Table of contents

Volume 22

Number 5, September 2001

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PAPERS

471

An exact mathematical solution, in terms of elementary functions, is presented for the two-dimensional problem of a mass rotating on a linear spring. The two governing equations in polar coordinates are nonlinear, coupled ordinary differential equations, but they can be solved analytically in sequence. In general, the orbit of the mass is an ellipse with the fixed end of the spring located at the centre of the ellipse. The orbital frequency is identical to the natural frequency of the spring and it is independent of the amplitude of the motion (independent of the major and minor axes of the ellipse). Based on the solution the following claim is made. No matter how the mass is perturbed, within its plane of motion, the orbital frequency will remain constant. The disturbance can be infinitesimal or finite and it can cause either the total energy or the angular momentum of the system or both to increase or decrease but the orbital period will not change. It follows from the fixed end of the spring being at the ellipse's centre that the radial vibration of the mass has twice the natural frequency of the spring; i.e. two maxima and minima in one orbital period, which is not possible unless there is rotation.

477

Two student experiments involving a rotating magnetic field are described. The first experiment consists of measurements of the rotational speed of an induction motor versus its load. The second is a determination of the torque on a conductor as a function of the frequency of rotation of the magnetic field. The experiments may become a useful addition to those published earlier.

483

When the electronic partition functions of atoms or molecules are evaluated in textbooks, only the contribution of the ground state is considered. The excited states' contribution is argued to be negligible. However, a closer look shows that the partition function diverges if such states are taken into account. This paper shows that the blind use of mathematics is the reason behind this odd behaviour.

487

and

The regular-geometric-figure solution to the N-body problem is presented in a very simple way. The Newtonian formalism is used without resorting to a more involved rotating coordinate system. Those configurations occur for other kinds of interactions beyond the gravitational ones for some special values of the parameters of the forces. For the harmonic oscillator, in particular, it is shown that the N-body problem is reduced to N one-body problems.

491

Scanning tunnelling microscopes can be used to detect transitions between reversible and irreversible deformations of materials. Since the occurrence of stress-strain hysteresis is a necessary condition for the generation of material defects, and the cumulation of defects is, in turn, the underlying cause of fatigue failure, the observation of non-hysteretic reversible deformations extending over many atomic lengths implies that mechanical nanoscale devices are potentially capable of having service lives of extremely long duration.

501

and

This study assessed the effectiveness of concept maps as learning tools in developing students' conceptual understanding in a freshmen college physics laboratory course, and explored students' perceptions regarding the usefulness of concept maps in the laboratory. The intervention group participants who constructed pre- and post-laboratory concept maps scored substantially higher (on the order of 12 percentage points) on a test that assessed their conceptual understanding of the target physics concepts than participants who did not construct such maps. This difference, however, was not statistically significant. Moreover, the intervention group participants noted that concept mapping helped them to organize their knowledge and prepare for the course experiments, and promoted their understanding of the target physics content.

513

and

We present a Hamilton-Jacobi formulation of the central force problem in which the angular polar coordinate rather than time plays the role of independent variable.

519

Within the kinetic theory of an ideal gas, the flux of particles having a number density n, and average velocity bar v impinging on a plane from one side, is sometimes written in textbooks as nbar v/6 and sometimes as nbar v/4. The validity of each expression is worked out here with emphasis on their effect on the pre-factor for the expressions of the transport parameters such as viscosity, diffusion coefficient and heat conductivity. It is shown that nbar v/4 is valid in equilibrium while only when there are gradients, effectively the flux becomes nbar v/6. For the correct derivation of the transport parameters the introduction of a distribution function for the collision times or mean free paths is essential. A methodology is suggested on how to teach this subject to undergraduate and graduate students.

527

Regnault's tables of the thermodynamic properties of steam and other data were standard during much of the 19th century. To calculate them from the experimental measurements, he used a graphical method to distinguish between random and systematic errors, when both were so small that he had to plot points with an accuracy of one-hundredth of a millimetre. He did this on a large copper plate and did the curve fitting on the plate. This episode is set against the development of the drawing of experimental graphs from the mid-18th century onwards.

533

, and

We use non-relativistic perturbation theory to calculate the leading correction to the quarkonium spectrum from vacuum polarization. The correction brings the spectrum into qualitative, but not quantitative, agreement with the measured bottomonium spectrum. The calculation is appropriate for an undergraduate course in quantum mechanics.

541

, and

We describe a simple experimental arrangement for probing spatial variations in the index of refraction of air. Shadowgraph laser imaging techniques are used for the case of a horizontal cylinder heated to different temperatures which provides a highly symmetric and well defined geometry for demonstrating the usefulness of the shadowgraph approach. This experiment combines elements of geometrical and physical optics with concepts of thermal energy transfer and techniques for digital image analysis. The methodology can be adapted for the study of a wide range of optical media which exhibit variations in the index of refraction.

549

A computer model has been constructed of a long case clock standing on a resilient surface, or within a case of impaired shear stiffness, whereby the head of the clock rocks in response to the swinging of its pendulum. The equations of motion are written in matrix form, and are solved by matrix inversion. The model accounts for the tendency of such a clock to stop when its driving weight has descended to about the level of the bob of the pendulum. The model predicts that the lengthening of the suspension of the weight by insertion of a link would permit the clock to run on until the weight becomes grounded. It also predicts that use of the chiming weight as a resonant absorber, by hanging it from a tuned suspension of fixed length, not only allows such a clock to run for the full term of a wind, but improves the constancy of its rate. The effects of a link, and of the resonant absorber, have been verified experimentally.

