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Galileo devised a simple terrestrial telescope that produces an upright image. It consists of a converging objective lens and a diverging eyepiece at opposite ends of the telescope tube. For distant objects, the tube length is the objective focal length less the absolute value of the eyepiece focal length. (a) Does the user of the telescope see a real or virtual image? (b) Where is the final image? (c) If a telescope is to be constructed with a tube of length \(10.0 \mathrm{~cm}\) and a magnification of \(3.00\), what are the focal lengths of the objective and eyepiece?

Short Answer

Expert verified
The user of the telescope sees a virtual image. The final image is at the usual reading distance from the eye or at infinite distance for normal vision. The focal lengths of the objective lens and eyepiece are 7.5 cm and -2.5 cm respectively.

Step by step solution

01

Determining the Nature of the Image

For a simple telescope, an upright (erect) image that can be seen by the user is formed, and such images are considered virtual. Thus, the user of the telescope sees a virtual image.
02

Location of the Final Image

The final image is formed at the focal point of the eyepiece. And since the users of the telescope can observe it with the eye, the image must be located at the near point. This is at the usual reading distance or at infinite distance for normal vision.
03

Calculation of the Focal Lengths

We have the relation that the tube length is equal to the focal length of the objective lens less the absolute value of the eyepiece focal length (|fE|). Let’s denote the focal length of the objective lens as fO. So, we have fO - |fE| = 10 cm. We also know that the magnification (m) of a telescope is given by the negative ratio of the focal length of the objective lens to that of eyepiece, or m = -fO / fE. Plugging in the given magnification of 3, we get -fO / fE = -3, or fO = 3fE. Solving these two equations simultaneously, we find fO = 7.5 cm and fE = -2.5 cm. The negative sign indicates that the eyepiece is a diverging lens.

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Key Concepts

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

Virtual Image
In the context of Galileo's terrestrial telescope, when we speak of a virtual image, we're talking about an image that appears to be in a location where light doesn't actually converge. A virtual image isn't visible on a screen, unlike a real image which is formed when light rays converge to a point. Instead, it can only be seen by looking through the optical device that creates it—in this case, the telescope.

For instance, when you gaze through a telescope, the virtual image is what you 'see' as the outcome of the light being bent by the lenses. This image appears upright in Galileo's telescope design, and your eyes interpret it as though it's coming from a different direction than it truly is. This ability to produce a virtual image allows astronomers and hobbyists alike to observe distant objects in the sky or on the terrestrial plane with greater clarity.
Magnification
Magnification is a measure of how much larger or closer an object appears when viewed through a lens or telescope. In our textbook exercise, the magnification achieved by Galileo's telescope is specified as 3.00. This means the telescope makes things appear three times larger than they do with the naked eye.

The magnification is mathematically defined as the ratio of the size of the image to the size of the object, but for telescopes, it can also be expressed as the ratio of the focal lengths of the objective lens to the eyepiece. Since magnification can significantly impact the usability and effectiveness of a telescope, it is crucial for anyone looking to gaze at the stars or distant landscapes to understand how magnification plays a role in their observations.
Lens Focal Length
Focal length is a critical concept in the study of telescope optics. It is defined as the distance from the lens (or mirror in some telescopes) to the point where it converges a beam of light to a focus. The objective lens's focal length determines the telescope's ability to gather light and resolve finer details of distant objects.

Galileo's telescope, for example, uses a converging objective lens with a longer focal length to collect light from distant objects, and a diverging eyepiece with a shorter absolute focal length to produce an upright image. The relationship between the focal lengths of these two lenses governs how the telescope functions. When constructing a telescope, as in the exercise, one must decide on the focal lengths of both the objective and the eyepiece to achieve the desired magnification and tube length—key parameters for anyone engaged in the intricate task of telescope design or selection.

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Most popular questions from this chapter

The Michelson interferometer can be used to measure the index of refraction of a gas by placing an evacuated transparent tube in the light path along one arm of the device. Fringe shifts occur as the gas is slowly added to the tube. Assume \(600-\mathrm{nm}\) light is used, the tube is \(5.00 \mathrm{~cm}\) long, and 160 fringe shifts occur as the pressure of the gas in the tube increases to atmospheric pressure. What is the index of refraction of the gas? Hint: The fringe shifts occur because the wavelength of the light changes inside the gas-filled tube.

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