57 through 68 GO 64, 65 SSM 59 Transmission through thin layers In Fig. 35-43, light is incident perpendicularly on a thin layer of material 2 that lies between (thicker) materials 1 and 3. (The rays are tilted only for clarity.) Part of the light ends up in material 3 as ray r 3 (the light does not reflect inside material 2) and r 4 (the light reflects twice inside material 2). The waves of r 3 and r 4 interfere, and here we consider the type of interference to be either maximum (max) or minimum (min). For this situation, each problem in Table 35-3 refers to the indexes of refraction, n 1, n 2, and n 3, the type of interference, the thin-layer thickness L in nanometers, and the wavelength λ in nanometers of the light as measured in air. Where λ is missing, give the wavelength that is in the visible range. Where L is missing, give the second least thickness or the third least thickness as indicated. Figure 35-43 Problem 57 through 68. Table 35-3 Problems 57 through 68: Transmission Through Thin Layers. See the setup for these problems. n 1 n 2 n 3 Type L λ 57 1.55 1.60 1.33 min 285 58 1.32 1.75 1.39 min 3rd 382 59 1.68 1.59 1.50 max 415 60 1.50 1.34 1.42 max 380 61 1.32 1.75 1.39 min 325 62 1.68 1.59 1.50 max 2nd 342 63 1.40 1.46 1.75 max 2nd 482 64 1.40 1.46 1.75 max 210 65 1.60 1.40 1.80 min 2nd 632 66 1.60 1.40 1.80 max 200 67 1.50 1.34 1.42 min 2nd 587 68 1.55 1.60 1.33 min 3rd 612
57 through 68 GO 64, 65 SSM 59 Transmission through thin layers In Fig. 35-43, light is incident perpendicularly on a thin layer of material 2 that lies between (thicker) materials 1 and 3. (The rays are tilted only for clarity.) Part of the light ends up in material 3 as ray r 3 (the light does not reflect inside material 2) and r 4 (the light reflects twice inside material 2). The waves of r 3 and r 4 interfere, and here we consider the type of interference to be either maximum (max) or minimum (min). For this situation, each problem in Table 35-3 refers to the indexes of refraction, n 1, n 2, and n 3, the type of interference, the thin-layer thickness L in nanometers, and the wavelength λ in nanometers of the light as measured in air. Where λ is missing, give the wavelength that is in the visible range. Where L is missing, give the second least thickness or the third least thickness as indicated. Figure 35-43 Problem 57 through 68. Table 35-3 Problems 57 through 68: Transmission Through Thin Layers. See the setup for these problems. n 1 n 2 n 3 Type L λ 57 1.55 1.60 1.33 min 285 58 1.32 1.75 1.39 min 3rd 382 59 1.68 1.59 1.50 max 415 60 1.50 1.34 1.42 max 380 61 1.32 1.75 1.39 min 325 62 1.68 1.59 1.50 max 2nd 342 63 1.40 1.46 1.75 max 2nd 482 64 1.40 1.46 1.75 max 210 65 1.60 1.40 1.80 min 2nd 632 66 1.60 1.40 1.80 max 200 67 1.50 1.34 1.42 min 2nd 587 68 1.55 1.60 1.33 min 3rd 612
57 through 68 GO 64, 65 SSM 59 Transmission through thin layers In Fig. 35-43, light is incident perpendicularly on a thin layer of material 2 that lies between (thicker) materials 1 and 3. (The rays are tilted only for clarity.) Part of the light ends up in material 3 as ray r3 (the light does not reflect inside material 2) and r4 (the light reflects twice inside material 2). The waves of r3 and r4 interfere, and here we consider the type of interference to be either maximum (max) or minimum (min). For this situation, each problem in Table 35-3 refers to the indexes of refraction, n1,n2, and n3, the type of interference, the thin-layer thickness L in nanometers, and the wavelength λ in nanometers of the light as measured in air. Where λ is missing, give the wavelength that is in the visible range. Where L is missing, give the second least thickness or the third least thickness as indicated.
Figure 35-43 Problem 57 through 68.
Table 35-3 Problems 57 through 68: Transmission Through Thin Layers. See the setup for these problems.
air is pushed steadily though a forced air pipe at a steady speed of 4.0 m/s. the pipe measures 56 cm by 22 cm. how fast will air move though a narrower portion of the pipe that is also rectangular and measures 32 cm by 22 cm
No chatgpt pls will upvote
13.87 ... Interplanetary Navigation. The most efficient way
to send a spacecraft from the earth to another planet is by using a
Hohmann transfer orbit (Fig. P13.87). If the orbits of the departure
and destination planets are circular, the Hohmann transfer orbit is an
elliptical orbit whose perihelion and aphelion are tangent to the
orbits of the two planets. The rockets are fired briefly at the depar-
ture planet to put the spacecraft into the transfer orbit; the spacecraft
then coasts until it reaches the destination planet. The rockets are
then fired again to put the spacecraft into the same orbit about the
sun as the destination planet. (a) For a flight from earth to Mars, in
what direction must the rockets be fired at the earth and at Mars: in
the direction of motion, or opposite the direction of motion? What
about for a flight from Mars to the earth? (b) How long does a one-
way trip from the the earth to Mars take, between the firings of the
rockets? (c) To reach Mars from the…
Microbiology with Diseases by Body System (5th Edition)
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