Focal Length of a Zoom Lens. Figure P34.101 shows a simple version of a zoom lens. The converging lens has focal length f 1 and the diverging lens has focal length f 2 = −| f 2 |. The two lenses are separated by a variable distance d that is always less than f 1 Also, the magnitude of the focal length of the diverging parallel rays of radius r 0 entering the converging lens, (a) Show that the radius of the ray bundle decreases to r ′ 0 = r 0 ( f 1 − d ) / f 1 at the point that it enters the diverging lens. (b) Show that the final image I′ is formed a distance s ′ 2 = | f 2 | ( f 1 − d ) / ( | f 2 | − f 1 + d ) to the right of the diverging lens. (c) If the rays that emerge from the diverging lens and reach the final image point are extended backward to the left of the diverging lens, they will eventually expand to the original radius r 0 at some point Q . The distance from the final image I ′ to the point Q is the effective focal length f of the lens combination; if the combination were replaced by a single lens of focal length f placed at Q , parallel rays would still be brought to a focus at I ′. Show that the effective focal length is given by f = f 1 | f 2 |/(| f 2 | − f 1 + d ). (d) If f 1 = 12.0cm, f 2 = − 18.0 cm, and the separation d is adjustable between 0 and 4.0 cm, find the maximum and minimum focal lengths of the combination. What value of d gives f = 30.0 cm? Figure P34.101
Focal Length of a Zoom Lens. Figure P34.101 shows a simple version of a zoom lens. The converging lens has focal length f 1 and the diverging lens has focal length f 2 = −| f 2 |. The two lenses are separated by a variable distance d that is always less than f 1 Also, the magnitude of the focal length of the diverging parallel rays of radius r 0 entering the converging lens, (a) Show that the radius of the ray bundle decreases to r ′ 0 = r 0 ( f 1 − d ) / f 1 at the point that it enters the diverging lens. (b) Show that the final image I′ is formed a distance s ′ 2 = | f 2 | ( f 1 − d ) / ( | f 2 | − f 1 + d ) to the right of the diverging lens. (c) If the rays that emerge from the diverging lens and reach the final image point are extended backward to the left of the diverging lens, they will eventually expand to the original radius r 0 at some point Q . The distance from the final image I ′ to the point Q is the effective focal length f of the lens combination; if the combination were replaced by a single lens of focal length f placed at Q , parallel rays would still be brought to a focus at I ′. Show that the effective focal length is given by f = f 1 | f 2 |/(| f 2 | − f 1 + d ). (d) If f 1 = 12.0cm, f 2 = − 18.0 cm, and the separation d is adjustable between 0 and 4.0 cm, find the maximum and minimum focal lengths of the combination. What value of d gives f = 30.0 cm? Figure P34.101
Focal Length of a Zoom Lens. Figure P34.101 shows a simple version of a zoom lens. The converging lens has focal length f1 and the diverging lens has focal length f2 = −|f2|. The two lenses are separated by a variable distance d that is always less than f1 Also, the magnitude of the focal length of the diverging parallel rays of radius r0 entering the converging lens, (a) Show that the radius of the ray bundle decreases to
r
′
0
=
r
0
(
f
1
−
d
)
/
f
1
at the point that it enters the diverging lens. (b) Show that the final image I′ is formed a distance
s
′
2
=
|
f
2
|
(
f
1
−
d
)
/
(
|
f
2
|
−
f
1
+
d
)
to the right of the diverging lens. (c) If the rays that emerge from the diverging lens and reach the final image point are extended backward to the left of the diverging lens, they will eventually expand to the original radius r0 at some point Q. The distance from the final image I′ to the point Q is the effective focal length f of the lens combination; if the combination were replaced by a single lens of focal length f placed at Q, parallel rays would still be brought to a focus at I′. Show that the effective focal length is given by f = f1|f2|/(|f2| − f1 + d). (d) If f1 = 12.0cm, f2 = − 18.0 cm, and the separation d is adjustable between 0 and 4.0 cm, find the maximum and minimum focal lengths of the combination. What value of d gives f = 30.0 cm?
The magnitude of the net force exerted in the x direction on a 3.00-kg particle varies in time as shown in the figure below.
F(N)
4
3
A
2
t(s)
1
2 3
45
(a) Find the impulse of the force over the 5.00-s time interval.
==
N⚫s
(b) Find the final velocity the particle attains if it is originally at rest.
m/s
(c) Find its final velocity if its original velocity is -3.50 î m/s.
V₁
m/s
(d) Find the average force exerted on the particle for the time interval between 0 and 5.00 s.
=
avg
N
••63 SSM www In the circuit of
Fig. 27-65, 8 = 1.2 kV, C = 6.5 µF,
R₁
S
R₂
R3
800
C
H
R₁ = R₂ = R3 = 0.73 MQ. With C
completely uncharged, switch S is
suddenly closed (at t = 0). At t = 0,
what are (a) current i̟ in resistor 1,
(b) current 2 in resistor 2, and
(c) current i3 in resistor 3? At t = ∞o
(that is, after many time constants), what are (d) i₁, (e) i₂, and (f) iz?
What is the potential difference V2 across resistor 2 at (g) t = 0 and
(h) t = ∞o? (i) Sketch V2 versus t between these two extreme times.
Figure 27-65 Problem 63.
Thor flies by spinning his hammer really fast from a leather strap at the end of the handle, letting go, then grabbing it and having it pull him. If Thor wants to reach escape velocity (velocity needed to leave Earth’s atmosphere), he will need the linear velocity of the center of mass of the hammer to be 11,200 m/s. Thor's escape velocity is 33532.9 rad/s, the angular velocity is 8055.5 rad/s^2. While the hammer is spinning at its maximum speed what impossibly large tension does the leather strap, which the hammer is spinning by, exert when the hammer is at its lowest point? the hammer has a total mass of 20.0kg.
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