Teacher Notes
|
||||||
---|---|---|---|---|---|---|
Energy in PhotonsDemonstration Kit![]() IntroductionStudents often confuse the concepts of intensity of light and energy of light. This demonstration provides a clear way to demonstrate that the intensity, or brightness, of light is NOT the same as the amount of energy a particular color of light possesses. Concepts
MaterialsEnergy in Photons Demonstrator Card—assembled and ready to use*
Light source—classroom lights work well *Materials included in kit Safety PrecautionsAlways follow standard laboratory safety rules when performing demonstrations. Procedure
Student Worksheet PDFTeacher Tips
Further Extensions
Correlation to Next Generation Science Standards (NGSS)†Science & Engineering PracticesAsking questions and defining problemsPlanning and carrying out investigations Engaging in argument from evidence Analyzing and interpreting data Using mathematics and computational thinking Obtaining, evaluation, and communicating information Disciplinary Core IdeasMS-PS4.A: Wave PropertiesMS-PS4.B: Electromagnetic Radiation HS-PS3.A: Definitions of Energy HS-PS4.A: Wave Properties HS-PS4.B: Electromagnetic Radiation Crosscutting ConceptsPatternsScale, proportion, and quantity Energy and matter Performance ExpectationsMS-PS4-1. Use mathematical representations to describe a simple model for waves that includes how the amplitude of a wave is related to the energy in a wave. Answers to Questions
DiscussionThe Electromagnetic Spectrum {12845_Discussion_Figure_2_Electromagnetic spectrum}
The visible portion of the electromagnetic spectrum is only a small part of the entire spectrum. It spans the wavelength region from about 400 to 700 nm. The human eye sees light of 400 nm as violet and 700 nm as red. Because wavelength is inversely proportional to energy according to the equation E = hc/λ, violet light is higher energy light than red light. The color of light seen with the human eye varies from red to violet (low to high energy) according to the familiar phrase ROY G BIV: red, orange, yellow, green, blue, indigo, violet. As the color of the light changes, so does the amount of energy it possesses. White light, like that from a fluorescent light, contains all of the colors in the visible spectrum. Intensity versus Energy of Light: The Photoelectric Effect Another characteristic of light, in addition to its energy, is its intensity. Intensity can be thought of as the brightness of the light. According to the theories of classical physics, energy is proportional to intensity, so that the more intense a light source, the more energy it gives off. Under this assumption, very bright (intense) yellow light should cause the phosphorescent strip in the Demonstrator Card to glow. However, this is not observed. Instead, the phosphorescent strip glows only when blue or violet light is shined on it. This phenomenon is analogous to the photoelectric effect, one of the classical paradoxes that led to the discovery of quantum mechanics. The photoelectric effect involves the ejection of electrons from a metal surface when light is shined on it; the energy of the electrons ejected depends upon the wavelength of the light, not the intensity. Einstein explained the photoelectric effect by suggesting that light consists of photons, each with energy E = hν. If a photon of light strikes a metal surface with more energy than the energy binding an electron to the surface, the photon will cause an electron to be ejected. The more intense a light source (greater number of photons), the greater the number of electrons ejected. If a photon striking the surface of a metal does not have more energy than the energy binding an electron to the surface, an electron cannot be ejected, no matter how many photons (with this amount of energy) strike the surface. The glowing of the phosphorescent strip in the Demonstrator Card is due to the emission of photons, analogous to the ejection of electrons from the surface of a metal. The phosphorescent material has a critical wavelength (or energy) of light. If a light source is shined on the phosphorescent strip and it contains photons whose energy is greater than the energy needed to cause the strip to glow, it will glow. If the intensity of this source is increased, the glowing of the strip will increase. If, however, a light source is shined on the phosphorescent strip that contains photons whose energy is less than the critical energy for the phosphorescent strip, no glowing will occur, no matter how bright the light source. Absorption and Transmission of Light Why do the filters appear violet, blue, green, yellow, orange and red? They are each composed of different molecules—molecules that absorb different wavelengths of light. For example, the red filter appears red to the human eye because it is transmitting red light. When white light is shined upon the red filter, the molecules in the filter absorb some of the wavelengths of the light and transmit others. All non-red wavelengths of light will be absorbed by the red filter to some extent, although green light will be absorbed the most. The green photons hit the filter and are absorbed by the molecules in the filter. They do not make it through the filter, and hence, a green color is not seen from this filter. In contrast, red photons are not absorbed by the molecules in the red filter, so they pass right through the filter, and a red color is observed. How is it known that the red filter absorbs the green wavelengths of light? Red and green are complementary colors—they are across from each other on the color wheel (see Figure 3). {12845_Discussion_Figure_3}
In general, colors opposite each other on the color wheel are complementary colors. For example, by looking at the wheel, the fact that violet and yellow are complementary colors can be seen. Therefore, in analogy to the red filter, it can be assumed that the violet filter absorbs yellow light and transmits violet light. The color wheel and the idea of complementary colors can be used as a first estimation of the wavelengths that are absorbed by a substance based on its color. The following table lists the wavelengths associated with each of the colors in the visible spectrum and their complements. The representative wavelength can be used as a benchmark for each color. For example, instead of referring to green as light in the wavelength range 500–600 nm, one could simply say that green light is 520 nm. {12845_Discussion_Table_1}
Transmission curves are available for each of the filters in the Demonstrator Card. These curves show which wavelengths of light are actually transmitted by each filter—the highest peak on each curve points to the wavelength that is transmitted the most (see Figure 4).
