/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 63 A rear view mirror of a vehicle ... [FREE SOLUTION] | 91Ó°ÊÓ

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A rear view mirror of a vehicle is cylindrical having radius of curvature \(5 \mathrm{~cm}\) and length of arc of curved surface is \(10 \mathrm{~cm}\). The field of view in radian, if it is assumed that the eye of the driver is at a large distance from the mirror, is: (a) \(0.5\) (b) 1 (c) 2 (d) 4

Short Answer

Expert verified
The field of view is 2 radians.

Step by step solution

01

Understand the Problem

We are given a cylindrical rear-view mirror with a radius of curvature of the curved surface of \(5\text{ cm}\) and an arc length of \(10\text{ cm}\). We need to find the field of view in radians, assuming the driver’s eye is at a large distance.
02

Identify the Formula

The field of view or the angle \( \theta \) in radians for a circular arc is given by the formula:\[ \theta = \frac{\text{Arc Length}}{\text{Radius of Curvature}} \] Here, the arc length is \(10\text{ cm}\) and the radius is \(5\text{ cm}\).
03

Substitute the Values

Plug the given values into the formula:\[ \theta = \frac{10}{5} \]
04

Calculate the Result

Perform the division to find \( \theta \):\[ \theta = 2 \]

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Key Concepts

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

Cylindrical Mirrors
Cylindrical mirrors are fascinating devices often used to expand the field of view in different applications, including vehicle rear-view mirrors. Unlike flat or spherical mirrors, cylindrical mirrors have a unique curved surface that focuses light differently. They can be visualized as a section of a cylinder. This specific shape allows images to be stretched across the surface, which gives users a wider view.
A cylindrical mirror, by definition, has one curved surface with a constant radius along its height. This design is beneficial in applications where space is limited, yet a wide field of vision is necessary. In vehicles, this kind of mirror helps drivers see more of the rear without needing a larger mirror. As important components of optical systems, they also play a role in laser scanning, where precise control over how light is spread and focused is needed.
In practical terms, the curvature helps project an image that covers a wide angle, making these mirrors highly effective for safety and practicality. By understanding how cylindrical mirrors work, we can appreciate their role in expanding our visual capabilities efficiently and compactly.
Field of View
The field of view (FOV) is an essential concept when discussing mirrors and optical devices. It's defined as the extent of the observable world that is seen at any given moment through an optical instrument. In other words, it's how much you can see, from one side to the other, looking through the device or reflection surface. The FOV can be expressed in degrees or radians, depending on the precision required.
When it comes to cylindrical mirrors, the field of view is crucial because it tells us how much area one can visually cover using the mirror. For a driver using a rear-view mirror, a larger field of view means they can see more of the road behind them, which translates to better safety and maneuverability.
In the problem given, the field of view is calculated in radians. This unit of measurement is particularly useful, as it is directly related to the geometry of the circle. Understanding the field of view helps in assessing how effective a particular mirror design will be in practical scenarios, such as preventing blind spots in cars.
Radial Measurement Formula
The radial measurement formula comes into play when calculating the field of view for mirrors and similar optical devices. This mathematical relationship is quite simple yet highly effective for determining the angle of view.
The formula for understanding this concept is:
  • \[ \theta = \frac{\text{Arc Length}}{\text{Radius of Curvature}} \]
This equation is derived from the basic principles of circular geometry. It allows us to determine how much of the circle we can "see" based on the arc length and the radius of curvature. The arc length is essentially the segment of the circle's circumference that the mirror takes up, while the radius of curvature is the mirror's radius.
The formula can predict how much area can be seen or covered by the mirror just by using two straightforward measurements. By substituting the known values, like in the problem with a 10 cm arc length and a 5 cm radius, the field of view is easily calculated. This makes it a powerful tool for quick calculations in various fields such as optical engineering, automotive design, and even robotics.

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Most popular questions from this chapter

Infront of a vertical wall, a plane mirror of square shape is mounted parallel to the wall at some distance from it. On the wall, a point light source is fixed and light from it gets reflected from the mirror and forms a path on the wall. If the mirror is moved parallel to itself towards the wall, then (i) centre of the patch may remain stationary (ii) the patch may remain square in shape (iii) area of patch decreases Choose correct statement: (a) (i) and (ii) are correct (b) (i) and (iii) are correct (c) (ii) and (iii) are correct (d) none of the above

A point object \(P\) is placed at centre of curvature of a concave mirror of focal length \(25 \mathrm{~cm}\). The mirror is cut into two halves and shifted symmetrically \(1 \mathrm{~cm}\) apart in perpendicular to the optical axis. The distance between images formed by both parts is: (a) \(2 \mathrm{~cm}\) (b) \(1 \mathrm{~cm}\) (c) \(3 \mathrm{~cm}\) (d) \(4 \mathrm{~cm}\)

A narrow beam of light after reflection by a plane mirror falls on a scale \(100 \mathrm{~cm}\) from the mirror. When the mirror is rotated a little the spot moves through \(2 \mathrm{~cm}\), the angle, through which the mirror is rotated is : (a) \(0.02 \mathrm{rad}\) (b) \(0.01 \mathrm{rad}\) (c) \(200 \mathrm{rad}\) (d) \(\frac{0.01}{180} \pi \mathrm{rad}\)

Images in spherical mirrors suffer from several defects. Some of which is/are: (a) diffraction effect (b) the magnification varies with the distance of the object from mirror (c) a point source will not produce a point image (d) all of the above

A car is moving towards a plane mirror at a speed of \(30 \mathrm{~m} / \mathrm{s}\). Then the relative speed of its image with respect to the car will be : (a) \(30 \mathrm{~m} / \mathrm{s}\) (b) \(60 \mathrm{~m} / \mathrm{s}\) (c) \(15 \mathrm{~m} / \mathrm{s}\) (d) \(45 \mathrm{~m} / \mathrm{s}\)

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