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Waves, Particles, and Facts

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Perception and Discovery

Part of the book series: Synthese Library ((SYLI,volume 389))

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Abstract

The logic of notions like see, observe, witness, notice, data, evidence, and facts has, for my purposes at least, been thoroughly explored. For the next few chapters I should like to see how the morals drawn from our work so far can be applied in cases of actual scientific perplexity. The present chapter, therefore, as well as the two to follow, will be addressed, not to logical exploration (as the previous chapters were), but to the application of the fruits of our study to typical cases of experimental research.

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Notes

  1. 1.

    For a fuller discussion of Young and Fresnel’s work see Mach (1926, chs. VIII–IX).

  2. 2.

    Hertz (1900, 63). Originally published in as Hertz (1887).

  3. 3.

    See, for instance, Halliday and Resnick (1962, vol. II, 1088).

References

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  • Compton, A. H. 1926. X-rays and electrons: an outline of recent X-ray theory. New York: D. Van Nostrand Company.

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  • De Broglie, Louis. 1930. An introduction to the study of wave mechanics. Trans. H. T. Flint. New York: Dutton & Co.

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  • Halliday, David, and Robert Resnick. 1962. Physics for students of science and engineering, 2nd ed. New York: John Wiley and Sons.

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  • Hertz, Heinrich. 1887. Über einen Einfluss des ultravioletten Lichts auf die elekrische Entladung. Sitzungsberichte der Königlich Preußischen Akademie der Berliner Akademie der Wissenschaft 2: 487–490.

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  • Hertz, Heinrich. 1900. Electric waves. Trans. D. E. Jones. London: Macmillan.

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Appendix

For calculations of the general case see, for example, De Broglie (1930, 146–148) (non-relativistic) and Compton (1926, 265–268 and Appendix 6) (relativistic).

Appendix

1.1 The Compton Long Wave-Length Shift Calculated for a Scattering Angle (ø) of 90°

figure f
  • X-component momentum obeys the equation \( m{v}_x=\frac{hv}{c} \)

  • and for the Y-component momentum \( m{v}_y=-\frac{h{v}^{\prime }}{c} \)

  • where v′ is the frequency of the scattered quantum.

Energy conservation is given by the formula (neglecting relativistic effects)

$$ hv=h{v}^{\prime }+\frac{1}{2}m\left({v}_x^2+{v}_y^2\right). $$

Now we have from the momentum formula that

$$ {v}_x^2+{v}_y^2=\frac{h^2}{m^2{c}^2}\left({v}^2+{v^{\prime}}^2\right). $$

Substituting this into the energy formula we obtain

$$ \frac{v-{v}^{\prime }}{v^2+{v^{\prime}}^2}=\frac{1}{2}\frac{h}{m{c}^2} $$

and putting the result in terms of the x-ray wave lengths \( \lambda =\frac{c}{v} \) and \( {\lambda}^{\prime }=\frac{c}{v^{\prime }} \) we get

$$ \frac{\lambda {\lambda}^{\prime}\left({\lambda}^{\prime }-\lambda \right)}{\lambda^2-{\lambda^{\prime}}^2}=\frac{1}{2}\frac{h}{mc}. $$

Since the shift in wave length (λ λ) is quite small in comparison with the wave length itself, λ 2 + λ ′2 = λλ approximately and

$$ {\lambda}^{\prime }-\lambda =\frac{h}{mc}. $$

This is exactly the wave-length shift as found by experiment for 90° scattering. At smaller scattering angles the shift is less, becoming zero at ø = 0°; and at ø = 180° it attains the value of 2 h/mc.

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Lund, M.D. (2018). Waves, Particles, and Facts. In: Lund, M.D. (eds) Perception and Discovery. Synthese Library, vol 389. Springer, Cham. https://doi.org/10.1007/978-3-319-69745-1_12

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