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 ๐ in nanometers of the light as measured in air. Where ๐ 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 35-45 n 1 n 2 n 3 Type L ๐ 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 Table 35-3: Transmission Through Thin Layers.
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 ๐ in nanometers of the light as measured in air. Where ๐ 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 35-45 n 1 n 2 n 3 Type L ๐ 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 Table 35-3: Transmission Through Thin Layers.
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 ๐ in nanometers of the light as measured in air. Where ๐ 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.
Consider the situation in the figure below; a neutral conducting ball hangs from the ceiling by an insulating string, and a charged insulating rod is going to be placed nearby.
A. First, if the rod was not there, what statement best describes the charge distribution of the ball?
1) โSince it is a conductor, all the charges are on the outside of the ball.โ2) โThe ball is neutral, so it has no positive or negative charges anywhere.โ3) โThe positive and negative charges are separated from each other, but we don't know what direction the ball is polarized.โ4) โThe positive and negative charges are evenly distributed everywhere in the ball.โ
B.ย Now, when the rod is moved close to the ball, what happens to the charges on the ball?
1) โThere is a separation of charges in the ball; the side closer to the rod becomes positively charged, and the opposite side becomes negatively charged.โ2) โNegative charge is drawn from the ground (via the string), so the ball acquires a net negative charge.โ3)โฆ
answer question ย 5-9
AMPS
VOLTS
OHMS
5) 50 A
110 V
6) .08 A
39 V
7) 0.5 A
60
8) 2.5 A
110 V
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