18禁黄无码免费网站高潮丨国产av天堂无码一区二区三区丨中国猛少妇色xxxxx丨无码网站天天爽免费看视频丨97国产精品人妻无码久久久

撥號(hào)18861759551

你的位置:首頁(yè) > 技術(shù)文章 > 光學(xué)101:1級(jí)理論基礎(chǔ)

技術(shù)文章

光學(xué)101:1級(jí)理論基礎(chǔ)

技術(shù)文章

Optics 101: Level 1 Theoretical Foundations

The Electromagnetic Spectrum | Interference | Reflection| Refraction | Dispersion | Diffraction

 

Optics is the branch of physics that deals with light and its properties and behavior. It is a vast science covering many simple and complex subjects ranging from the reflection of light off a metallic surface to create an image, to the interaction of multiple layers of coating to create a high optical density rugate notch filter. As such, it is important to learn the basic theoretical foundations governing the electromagnetic spectrum, interference, reflection, refraction, dispersion, and diffraction before picking the best component for one's optics, imaging, and/or photonics applications.

 

THE ELECTROMAGNETIC SPECTRUM

Light is a type of electromagnetic radiation usually characterized by the length of the radiation of interest, specified in terms of wavelength, or lambda (λ). Wavelength is commonly measured in nm (10-9 meters) or μm (10-6 meters). The electromagnetic spectrum encompasses all wavelengths of radiation ranging from long wavelengths (radio waves) to very short wavelengths (gamma rays); Figure 1 illustrates this vast spectrum. The most relevant wavelengths to optics are the ultraviolet, visible, and infrared ranges. Ultraviolet (UV) rays, defined as 1– 400nm, are used in tanning beds and are responsible for sunburns. Visible rays, defined as 400 - 750nm, comprise the part of the spectrum that can be perceived by the human eye and make up the colors people see. The visible range is responsible for rainbows and the familiar ROYGBIV - the mnemonic many learn in school to help memorize the wavelengths of visible light starting with the longest wavelength to the shortest. Lastly, infrared (IR) rays, defined as 750nm – 1000μm, are used in heating applications. IR radiation can be broken up further into near-infrared (750nm - 3μm), mid-wave infrared (3 - 30μm) and far-infrared (30 – 1000μm).

 

Figure 1: Electromagnetic Spectrum

 

INTERFERENCE

Isaac Newton (1643 - 1727) was one of the first physicists to propose that light was comprised of small particles. A century later, Thomas Young (1773 - 1829) proposed a new theory of light which demonstrated light's wave qualities. In his double-slit experiment, Young passed light through two closely spaced slits and found that the light interfered with itself (Figure 2). This interference could not be explained if light was purely a particle, but could if light was a wave. Though light has both particle and wave characteristics, known as the wave-particle duality, the wave theory of light is important in optics while the particle theory in other branches of physics.

 

Interference occurs when two or more waves of light add together to form a new pattern. Constructive interference occurs when the troughs of the waves align with each other, while destructive interference occurs when the troughs of one wave align with the peaks of the other (Figure 3). In Figure 3, the peaks are indicated with blue and the troughs with red and yellow. Constructive interference of two waves results in brighter bands of light, whereas destructive interference results in darker bands. In terms of sound waves, constructive interference can make sound louder while destructive interference can cause dead spots where sound cannot be heard.

 

Interference is an important theoretical foundation in optics. Thinking of light as waves of radiation similar to ripples in water can be extremely useful. In addition, understanding this wave nature of light makes the concepts of reflection, refraction, dispersion and diffraction discussed in the following sections easier to understand.

Figure 2: Thomas Young's Double-Slit Experiment

Figure 3: Constructive and Destructive Interference

 

REFLECTION

Reflection is the change in direction of a wavefront when it hits an object and returns at an angle. The law of reflection states that the angle of incidence (angle at which light approaches the surface) is equal to the angle of reflection (angle at which light leaves the surface). Figure 4 illustrates reflection from a first surface mirror. Ideally, if the reflecting surface is smooth, all of the reflected rays will be parallel, defined as specular, or regular, reflection. If the surface is rough, the rays will not be parallel; this is referred to as diffuse, or irregular, reflection. Mirrors are known for their reflective qualities which are determined by the material used and the coating applied.

Figure 4: Reflection from a First Surface Mirror

 

REFRACTION

While reflection causes the angle of incidence to equal the angle of reflection, refraction occurs when the wavefront changes direction as it passes through a medium. The degree of refraction is dependent upon the wavelength of light and the index of refraction of the medium. Index of refraction (n) is the ratio of the speed of light in a vacuum (c) to the speed of light within a given medium (v). This can be mathematically expressed by Equation 1. Index of refraction is a means of quantifying the effect of light slowing down as it enters a high index medium from a low index medium (Figure 5).

 

Figure 5: Light Refraction from a Low Index to a High Index Medium

 

where n1 is the index of the incident medium, θ1 is the angle of the incident ray, n2 is the index of the refracted/reflected medium, and θ2 is the angle of the refracted/reflected ray.