{12845_Discussion_Figure_4}
From these curves, the absorbed wavelengths of light can be inferred since absorbance is inversely proportional to transmittance according to the equation A = – log T. Compare the estimation of the absorbed wavelengths for each filter from above with the actual absorption as shown in these transmittance curves. It is evident that these filters are not “pure” filters—they do not transmit a single wavelength, or even a single color in most cases. But, they do filter enough of the other wavelengths so that only a single color appears to be shining through the filter. The cutoff wavelength for exciting the phosphorescent strip is about 480 nm. Photons with a higher wavelength (less energy) will not cause the strip to glow, while photons with lower wavelengths (more energy) will cause the phosphorescent glow. Looking at the table on page 4, 480 nm is right on the border between blue and green light. Therefore, blue or violet photons (which are not absorbed by the blue and violet filters, but are instead transmitted through these filters) will contain enough energy to excite the strip and cause it to glow. The green, yellow, orange, and red filters absorb the blue and violet photons instead of allowing them to be transmitted. Therefore, the light coming through these filters does not contain enough energy to excite the phosphorescent strip and, as a result, no glow is observed. Phosphorescence Luminescence is the emission of radiation (light) by a substance as a result of absorption of energy from photons, charged particles or chemical change. It is a general term that includes fluorescence, phosphorescence and chemiluminescence, to name just a few special types. Phosphorescence is different from the other types of luminescence in that light continues to be emitted even after the exciting source has been removed. This is sometimes referred to as the “afterglow.” In this demonstration, the exciting source is the classroom lights. The strip in the Demonstrator Card glows even after the lights have been turned off (removal of the exciting source), so it can be classified as a phosphorescent material. Why does a phosphorescent material continue to glow even after the exciting source has been removed? This can be explained by looking at an energy level diagram for the phosphorescent material. In both phosphorescence and fluorescence, a light source is shined on the material, and a photon is absorbed. The energy from the photon is transferred to an electron which makes a transition to an excited electronic state. From this excited electronic state, the electron naturally wants to relax back down to its ground state (see Figure 5). When the electron relaxes back down, it does not necessarily jump down to the ground state in a single step. The relaxation pathway varies, and is different depending on whether the material is fluorescing or phosphorescing. {12845_Discussion_Figure_5}
In fluorescence, the electron relaxes down to a lower energy state and emits a photon in the process. If this photon has a wavelength in the visible portion of the electromagnetic spectrum, we observe a colorful, glowing effect. This process is practically instantaneous so the fluorescence is observed as soon as the exciting source is present and disappears as soon as the exciting source is removed. An example of fluorescence is the way white shirts washed in Tide® glow under a black light. In phosphorescence, the excited electron first makes a slow transition to another excited state very close in energy to the initial excited state. From this second excited state, the electron then relaxes down to a state lower in energy, emitting a photon in the process. The characteristic afterglow of phosphorescence is due to the delayed emission that occurs because the transition between the first two excited states is slow. ReferencesThanks to Rhonda Reist of Olathe High School, Olathe, KS, for providing us with the idea for this“brilliant” demonstration. Recommended Products
|
||||||