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An object is 10.0 mm from the objective of a certain compound microscope. The lenses are 300 mm apart, and the intermediate image is 50.0 mm from the eyepiece. What overall magnification is produced by the instrument?

Short Answer

Expert verified

The overall magnification of the instrument is -125.

Step by step solution

01

Step 1: The given data

  1. The focal length of the eyepiece,fev=50mm.fev=50mm
  2. The object's distance from the microscope,p=10mm.
  3. The separation between the lens system,fob+s+fev=300mm.
02

Determining the concept of overall magnification

The ratio of the height of the image to the height of the object is given as the lateral magnification of the lens or the mirror. Now, the magnification of the mirror or the lens can also be given as the negative value of the ratio of the image distance to the object distance from the mirror. In a compound microscope, the total magnification is the product of the objective and ocular lenses.

Formula:

The mirror equation,

1f=1i+1p (i)

Where f = focal length, p = object distance from the mirror, i = image distance.

The overall magnification of a compound microscope,

mθ=-sfob25cmfey (ii)

Where s is the tube length of the microscope, fob is the focal length of the objective, and fey is the focal length of the eyepiece.

03

 Determining the overall magnification of the instrument.

Calculate the intermediate image distance as,

i=fob+s+fey-fey

By substituting the given value, the value of the image distance can be given as follows:

role="math" localid="1663026969553" 1fob=110+1250fob=250×10250+10=25026=9.6153cm≈9.62mm

Now, the tube length of the compound microscope can be given as follows:

s=fob+s+fev-fob-fev=300-9.62-50=240mm

Now, the overall magnification of the compound microscope can be given using the above data in equation (ii) as follows:

M=-2409.62×25×1050=-2409.62×5=-124.74≈-125

Therefore, the overall magnification of the instrument is -125.

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Most popular questions from this chapter

Two thin lenses of focal lengths f1andf2 are in contact and share the same central axis. Show that, in image formation, they are equivalent to a single thin lens for which the focal length is f=f1f2(f1+f2).

(a) Show that if the object O in Fig. 34-19c is moved from focal point F1toward the observer’s eye, the image moves in from infinity and the angle (and thus the angular magnification mu) increases. (b) If you continue this process, where is the image when mu has its maximum usable value? (You can then still increase, but the image will no longer be clear.) (c) Show that the maximum usable value of ismθ=1+25cmf.(d) Show that in this situation the angular magnification is equal to the lateral magnification.

32 through 38 37, 38 33, 35 Spherical refracting surfaces. An object Ostands on the central axis of a spherical refracting surface. For this situation, each problem in Table 34-5 refers to the index of refraction n1where the object is located, (a) the index of refraction n2on the other side of the refracting surface, (b) the object distance p, (c) the radius of curvature rof the surface, and (d) the image distance i. (All distances are in centimeters.) Fill in the missing information, including whether the image is (e) real (R)or virtual (V)and (f) on the same side of the surface as the objector on the opposite side.

The equation 1p+1i=2rfor spherical mirrors is an approximation that is valid if the image is formed by rays that make only small angles with the central axis. In reality, many of the angles are large, which smears the image a little. You can determine how much. Refer to Fig. 34-22 and consider a ray that leaves a point source (the object) on the central axis and that makes an angle a with that axis. First, find the point of intersection of the ray with the mirror. If the coordinates of this intersection point are x and y and the origin is placed at the center of curvature, then y=(x+p-r)tan a and x2+ y2= r2where pis the object distance and r is the mirror’s radius of curvature. Next, use tanβ=yxto find the angle b at the point of intersection, and then useα+y=2βtofind the value of g. Finally, use the relationtany=y(x+i-r)to find the distance iof the image. (a) Suppose r=12cmand r=12cm. For each of the following values of a, find the position of the image — that is, the position of the point where the reflected ray crosses the central axis:(0.500,0.100,0.0100rad). Compare the results with those obtained with theequation1p+1i=2r.(b) Repeat the calculations for p=4.00cm.

You look down at a coin that lies at the bottom of a pool of liquid of depthand index of refraction(Fig. 34-57). Because you view with two eyes, which intercept different rays of light from the coin, you perceive the coin to bewhere extensions of the intercepted rays cross, at depthdainstead of d. Assuming that the intercepted rays in Fig. 34-57 are close to a vertical axis through the coin, show that da=dn.


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