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| 1 | +import math |
| 2 | + |
| 3 | +""" |
| 4 | +Finding the intensity of light transmitted through a polariser using Malus Law |
| 5 | +and by taking initial intensity and angle between polariser and axis as input |
| 6 | +
|
| 7 | +Description : Malus's law, which is named after Étienne-Louis Malus, |
| 8 | +says that when a perfect polarizer is placed in a polarized |
| 9 | +beam of light, the irradiance, I, of the light that passes |
| 10 | +through is given by |
| 11 | + I=I'cos²θ |
| 12 | +where I' is the initial intensity and θ is the angle between the light's |
| 13 | +initial polarization direction and the axis of the polarizer. |
| 14 | +A beam of unpolarized light can be thought of as containing a |
| 15 | +uniform mixture of linear polarizations at all possible angles. |
| 16 | +Since the average value of cos²θ is 1/2, the transmission coefficient becomes |
| 17 | +I/I' = 1/2 |
| 18 | +In practice, some light is lost in the polarizer and the actual transmission |
| 19 | +will be somewhat lower than this, around 38% for Polaroid-type polarizers but |
| 20 | +considerably higher (>49.9%) for some birefringent prism types. |
| 21 | +If two polarizers are placed one after another (the second polarizer is |
| 22 | +generally called an analyzer), the mutual angle between their polarizing axes |
| 23 | +gives the value of θ in Malus's law. If the two axes are orthogonal, the |
| 24 | +polarizers are crossed and in theory no light is transmitted, though again |
| 25 | +practically speaking no polarizer is perfect and the transmission is not exactly |
| 26 | +zero (for example, crossed Polaroid sheets appear slightly blue in colour because |
| 27 | +their extinction ratio is better in the red). If a transparent object is placed |
| 28 | +between the crossed polarizers, any polarization effects present in the sample |
| 29 | +(such as birefringence) will be shown as an increase in transmission. |
| 30 | +This effect is used in polarimetry to measure the optical activity of a sample. |
| 31 | +Real polarizers are also not perfect blockers of the polarization orthogonal to |
| 32 | +their polarization axis; the ratio of the transmission of the unwanted component |
| 33 | +to the wanted component is called the extinction ratio, and varies from around |
| 34 | +1:500 for Polaroid to about 1:106 for Glan–Taylor prism polarizers. |
| 35 | +
|
| 36 | +Reference : "https://en.wikipedia.org/wiki/Polarizer#Malus's_law_and_other_properties" |
| 37 | +""" |
| 38 | + |
| 39 | + |
| 40 | +def malus_law(initial_intensity: float, angle: float) -> float: |
| 41 | + """ |
| 42 | + >>> round(malus_law(10,45),2) |
| 43 | + 5.0 |
| 44 | + >>> round(malus_law(100,60),2) |
| 45 | + 25.0 |
| 46 | + >>> round(malus_law(50,150),2) |
| 47 | + 37.5 |
| 48 | + >>> round(malus_law(75,270),2) |
| 49 | + 0.0 |
| 50 | + >>> round(malus_law(10,-900),2) |
| 51 | + Traceback (most recent call last): |
| 52 | + ... |
| 53 | + ValueError: In Malus Law, the angle is in the range 0-360 degrees |
| 54 | + >>> round(malus_law(10,900),2) |
| 55 | + Traceback (most recent call last): |
| 56 | + ... |
| 57 | + ValueError: In Malus Law, the angle is in the range 0-360 degrees |
| 58 | + >>> round(malus_law(-100,900),2) |
| 59 | + Traceback (most recent call last): |
| 60 | + ... |
| 61 | + ValueError: The value of intensity cannot be negative |
| 62 | + >>> round(malus_law(100,180),2) |
| 63 | + 100.0 |
| 64 | + >>> round(malus_law(100,360),2) |
| 65 | + 100.0 |
| 66 | + """ |
| 67 | + |
| 68 | + if initial_intensity < 0: |
| 69 | + raise ValueError("The value of intensity cannot be negative") |
| 70 | + # handling of negative values of initial intensity |
| 71 | + if angle < 0 or angle > 360: |
| 72 | + raise ValueError("In Malus Law, the angle is in the range 0-360 degrees") |
| 73 | + # handling of values out of allowed range |
| 74 | + return initial_intensity * (math.cos(math.radians(angle)) ** 2) |
| 75 | + |
| 76 | + |
| 77 | +if __name__ == "__main__": |
| 78 | + import doctest |
| 79 | + |
| 80 | + doctest.testmod(name="malus_law") |
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