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Ray Optics Fundamentals

Convex Mirror Image Formation

Explore how convex mirrors diverge light rays to expand the field of view. Toggle between a car side-view mirror showing cars behind, a dome security mirror revealing aisle corners, and a ray laboratory tracking virtual image construction behind the glass.

Convex Mirror Interactive Demo

Interact with driver-side mirrors, overhead dome mirrors, and ray benches to see virtual, upright, diminished images.

Simulating...

Live Telemetry

Formulas: 1/f = 1/u + 1/v & m = -v/u
Object Distance (u)
-100.0 cm
Image Distance (v)
+33.3 cm
Focal Length (f)
+50.0 cm
Radius (R)
+100.0 cm
Magnification (m)
+0.33
Field of View
110°

Physics of Convex Mirrors

A convex mirror, also known as a diverging mirror, is a curved mirror in which the reflective surface bulges outward toward the light source. Because of this shape, when parallel rays of light strike a convex mirror, they reflect outward and spread apart (diverge).

Principal Components and Definitions

  • Pole (P): The geometric center of the reflecting spherical surface of the mirror.
  • Center of Curvature (C): The center of the hollow sphere of glass from which the mirror was cut. It lies behind the reflecting surface of a convex mirror.
  • Radius of Curvature (R): The radius of the sphere of which the mirror is a part. Under the Cartesian sign convention, $R$ is positive for convex mirrors.
  • Principal Axis: The straight line passing through the Pole (P) and the Center of Curvature (C).
  • Principal Focus (F): The point behind the mirror on the principal axis where all rays parallel to the axis appear to diverge from after reflection.
  • Focal Length (f): The distance between the Pole (P) and the Principal Focus (F). It is positive for convex mirrors and satisfies:
f = R / 2

Rules for Drawing Ray Diagrams

To trace and construct the image formed by a convex mirror, we utilize at least two of the following key rays originating from the tip of the object:

  1. Ray Parallel to Principal Axis: A ray starting parallel to the principal axis reflects such that its back-extension passes through the virtual focus (F) behind the mirror.
  2. Ray Directed Toward Focus: A ray traveling toward the virtual focus (F) reflects parallel to the principal axis.
  3. Ray Directed Toward Center of Curvature: A ray directed toward the Center of Curvature (C) hits the mirror surface perpendicularly (along the normal line) and reflects directly back along its own path.
  4. Ray Striking the Pole: A ray incident at the Pole (P) reflects symmetrically at an equal angle relative to the principal axis (obeying the Law of Reflection, $\theta_i = \theta_r$).

Image Formation and Properties

Unlike concave mirrors, which form different types of images depending on distance, a convex mirror **always** forms the same class of image for any real object position:

Always Virtual

Because the reflected light rays diverge in front of the mirror, they can never intersect to form a real image. The image is formed behind the mirror where the virtual ray extensions meet.

Always Upright (Erect)

The virtual image is oriented in the same vertical direction as the object ($m > 0$). It never flips upside down, which is essential for passenger side mirrors.

Always Diminished

The image formed is always smaller than the actual object size ($|m| < 1$). As the object is brought closer to the mirror, the image grows slightly larger, but it never equals or exceeds the object's height.

Wide Field of View

By curving outward, a convex mirror collects light from a much wider angular cone than a flat mirror, allowing the observer to see a vastly expanded panoramic view.

The Spherical Mirror Equations

The quantitative relationship between the object distance ($u$), image distance ($v$), and focal length ($f$) is governed by the **mirror formula**:

1/f = 1/u + 1/v

The ratio of the image height ($h_i$) to the object height ($h_o$) is defined as the **linear magnification** ($m$):

m = h_i / h_o = -v/u

Cartesian Sign Convention for Convex Mirrors:

  • The object is placed in front of the mirror (against the direction of light), so the object distance **$u$ is always negative** ($u < 0$).
  • The focus and center of curvature lie behind the mirror, so **$f$ and $R$ are always positive** ($f > 0$, $R > 0$).
  • Consequently, the image distance **$v$ is always positive** ($v > 0$), meaning the image is always formed behind the mirror.
  • Since $v$ is positive and $u$ is negative, $m = -v/u$ is **always positive** ($m > 0$), representing an upright, virtual image.

Real-world Applications

  • Automobile Side Mirrors: Used to provide a wide-angle view of the lanes behind, helping drivers change lanes safely.
  • Store Security Mirrors: Dome convex mirrors mounted high in supermarket aisles let clerks monitor hidden corners.
  • Blind Corner Safety: Placed at sharp street turns, parking garage exits, and driveways to show oncoming vehicle headlights.
  • ATM Safety: Small convex mirrors on ATMs allow users to see if someone is standing too close behind them.

Solved Examples

Example 1

An object is placed at a distance of 20.0 cm in front of a convex mirror of focal length 15.0 cm. Find the position, magnification, and properties of the image formed.

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Final Answer:

Example 2

A vehicle uses a convex side-view mirror with a radius of curvature of 3.0 m. If a car behind is located 5.0 m from this mirror, find the position, magnification, and properties of the image formed.

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Final Answer:

Example 3

A convex shop security mirror of focal length 20.0 cm forms an image which is exactly 1/4 of the size of the object. How far is the object located from the mirror?

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Final Answer:

Self-Check Questions

Question 1

Explain why the focal length of a convex mirror is considered positive while that of a concave mirror is negative.

Show Answer & Explanation

By convention, the pole of the mirror is treated as the origin, and the direction of incident light is positive. For a concave mirror, parallel incident rays converge to a real focal point in front of the mirror (against the light direction), making its focal length negative. For a convex mirror, parallel incident rays reflect and diverge; when traced backward, they appear to meet at a virtual focal point behind the mirror (in the direction of light propagation), making its focal length positive.

Question 2

Why is a convex mirror preferred over a plane mirror as a passenger-side rear-view mirror in automobiles?

Show Answer & Explanation

A convex mirror is preferred because it curves outward, which diverges reflected light and provides a significantly wider field of view compared to a flat plane mirror of the same size. This allows drivers to monitor multiple lanes of traffic and reduces dangerous blind spots. However, it makes objects appear smaller and thus look further away than they actually are.

Question 3

A convex mirror is completely submerged in water. How does this affect its focal length and image formation?

Show Answer & Explanation

The focal length of a spherical mirror depends solely on its geometric radius of curvature (f = R/2). Unlike lenses, which rely on light refraction (which changes depending on the surrounding medium's refractive index), mirrors rely on reflection. Since the Law of Reflection holds true in any medium, submerging a convex mirror in water does not change its focal length or the mathematical positions of the images it forms.

Question 4

Can a convex mirror ever form a real image? Explain your answer.

Show Answer & Explanation

Under normal conditions with a real object (where light rays diverge from a physical object in front of the mirror), a convex mirror can ONLY form a virtual, upright, and diminished image behind the mirror. This is because the reflecting surface curves outward, causing all real reflected rays to diverge. However, if a convergent beam of light is incident on the mirror (forming a virtual object behind the mirror between the pole P and focus F), the reflected rays can converge to form a real image in front of the mirror. In school physics, we assume real objects, so images are always virtual.