of the technique (a) a 10-nm-square scan of a silicon(lll) crystal showing defects and terraces from Ref. 21 (b) the surface of an Ag-Au alloy electrode being electrochemically roughened at 0.2 V and 2 and 42 min after reaching 0.70 V (from Ref. 22) (c) an island of CO molecules on a platinum surface formed by sliding the molecules along the surface with the STM tip (from Ref. 41).
While field ion microscopy has provided an effective means to visualize surface atoms and adsorbates, field emission is the preferred technique for measurement of the energetic properties of the surface. The effect of an applied field on the rate of electron emission was described by Fowler and Nordheim [65] and is shown schematically in Fig. Vlll 5. In the absence of a field, a barrier corresponding to the thermionic work function, prevents electrons from escaping from the Fermi level. An applied field, reduces this barrier to 4> - F, where the potential V decreases linearly with distance according to V = xF. Quantum-mechanical tunneling is now possible through this finite barrier, and the solufion for an electron in a finite potential box gives... [Pg.300]

We have considered briefly the important macroscopic description of a solid adsorbent, namely, its speciflc surface area, its possible fractal nature, and if porous, its pore size distribution. In addition, it is important to know as much as possible about the microscopic structure of the surface, and contemporary surface spectroscopic and diffraction techniques, discussed in Chapter VIII, provide a good deal of such information (see also Refs. 55 and 56 for short general reviews, and the monograph by Somoijai [57]). Scanning tunneling microscopy (STM) and atomic force microscopy (AFT) are now widely used to obtain the structure of surfaces and of adsorbed layers on a molecular scale (see Chapter VIII, Section XVIII-2B, and Ref. 58). On a less informative and more statistical basis are site energy distributions (Section XVII-14) there is also the somewhat laige-scale type of structure due to surface imperfections and dislocations (Section VII-4D and Fig. XVIII-14). [Pg.581]

We confine ourselves here to scanning probe microscopies (see Section VIII-2B) scanning tunneling microscopy (STM) and atomic force microscopy (AFM), in which successive profiles of a surface (see Fig. VIII-1) are combined to provide a contour map of a surface. It is conventional to display a map in terms of dark to light areas, in order of increasing height above the surface ordinary contour maps would be confusing to the eye. [Pg.688]

There has been a general updating of the material in all the chapters the treatment of films at the liquid-air and liquid-solid interfaces has been expanded, particularly in the area of contemporary techniques and that of macromolecular films. The scanning microscopies (tunneling and atomic force) now contribute more prominently. The topic of heterogeneous catalysis has been expanded to include the well-studied case of oxidation of carbon monoxide on metals, and there is now more emphasis on the flexible surface, that is, the restructuring of surfaces when adsorption occurs. New calculational methods are discussed. [Pg.802]

At a surface, not only can the atomic structure differ from the bulk, but electronic energy levels are present that do not exist in the bulk band structure. These are referred to as surface states . If the states are occupied, they can easily be measured with photoelectron spectroscopy (described in section A 1.7.5.1 and section Bl.25.2). If the states are unoccupied, a teclmique such as inverse photoemission or x-ray absorption is required [22, 23]. Also, note that STM has been used to measure surface states by monitoring the tunnelling current as a fiinction of the bias voltage [24] (see section BT20). This is sometimes called scamiing tuimelling spectroscopy (STS). [Pg.293]

Binnig G and Rohrer FI 1987 Scanning tunneling microscopy—from birth to adolescence Rev. Mod. Rhys. 59 615... [Pg.319]

Marrian C R K, Perkins F K, Brandow S L, Koloski T S, Dobisz E A and Calvert J M 1994 Low voltage electron beam lithography in self-assembled ultrathin films with the scanning tunneling microscope Appi. Rhys. Lett. 64 390... [Pg.319]

Stroscio J A and Eigler D M 1991 Atomic and molecular manipulation with the scanning tunneling microscope Science 254 319... [Pg.319]

Eigler D M and Schweizer E K 1990 Positioning single atoms with a scanning tunneling microscope Nature 344 524... [Pg.319]

Stipe B C, Rezaei M A, Flo W, Gao S, Persson M and Lundqvist B I 1997 Single-molecule dissociation by tunneling electrons Rhys. Rev. Lett. 78 4410... [Pg.319]

Drake B, Sonnenfeld R, Schneir J and Hansma P K 1987 Scanning tunneling microscopy of process at liquid-solid interfaces Surf. Sc/. 181 92... [Pg.320]

Giancarlo L C and Flynn G W 1988 Scanning tunneling and atomic force microscopy probes of self-assembled, physisorbed monolayers A/ / . Rev. Phys. Chem. 49 297... [Pg.320]

Schneir J, Harary H H, Dagata J A, Hansma P Kand Sonnenfeld R 1989 Scanning tunneling microscopy and fabrication of nanometer scale structure at the liquid-gold interface Scanning Microsc. 3 719... [Pg.320]

Pine A S, Lafferty W J and Howard B J 1984 Vibrational predissociation, tunneling, and rotational saturation in the HF and DF dimers J. Chem. Phys. 81 2939-50... [Pg.794]

Luntz A C and Harris J 1992 The role of tunneling in precursor mediated dissociation Alkanes on metal surfaces J. [Pg.919]

