02 Fresnel Double Prism

02 Fresnel Double Prism#

Aim#

To show the interference of two coherent, virtual, sources (wavefront splitting).

Subjects#

  • 6D10 (Interference From Two Sources)

Diagram#

../../../../../_images/figure_0245.png

Fig. 619 .#

Equipment#

  • Laser.

  • Microscope objective (40x)

  • Lens, \(150 \mathrm{~mm}\).

  • Lens of short focal length (we use \(50 \mathrm{~mm}\) )

  • Double prism.

  • Viewing screen/wall.

Presentation#

Preparation#

The laserbeam is switched on and expanded using a telescope consisting of the microscope objective and the converging lens of \(150 \mathrm{~mm}\). The expanded beam is then focussed by the lens of \(50 \mathrm{~mm}\).

Presentation#

On the viewing screen, a couple of meters away we see a large circular light spot. (Blowing smoke into the lens set-up enlightens the light path).

../../../../../_images/figure_1198.png

Fig. 620 .#

When descending the biprism (apex line vertical) into the diverging beam, close to the focal point (see Figure 620), we see that the original circular light spot is refracted into two half circle segments and that in the centre these two halves overlap (see Figure 621), narrowing the original lightspot.

../../../../../_images/figure_2116.png

Fig. 621 .#

The centre shows an increase in light intensity. When the biprism is moved closer to the focal point of the \(50 \mathrm{~mm}\) lens, we will easily see that the centre contains fringes, lines of positive and negative interference. When the biprism is close to this focal point the fringe spacing is large; when the biprism is moving away from the focal point, the fringe spacing is smaller but can still be observed when the viewing screen is tilted.

Explanation#

See Figure 622. The left portion of the wavefront is refracted to the right, the right portion to the left. In the region of superposition interference occurs.

../../../../../_images/figure_331.png

Fig. 622 .#

The virtual sources \(S_{1}\) and \(S_{2}\) can be considered as separate virtual coherent sources placed a distance \(a\) apart. The separation of the fringes ( \(\Delta y\) ) is given by: \(\Delta y \approx \frac{s}{a} \lambda\) ( \(s\) being the distance between the plane of the two sources and the screen).

Remarks#

When the biprism approaches the focal point too close, the interference image becomes distorted. This happens largely due too the fact that we use spherical lenses in stead of cylindrical.

Sources#

  • Hecht, Eugene, Optics, pag. 391

  • Leybold-Heraeus, Physikalische Handblätter, pag. DK 535.412;d

  • Phywe, University Laboratory Experiments, part Vol. 1-5, pag. 2.5

  • Sutton, Richard Manliffe, Demonstration experiments in Physics, pag. 403

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