LETTERS AND COMMENTS

L17

, and

An elementary mechanical example is discussed in which the appearance of the easiest inertial force leads naturally to two different but equivalent Lagrangians. This provides a family of simple examples to discuss gauge invariance in analytical mechanics. The physical meaning of the gauge in these examples is also analysed.

BOOK REVIEW

561

It is now accepted, virtually without question, that the equations which govern the electromagnetic fields in vacuuo are those of James Clerk Maxwell. They take the following extremely elegant and covariant form:

These equations are so familiar to the modern student of physics that they appear almost timeless in nature. All modern texts on the subject (at least those published in the last fifty years) quote them, their structure is almost assumed to be self-evident and they now possess a status similar to the laws of classical thermodynamics. The question arises as to the way in which they have attained their current exalted position and the path by which we have travelled from the myriad of experimental observations of Faraday and his contemporaries to the current refined state of abstract understanding. Who were the protagonists and how great did they labour for our current knowledge? The detailed analysis and understanding of the eighty or so years of endeavour which led from `Ampere to Einstein' has been the daunting task that Professor Olivier Darrigol has set himself. I must admit that I find it very difficult to do justice in a brief review to this monumental work of scholarship, and for my errors or omission I apologise at the outset.

Darrigol's monograph is a highly detailed and mathematical account of the historical development of electromagnetism which, fortunately for the reader, has been transcribed from the original arcane mathematical expression into modern vector notation so that one does not have to struggle with the cumbersome notation of Maxwell or the almost impenetrable notation of Heaviside to follow the detail of the physical arguments. This in itself is a great act of generosity to the reader without which this historical development would be extremely difficult to comprehend. Rather than giving a blow by blow account of this excellent text I would like to choose a few areas which have particularly impressed me.

The first is associated with the work of Gauss on magnetism. Gauss was particularly concerned that the detailed artefacts of particular experiments should not affect the underlying physics being observed. To this end he introduced the idea of reducing measurements to absolute units of distance, force and ponderable mass (pole strength) through an inverse square law of force. And to ensure that his measurements were independent of the experimental procedures adopted, he was in the habit of using several different techniques to measure the same physical quantity. Gauss was an exceptionally gifted mathematician and practical experimenter and he laid some very important foundations.

My second area is the incomparable Maxwell. He arrived on the scene when Faraday had essentially completed his life's work. Maxwell then brought to bear his formidable mathematical ability to synthesise the complete system of observations of all the disparate effects of electromagnetism through the process of mechanically modelling the systems of forces and torques. Darrigol gives a detailed account of the way in which Maxwell used complicated mechanical analogues (gears and cogs, frictionless rollers etc.) to build and translate the jumble of effects into a single mathematical structure. Without these mechanical analogues it would not have been possible for Maxwell to construct his system of mathematical equations, however when the synthesis was complete the mechanical framework could be allowed to fall away and leave the mathematical structures completely model-free. Maxwell's set of four equations have thus been raised to the status enjoyed by the relationships of classical thermodynamics. Darrigol takes pains to point out that Maxwell had no clear understanding of what for instance electric current actually was and it is worth re-quoting Maxwell on this subject:

`It is extremely improbable that when we come to understand the true nature of electrolysis we shall retain in any form the theory of molecular charges, for then we shall have obtained a secure basis on which to form a true theory of electric currents and so become independent of these provisional theories.'

After Maxwell's great work of synthesis the subject was left with electromagnetic waves travelling in an aether and a theory which cast different observations of the same phenomena in frame dependent forms. For example the theory of the force on a coil moving in a magnetic field depended upon whether the coil or source of the field were in motion (with respect to the observer). One also had the difficult problem of the lack of effect of the motion of the aether upon the velocity of electromagnetic radiation which was assumed to be its supporting medium. These problems were coped with in somewhat ad hoc ways and by the turn of the last century they could be handled reasonably quantitatively, particularly through the far-sighted work of Lorentz. Darrigol describes in intimate detail the way in which the work of Poincare, Lorentz and many others foreshadowed the developments made by Einstein. However, history has rewarded Einstein, somewhat unfairly, for his contribution to the frame invariant formalism of electromagnetism, for although his contribution was important it does so many others a considerable injustice to ignore their own contributions.

In summary I must admit to being somewhat overwhelmed by the depth and breadth of the study undertaken by Darrigol. However, for anyone who has an interest in the subject of electromagnetism I would recommend that this book be put very high on their reading list. When I first started to get to terms with it, I wondered to whom it was directed. Apart from being a work of quite monumental scholarship, I questioned for whom it was actually written. It seemed that in order to benefit from studying this text one would need to have a fair understanding of electromagnetic theory, it would help considerably to be familiar with special relativity and also to possess a nodding acquaintance with tensor calculus, although this is not essential. These requirements would appear to reduce the readership somewhat; however there are lessons to be learned here for anyone who would make progress in the study of physics. The fine minds who took part in the noble battle to systematise and understand electromagnetic theory are some of the greatest scientific thinkers in our history and although they lived before the internal combustion engine their approach to problem solving has lessons for us all today. I cannot resist at this point mentioning a quotation which Darrigol cites from Gauss (p51):

`Nil actum reputans si quid superesset agendum' (Nothing has been done if something remains to be done).

Gauss lived in an age when the philosophy, `publish or perish' was not a prerequisite of academic life and so could complete his work before rushing into print.

History has judged the characters who people Darrigol's study very well: however one is left to ponder just how well history will judge our present generations.