 

If the angle of incidence is greater than a critical angle θc (when the angle of refraction = 90°), then light is reflected instead of refracted. This process is referred to as total internal reflection (TIR). Figure 6 illustrates TIR within a given medium.

 

Figure 6: Total Internal Reflection

 

TIR is mathematically expressed by Equation 3:

Total Internal Reflection is responsible for the sparkle one sees in diamonds. Due to their high index of refraction, diamonds exhibit a high degree of TIR which causes them to reflect light at a variety of angles, or sparkle. Another notable example of TIR is in fiber optics, where light entering one end of a glass or plastic fiber optic will undergo several reflections throughout the fiber's length until it exits the other end (Figure 7). Since TIR occurs for a critical angle, fiber optics have specific acceptance angles and minimum bend radii which dictate the largest angle at which light can enter and be reflected and the smallest radii the fibers can be bent to achieve TIR.

 

Figure 7: Total Internal Refraction in a Single Fiber Optic

 

DISPERSION

Dispersion is a measure of how much the index of refraction of a material changes with respect to wavelength. Dispersion also determines the separation of wavelengths known as chromatic aberration (Figure 8). A glass with high dispersion will separate light more than a glass with low dispersion. One way to quantify dispersion is to express it by Abbe number. Abbe number (vd) is a function of the refractive index of a material at the f (486.1nm), d (587.6nm), and c (656.3nm) wavelengths of light (Equation 4).

The chromatic aberration caused by dispersion is responsible for the familiar rainbow effect one sees in optical lenses, prisms, and similar optical components. Dispersion can be a highly desirable phenomenon, as in the case of an equilateral prism to split light into its components colors. However, in other applications, dispersion can be detrimental to a system's performance.

Figure 8: Dispersion through a Prism

 

DIFFRACTION

The interference patterns created by Thomas Young's double-slit experiment can also be characterized by the phenomenon known as diffraction. Diffraction usually occurs when waves pass through a narrow slit or around a sharp edge. In general, the greater the difference between the size of the wavelength of light and the width of the slit or object the wavelength encounters, the greater the diffraction. The best example of diffraction is demonstrated using diffraction gratings. A diffraction grating's closely spaced, parallel grooves cause incident monochromatic light to bend, or diffract. The degree of diffraction creates specific interference patterns. Figures 9 and 10 illustrate various patterns achieved with diffractive optics. Diffraction is the underlying theoretical foundation behind many applications using diffraction gratings, spectrometers, monochrometers, laser projection heads, and a host of other components.

 

Multi-Line Red Laser Diffraction Pattern

Dot Matrix Red Laser Diffraction Pattern

 

The basic theoretical foundations governing the electromagnetic spectrum, interference, reflection, refraction, dispersion, and diffraction are important stepping stones to more complex optical concepts. Light's wave properties explain a great deal of optics; understanding the fundamental concepts of optics can greatly increase one's understanding of the way light interacts with a variety of optical, imaging, and photonics components.

聯(lián)系我們

地址:江蘇省江陰市人民東路1091號(hào)1017室 傳真:0510-68836817 Email:sales@rympo.com
24小時(shí)在線客服,為您服務(wù)!

版權(quán)所有 © 2025 江陰韻翔光電技術(shù)有限公司 備案號(hào):蘇ICP備16003332號(hào)-1 技術(shù)支持:化工儀器網(wǎng) 管理登陸 GoogleSitemap

在線咨詢
QQ客服
QQ:17041053
電話咨詢
0510-68836815
關(guān)注微信
主站蜘蛛池模板: 亚洲欧美洲成人一区二区| 青青青国产在线观看手机免费| 久久精品国产精品青草| 特黄做受又粗又长又大又硬| 国产全是老熟女太爽了| 色猫咪av在线观看| 纯肉无遮挡无码日本动漫| 国产精品亚洲片在线| 免费的黄网站在线观看| 亚洲www啪成人一区二区麻豆| 午夜免费视频| 国产精品久人妻精品老妇| 18禁美女裸体无遮挡网站| 欧美熟妇的性裸交| 99久久婷婷国产一区二区| 亚洲卡一卡二新区| 欧美性大战xxxxx久久久√| 亚裔大战黑人老外av| 国产亚洲精品欧洲在线观看 | 国产成人精品亚洲日本在线| 永久黄网站色视频免费无下载| 亚洲日韩爆乳中文字幕欧美| 久久久e热视频| 亚洲精品www久久久久久 | 亚洲中亚洲字幕无线乱码| 色偷偷一区二区无码视频| 特黄做受又粗又长又大又硬| 国精产品999国精产品官网| 性色a∨人人爽网站| 在线视频免费观看爽爽爽| 欧美熟妇乱子伦xx视频| 国产女精品视频网站免费蜜芽| 人妻熟人中文字幕一区二区| 强开小婷嫩苞又嫩又紧视频| 国产亚洲精品线观看k频道| 久无码久无码av无码| 国产亚洲精品成人aa片新蒲金| 伊人久久大香线蕉午夜| 国产精品亚洲片在线观看不卡| 欧美成人aaa片一区国产精品| 2020久久国产综合精品swag|