Red light of wavelength 650 nm strikes the side of the-prism (nred = 1.613) șhown in Fig. 19.17 at an incident angle of 53.8°. (a) Calculate the refracted angle relațive to a line perpendicular to the first air-glass interface. (b) If the prism has three 60° angles, calculate the incident angle at the second glass-air interface. (c) Calculate the refracted anglé relative to a line perpendic-lar to this surface. (d) Calculate the net angular change in direction of the light.
Red light of wavelength 650 nm strikes the side of the-prism (nred = 1.613) șhown in Fig. 19.17 at an incident angle of 53.8°. (a) Calculate the refracted angle relațive to a line perpendicular to the first air-glass interface. (b) If the prism has three 60° angles, calculate the incident angle at the second glass-air interface. (c) Calculate the refracted anglé relative to a line perpendic-lar to this surface. (d) Calculate the net angular change in direction of the light.
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Red light of wavelength 650 nm strikes the side of the-prism (nred = 1.613) șhown in Fig. 19.17 at an incident angle of 53.8°. (a) Calculate the refracted angle relațive to a line perpendicular to the first air-glass interface. (b) If the prism has three 60° angles, calculate the incident angle at the second glass-air interface. (c) Calculate the refracted anglé relative to a line perpendic-lar to this surface. (d) Calculate the net angular change in direction of the light.
![ses it to
ace (Fig. 19.18e), the
ds forward while the right edge
speed. As the wavefront emerges fr
her downward.
All colors of light undergo a similar change in direction, but the change is
test for those wavelengths (colors) that are slowed most in the glass. Hence,
et is deflected farthest downward and red the least (see Fig. 19.17).
This nonuniform deflection of light composed of many wavelengths is use
or analyzing the wavelengths of light coming from a source. Light from the
for example, is made of all different wavelengths. Thus, deflection of sun-
through a prism produces a rainbow of all the different colors (Fig. 19.17)
he other hand, a hot gas of hydrogen atoms emits light at only certain
te wavelengths: red light at about 656 nm and blue light at 486 nm,
m, and 410 nm. If the light given off by hydrogen atoms is passed through
ism and then projected on a screen, separate lines for each discrete wave-
are seen. The 410-nm blue light is deflected most; the red light is de-
White light
Screen
Red (650 nm)
Orange
Yellow
Green (500 nm)
Blue
Violet (400 nm)](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F2408ff62-3d68-40ee-b0f1-62bac3d6a305%2F138ad184-5136-4995-8002-27fe2da5ee98%2Fmdgycfd_processed.jpeg&w=3840&q=75)
Transcribed Image Text:ses it to
ace (Fig. 19.18e), the
ds forward while the right edge
speed. As the wavefront emerges fr
her downward.
All colors of light undergo a similar change in direction, but the change is
test for those wavelengths (colors) that are slowed most in the glass. Hence,
et is deflected farthest downward and red the least (see Fig. 19.17).
This nonuniform deflection of light composed of many wavelengths is use
or analyzing the wavelengths of light coming from a source. Light from the
for example, is made of all different wavelengths. Thus, deflection of sun-
through a prism produces a rainbow of all the different colors (Fig. 19.17)
he other hand, a hot gas of hydrogen atoms emits light at only certain
te wavelengths: red light at about 656 nm and blue light at 486 nm,
m, and 410 nm. If the light given off by hydrogen atoms is passed through
ism and then projected on a screen, separate lines for each discrete wave-
are seen. The 410-nm blue light is deflected most; the red light is de-
White light
Screen
Red (650 nm)
Orange
Yellow
Green (500 nm)
Blue
Violet (400 nm)
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