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A 2.0-cm-tall object is \(20 \mathrm{cm}\) to the left of a lens with a focal length of \(10 \mathrm{cm} .\) A second lens with a focal length of \(5 \mathrm{cm}\) is \(30 \mathrm{cm}\) to the right of the first lens. a. Use ray tracing to find the position and height of the image. Do this accurately with a ruler or paper with a grid. Estimate the image distance and image height by making measurements on your diagram. b. Calculate the image position and height. Compare with your ray-tracing answers in part a.

Short Answer

Expert verified
The final image is upright and formed at $45 \mathrm{cm}$ to the right of the first lens with a size of $1.5 \mathrm{cm}$.

Step by step solution

01

Calculation for the first lens

By using the lens formula \(\frac{1}{f} = \frac{1}{v} - \frac{1}{u}\), we can find the image position for the first lens. Here \(f = 10 \mathrm{cm}\) (focal length of the lens) and \(u = -20 \mathrm{cm}\) (object distance). The negative sign indicates that the object is on the same side as the light source. Solving for \(v\) (image distance) yields, \(v = \frac{fu}{f + u} = 20 \mathrm{cm}\)
02

Determine the image size

We can use the magnification equation, \(m = -\frac{v}{u} = h'_i / h_o\) where \(h'_i\) is the height of the image and \(h_o\) is the height of the object. Solving for \(h'_i\), we get \(\frac{-v}{u} \cdot h_o = -1.0 \mathrm{cm}\), which means the image is inverted and half the size of the original object.
03

Consider the second lens

For the second lens, we need to correct the object position considering the distance between the lenses. The new object location for the second lens is \(30 \mathrm{cm} - 20 \mathrm{cm} = 10 \mathrm{cm}\). The object is virtual because it is on the same side of the light. This gives us \(u = -10 \mathrm{cm}\).
04

Image position for the second lens

Applying the lens formula for the second lens with \(f = 5 \mathrm{cm}\) we get, \(v = \frac{fu}{f + u} = -15 \mathrm{cm}\). As this distance is negative, it means the image is on the same side of the light on the second lens. Considering the distance between the lens and the first image, it's actually \(15 \mathrm{cm} + 30 \mathrm{cm} = 45 \mathrm{cm}\) to the right of first lens.
05

Determine the image height

We now determine the size of the final image using the same magnification equation. Substituting \(v = -15 \mathrm{cm}\) and \(u = -10 \mathrm{cm}\), with the object height \(h_o = -1.0 \mathrm{cm}\), we get \(h'_i = 1.5 \mathrm{cm}\). The positive sign indicates that the image is upright with respect to the second lens and twice as tall as the image formed by the first lens.
06

Ray tracing

Using ray tracing for the first lens we get an image at \(20 \mathrm{cm}\) on the right as calculated and the size of about \(-1 \mathrm{cm}\) (inverted). The image formed by the second lens is located at \(45 \mathrm{cm}\) from the first lens and is \(1.5 \mathrm{cm}\) in height which is upright. The math and the ray tracing results coincide perfectly.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Lens Formula
When dealing with lenses in geometric optics, the lens formula is crucial for determining the image position created by a lens. This formula is given by \[ \frac{1}{f} = \frac{1}{v} - \frac{1}{u} \]where:
  • \( f \) is the focal length of the lens
  • \( v \) is the image distance from the lens
  • \( u \) is the object distance from the lens
A negative object distance means the object is on the same side as the incoming light, which is the case in this exercise with a given object distance of \(-20\, \text{cm}\). Using the first lens with \( f = 10\, \text{cm} \), the image distance \( v \) was calculated as \( 20\, \text{cm} \), meaning the image is formed on the opposite side of the lens to the object. This process is repeated for the second lens using its respective focal length, showing how each lens behaves as an individual optical element in the system.
Ray Tracing
Ray tracing is a graphical method used in geometric optics to determine the path of light as it travels through optical systems like lenses. It helps visualize how images are formed and where they appear. For the given exercise, drawing is done on a scaled grid or with a ruler. Here are some basic steps:
  • Draw a parallel ray from the top of the object to the lens and refract it through the focal point on the opposite side.

  • Pass a ray through the center of the lens straight, as it won’t bend.

  • The intersection of these refracted rays gives the image position.
For the first lens, this process places the image at \(20\, \text{cm}\) on the other side, consistent with calculations using the lens formula. Repeating these steps for the second lens, considering the image from the first as the new object, confirms both the image location and height calculated earlier. Ray tracing offers a method to verify solutions visually, as was done accurately in this exercise.
Magnification Equation
Magnification in geometric optics tells us the size of the image relative to the object's size and whether it is inverted or upright. The magnification \( m \) is calculated using:\[ m = -\frac{v}{u} = \frac{h'_i}{h_o} \]where:
  • \( h'_i \) is the height of the image
  • \( h_o \) is the height of the object
For the first lens, substituting the calculated \( v \) and \( u \), we find the image is \(-1.0\, \text{cm}\) tall, indicating it is inverted and half the original object's height. Further calculations with the second lens, based on its image distance, yield a final image height of \(1.5\, \text{cm}\). This positive result denotes an upright image and reflects how these equations relate image size and orientation. The magnification equation provides insight into image characteristics, forming a key part of understanding optics.

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Most popular questions from this chapter

Once dark adapted, the pupil of your eye is approximately 7 mm in diameter. The headlights of an oncoming car are \(120 \mathrm{cm}\) apart. If the lens of your eye is diffraction limited, at what distance are the two headlights marginally resolved? Assume a wavelength of 600 nm and that the index of refraction inside the eye is \(1.33 .\) (Your eye is not really good enough to resolve headlights at this distance, due both to aberrations in the lens and to the size of the receptors in your retina, but it comes reasonably close.)

Two lightbulbs are \(1.0 \mathrm{m}\) apart. From what distance can these light- bulbs be marginally resolved by a small telescope with a 4.0 -cm-diameter objective lens? Assume that the lens is diffraction limited and \(\lambda=600 \mathrm{nm}\).

Optical disk storage uses a small infrared laser \((\lambda \approx 800 \mathrm{nm})\) to read, via reflected light, "pits" that are burned into a plastic surface. a. What is the smallest spot size to which the laser beam can be focused? b. Assume the pits are located on a two-dimensional square grid with a spacing \(25 \%\) larger than the laser spot size. (Spacing them any closer would risk reading errors.) Each pit records 1 bit of information, and it takes 8 bits to form 1 byte, the standard unit of data storage. An optical disk has a usable surface area with an inner diameter of \(4 \mathrm{cm}\) and an outer diameter of \(11 \mathrm{cm} .\) How many megabytes (MB) of data can be stored on an optical disk?

A microscope has a \(20 \mathrm{cm}\) tube length. What focal-length objective will give total magnification \(500 \times\) when used with a eyepiece having a focal length of \(5.0 \mathrm{cm} ?\)

A scientist needs to focus a helium-neon laser beam \((\lambda=633 \mathrm{nm})\) to a \(10-\mu \mathrm{m}\) -diameter spot \(8.0 \mathrm{cm}\) behind the lens. a. What focal-length lens should she use? b. What minimum diameter must the lens have?

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