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1

Toro, E. F. Random-choice based hybrid methods for one and two dimensional gas dynamics. College of Aeronautics, Cranfield Institute of Technology, 1988.

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2

Patin, R. M. A one-dimensional simulation model for a two stage light gas gun with deformable piston. AIAA, 1986.

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3

Witte, David W. Computer code for determination of thermally perfect gas properties. National Aeronautics and Space Administration, Langley Research Center, 1994.

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4

E, Tatum Kenneth, and Langley Research Center, eds. Computer code for determination of thermally perfect gas properties. National Aeronautics and Space Administration, Langley Research Center, 1994.

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5

J, Kelly M. Low-dimensional semiconductors: Materials, physics, technology, devices. Clarendon Press, 1995.

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6

NATO Advanced Research Workshop on Optical Properties of Narrow-Gap Low-Dimensional Structures (1986 St. Andrews, Scotland). Optical properties of narrow-gap low-dimensional structures. Plenum Press, 1987.

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7

Tuenter, Hans J. H. Worst-case bounds for bin-packing heuristics with applications to the duality gap of the one-dimensional cutting stock problem. University of Birmingham, 1996.

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8

Thyagaraja, A., and D. F. Fletcher. CUDGEL: A One-dimensional Transient Simulation of Excimer Laser Gas Dynamics (Reports). AEA Technology Plc, 1989.

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9

Ferguson, Roderick A. One-Dimensional Queer. Polity Press, 2018.

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10

Ferguson, Roderick A. One-Dimensional Queer. Polity Press, 2018.

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11

One-Dimensional Queer. Polity, 2018.

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12

Escudier, Marcel. Compressible pipe flow. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198719878.003.0013.

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In this chapter gas flow through pipes is analysed, taking account of compressibility and either friction or heat exchange with the fluid. It is shown that in all cases the key parameter is the Mach number. The analyses are based upon the conservation laws for mass, momentum, and energy, together with an equation of state. So that significant results can be achieved, the flowing fluid is treated as a perfect gas, and the flow as one dimensional. Adiabatic pipe flow with wall friction is termed Fanno flow. Frictionless pipe flow with heat transfer is termed Rayleigh flow. It is found that both
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13

Escudier, Marcel. Compressible fluid flow. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198719878.003.0011.

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Compressible-gas flow through convergent and convergent-divergent nozzles is analysed in this chapter based upon the conservation laws for mass, momentum, and energy, together with considerations of thermodynamics. It is shown that in both cases the key parameter in describing the flow is the Mach number, which is used to distinguish between subsonic and supersonic flow. So that significant results can be achieved, the flowing fluid is treated as a perfect gas, and the flow as one dimensional. Flow through a convergent nozzle and the choking limitation is discussed. Flow through a normal shock
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14

de Bruijne, Arnoud, Joop van Buren, Anton Kösters, and Hans van der Marel. Geodetic reference frames in the Netherlands. Nederlandse Commissie voor Geodesie, 2005. http://dx.doi.org/10.54419/vy3c94.

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Unambiguous and homogeneous geodetic reference frames are essential to the proper determination of locations and heights. The reference frames used in the Netherlands are the Rijksdriehoekmeting (RD) for locations and the Normaal Amsterdamse Peil (NAP) for heights. The RD has traditionally been managed by the Kadaster; the NAP by Rijkswaterstaat. The emergence of satellite positioning has resulted in drastic changes to these geodetic reference frames. A surveyor is now offered one instrument, GPS (the Global Positioning System), capable of the simultaneous determination of locations and height
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15

Levin, Frank S. Surfing the Quantum World. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198808275.001.0001.

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Surfing the Quantum World bridges the gap between in-depth textbooks and typical popular science books on quantum ideas and phenomena. Among its significant features is the description of a host of mind-bending phenomena, such as a quantum object being in two places at once or a certain minus sign being the most consequential in the universe. Much of its first part is historical, starting with the ancient Greeks and their concepts of light, and ending with the creation of quantum mechanics. The second part begins by applying quantum mechanics and its probability nature to a pedagogical system,
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