Archives de catégorie : Carnot

Sadi Carnot

ANALOGY BETWEEN OPTICAL RAYS AND NONRELATIVISTIC PARTICLE TRAJECTORIES : A COMMENT

J. A. Arnaud

Am. J. Phys. 44, 1067 (1976)

ABSTRACT

The identification, medium refractive indexn = nonrelativistic particle velocityv, in the analogy of geometrical optics with nonrelativistic particle mechanics is physically correct and useful, but can easily be misinterpreted. The conditions under which the analogy holds are outlined. The significance of Descartes’s mechanical models is also discussed.

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EFFECT OF POLARISATION ON PULSE BROADENING IN MULTIMODE GRADED-INDEX OPTICAL FIBRES

J. A. Arnaud

Electronics Letters, Volume 11, Issue 23, 13 November 1975, p. 554 – 556

ABSTRACT

A formulation of ray optics that takes the polarisation of electromagnetic waves into account shows that the maximum difference in time delay between corresponding HE and EH modes is, for almost any multimode graded-index fibre, of the order of 10 000 (Δn/n)2/V ns/km, where V is the V-number of the fibre and Δn is the variation of the refractive index between axis and cladding. The effect of polarisation on pulse broadening is found to be negligible if the V-number of the fibre is much larger than about 20.

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COMMENTS ON : « RADIATION FROM CURVED DIELECTRIC SLABS AND FIBERS « 

J. A. Arnaud

Microwave Theory and Techniques, IEEE Transactions on  (Volume:23 ,  Issue: 11), pages 935 – 936, Nov. 1975

ABSTRACT

In the above paper, Lewin gave an expression for the bending loss of a dielectric fiber with circular cross section. I have shown that the bending loss of arbitrary optical guides can be obtained in a simple manner when the field of the straight guide is known. The purpose of this letter is to show that the results of the two theories are in agreement, except for a factor of 2.

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APPLICATION OF A PROPERTY OF THE AIRY FUNCTION TO FIBER OPTICS (SHORT PAPER)

J. Arnaud, W. Mammel 

IEEE Transactions on Microwave Theory and Techniques, (Volume:23,  Issue: 11), Pages 927–929, Nov 1975

ABSTRACT

The integral of the square of the Airy function from one of its zeros to infinity is equal to the square of the first derivative of the Airy function at the zero considered. Two important applications of this result to fiber optics are discussed.

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TRANSVERSE COUPLING IN FIBER OPTICS IV : CROSSTALK

J. A. Arnaud

Bell System Technical Journal, The  (Volume:54 ,  Issue: 8 ), pages 1431 – 1450, Oct. 1975

ABSTRACT

We evaluate the crosstalk between adjacent cores in an optical fiber that results from electromagnetic coupling. Means of reducing it are discussed. We find that a 0.5-μm-thick layer of silver can, in principle, reduce the crosstalk from −20 to −130 dB without significant increase of the loss. These theoretical results are obtained for two identical single-mode dielectric slabs. In reality, the slabs are not rigorously identical. Longitudinal fluctuations of slab thickness reduce the crosstalk by at least 40 dB. The slab spacing can accordingly be reduced from, typically, 11 to 6 μm for a constant crosstalk. If the slabs are made dissimilar with a relative difference in thickness of 10 percent, the spacing can be reduced further, to approximately 1.5 times the slab thickness. For example, a 15-μm spacing is required between single-mode dissimilar slabs if the nominal slab thickness is 10 μm, provided scattering can be neglected.

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PULSE BROADENING IN MULTIMODE OPTICAL FIBERS

J. A. Arnaud

Bell System Technical Journal, The  (Volume: 54 ,  Issue: 7 ), pages 1179 – 1205, Sept. 1975

ABSTRACT

Closed-form expressions are obtained for the impulse response of graded-index fibers whose relative permittivity is a homogeneous function of the two transverse coordinates x, y, and for the impulse width in graded-index fibers whose profile departs slightly, but otherwise arbitrarily, from a square law. The inhomogeneous dispersion of the material is taken into account. Pulse broadening can be reduced by a factor of 12 from the value obtained for square-law fibers. Simple expressions are found for the acceptance of highly oversized fibers.

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PULSE BROADENING IN NEAR-SQUARE-LAW GRADED-INDEX FIBRES

J. A. Arnaud

Electronics Letters, Volume 11, Issue 18, 4 September 1975, p. 447 – 448

ABSTRACT

A closed-form expression for pulse broadening in graded-index fibres that have small and circularly symmetric, but otherwise arbitrary, deviations from a square-law, and arbitrary dn/dλ, is applied to germania-doped fibres. The range of validity of the theoretical expression is defined by comparison with the results of numerical integration.

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GUIDANCE OF 100 GHZ BEAMS BY CYLINDRICAL MIRRORS

J. A. Arnaud, J. T. Ruscio

Microwave Theory and Techniques, IEEE Transactions on  (Volume:23 ,  Issue: 4 ), pages 377 – 379, Apr 1975

ABSTRACT

Microwave beams can be kept confined by sequences of pairs of cylindrical mirrors, each pair acting as a lens. At 100 GHz, with 1.2-m x 1.2-m focusers spaced 80 m apart, a loss of the order of 2 dB/km has been measured in clear weather. The use of this beam-guiding arrangement, called a « Hertzian cable, » for distribution of information in cities is discussed.

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APPLICATION OF THE MECHANICAL THEORY OF LIGHT TO FIBER OPTICS

J. A. Arnaud

Journal of Optical Society of America, vol. 65, n° 2, February 1975

ABSTRACT

The motion of charged particle in a space- and time – dependent potential and the motion of an optical pulse in an inhomogeneous anisotropic medium coincide when the dispersion surfaces are the same.

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RESONANT-GRID QUASI-OPTICAL DIPLEXERS

J.A. Arnaud, F. A. Pelow

Bell System Technical Journal, 1975,  (Volume:54 ,  Issue: 2 ), 263 – 283

ABSTRACT

Experimental results are reported concerning the transmission, reflection, and depolarization of metal grids that reflect an upper band, centered at 30 GHz, and transmit a lower band, centered at 20 GHz. With a single grid, the transmission loss is less than 0.1 dB, and the rejection exceeds 44 dB. Depolarization is measured under realistic conditions with direct dual-mode feed excitation. In a 10-percent band, depolarization is below 34 dB at all scanning angles for both the transmitted and reflected waves. Experiments with two parallel resonant grids are also reported.

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