The importance of low pressures has already been stressed as a criterion for surface science studies. However, it is also a limitation because real-world phenomena do not occur in a controlled vacuum. Instead, they occur at atmospheric pressures or higher, often at elevated temperatures, and in conditions of humidity or even contamination. Hence, a major tlmist in surface science has been to modify existmg techniques and equipment to pemiit detailed surface analysis under conditions that are less than ideal. The scamiing tunnelling microscope (STM) is a recent addition to the surface science arsenal and has the capability of providing atomic-scale infomiation at ambient pressures and elevated temperatures. Incredible insight into the nature of surface reactions has been achieved by means of the STM and other in situ teclmiques. [Pg.921]

Moffat T P, Fan FRF and Bard A 1991 Electrochemical and scanning tunneling microscopic study of dealloying of CUjAu J. Electrochem. Soc. 138 3224... [Pg.954]

The probability matrix plays an important role in many processes in chemical physics. For chemical reactions, the probability of reaction is often limited by tunnelling tlnough a barrier, or by the fonnation of metastable states (resonances) in an intennediate well. Equivalently, the conductivity of a molecular wire is related to the probability of transmission of conduction electrons tlttough the junction region between the wire and the electrodes to which the wire is attached. [Pg.964]

The obvious defect of classical trajectories is that they do not describe quantum effects. The best known of these effects is tunnelling tln-ough barriers, but there are others, such as effects due to quantization of the reagents and products and there are a variety of interference effects as well. To circumvent this deficiency, one can sometimes use semiclassical approximations such as WKB theory. WKB theory is specifically for motion of a particle in one dimension, but the generalizations of this theory to motion in tliree dimensions are known and will be mentioned at the end of this section. More complete descriptions of WKB theory can be found in many standard texts [1, 2, 3, 4 and 5, 18]. [Pg.999]

Gatti F, lung C, Leforestier C and Chapuisat X 1999 Fully coupled 6D calculations of the ammonia vibration-inversion-tunneling states with a split Hamiltonian pseudospectral approach J. Chem. Phys. Ill 7236 3... [Pg.1088]

Fehrensen B, Luckhaus D and Quack M 1999 Mode selective stereomutation tunnelling in hydrogen peroxide isotopomers Chem. Phys. Lett. 300 312-20... [Pg.1088]

H1] Qiu Y and Bai Z 1998 Vibration-rotation-tunneling dynamics of (HF)2 and (HCI)2 from fulldimensional quantum bound state calculations Advances in Moiecuiar Vibrations and Coiiision Dynamics, Voi. i-ii Moiecuiar dusters ed J Bowman and Z Bai (JAI Press) pp 183-204... [Pg.1088]


See other pages where Tunnels and Tunnelling is mentioned: [Pg.350]    [Pg.350]    [Pg.254]    [Pg.470]    [Pg.183]    [Pg.203]    [Pg.270]    [Pg.293]    [Pg.294]    [Pg.294]    [Pg.297]    [Pg.634]    [Pg.685]    [Pg.711]    [Pg.18]    [Pg.69]    [Pg.76]    [Pg.604]    [Pg.604]    [Pg.1028]    [Pg.1032]    [Pg.1032]   


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AFM and STM in Photochemistry Including Photon Tunneling (Kaupp)

Atomic forces and tunneling

Attractive atomic force and tunneling conductance

Band and Tunnel Dryers

Barriers and Tunneling Splittings

Case 1 Route 8 Nam Wan Tunnel and West Tsing Yi Viaduct

Coherent Proton Tunneling in Hydrogen Bonds of Isolated Molecules Malonaldehyde and Tropolone

Determination of Caustics and Propagation in Tunneling Region

Electron tunneling in micelles and vesicles

Electron tunneling in reactions involving chlorophyll and its synthetic analogues

Electron tunneling reactions between inorganic ion radicals and transition metal compounds

Extremely high kinetic isotope effects and tunneling

Free Energy and Temperature Dependence of Tunneling

Highways, tunnels, and bridges

Hydrogen Tunnelling and Enzyme Catalysis

Hydrogen diffusion and tunnelling

Hydrogen in metals structure, diffusion and tunnelling

Incoherent Tunneling and the Bell Model

Influence of higher-order tunneling processes and a finite cooling rate

Isotope effects and quantum tunneling

Kinetic Isotope Effects Continued Variational Transition State Theory and Tunneling

North LGV requirements and the Channel Tunnel

Quantum tunneling and activated flow of particles

Raman and Fluorescence Spectroscopy Coupled with Scanning Tunneling Microscopy

Reductase Hydrogen Tunneling and Protein Motion

Scanning Tunneling Microscopy and Its Derivatives

Scanning tunneling microscopy and related methods

Secondary deuterium KIEs and tunnelling

Special Topic 5.2 Isotope effects and tunnelling

Symmetry-breaking and Tunneling in

Tafel Slopes and Proton Tunneling

Theory of Scanning Tunneling Microscopy and Applications in Catalysis

Thermally activated reorientations and tunnel relaxation of orientational states in a phonon field

Tunnel and coupled motions

Tunnel-Diodes and Catalytic Bias

Tunneling Scattering and Bridge Effect

Tunneling and related effects

Tunneling as a contribution to catalysis prospects and problems

Tunneling in Jahn-Teller Systems and Multidimensional WKB Approximation

Tunneling, Transmission, and Reflection

Tunnelling, and

Tunnelling, and

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