Section Lens and Mirrors

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Lenses

BiconvexLens
Converging Lens.

Lenses are designed to refract light in a specific way to form images.

Ideal vs Reality

  • The idea of a focal point is actually an naive idealization.
  • In theory and in reality, one cannot construct a static lens or mirror that gathers all parallel light rays to an arbitrarily small point.
  • It would have violated the second law of thermodynamics because such a lens could generate an arbitrarily high temperature from a low temperature light source.
  • Mathematically it came from the conservation of volume in phase space $\Delta x \Delta p$ in classical mechanics.
  • Light rays will always miss each other slighlty around the focal point (i.e. slightly blurring the image) due to the above fundamental constraint from physics.

There are two types of lenses:

In this course we will only study symmetrical lenses, so both sides of the lenses are the same.

Converging (convex) lens. Also known as positive lens because $f\gt 0$.
Large convex lens
Light rays deflected by a converging lens.
Diverging (concave) lens. Also known as negative lens because $f\lt 0$.
Concave lens
Light rays deflected by a diverging lens.

Principle rays

Simulation - Converging and Diverging Lens: The Principle Rays

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Drag to move the object, and to change the focal lengths.
Dragging the focal points to the other side of the lens will change the lens from converging to diverging and vice versa.
Click on "Switch Rays" to show one principle ray at a time.
This simulation focuses on showing the rules regarding the principle rays so the image is purposely omitted. See the next simulation to learn how to find the image.
The symbols for the converging lens (left) and diverging lens (right) in a ray diagram. The symbols allow you to draw the lens accurately using rulers.

Image formation

Real vs virtual image

Drawing ray diagrams

Simulation - Converging and Diverging Lens: Finding the Image

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Drag to move the object, and to change the focal lengths.
Dragging the focal points to the other side of the lens will change the lens from converging to diverging and vice versa.

Video - Ray diagrams for lenses 1

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Video - Ray diagrams for lenses 02

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The lens equation
The location of the image can be found using the lens equation:
$$ \frac{1}{p} + \frac{1}{i} = \frac{1}{f} $$
Always ensure the focal length obeys the rule: $$ \left\{ \begin{eqnarray} f &\gt& 0 \hspace{1cm} \text{(converging lens)} \\ f &\lt& 0 \hspace{1cm} \text{(diverging lens)} \end{eqnarray} \right. $$ The image distance obeys the sign convention: $$ \left\{ \begin{eqnarray} i &\gt& 0 \hspace{1cm} \text{(image right of the lens)} \\ i &\lt& 0 \hspace{1cm} \text{(image left of the lens)} \end{eqnarray} \right. $$

The red arrows are the images at different lateral magnifications. The postions of the images are arbitrary and are not meant to represent $i$.

Lateral magnification
The magnification is the ratio of the image size $h_i$ to the object size $h_o$, and can be found with the object and image distances:
$$ m = \frac{h_i}{h_o} = -\frac{i}{p} $$

Describing the image
If you are asked to describe the image, it means answering three questions: Converging lens is complicated, but a diverging lens always produces images that are:

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When the object is on the focal point of a converging lens (i.e. $p=f$, the case between the two exercises above), the outgoing light rays are parallel and therefore never meet. We either say "no image is formed", or "the image is at infinity".

Convex lens (magnifying glass) and upside-down image
A converging lens viewing objects far away ($p \gt f$). The image is inverted ($m \lt 0$). For $p\gt 2f$ (such as the house in the figure), the image is also diminished ($|m|\lt 1$).
Magnifying glass2
A converging used as an magnifying glass when the object is put between $F$ and the lens ($p \lt f$). Note that the image is magnified ($m \gt 1$) and the object is upright ($m$ positive).
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Simulation - Two Lenses

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Drag to move the object, and to change the focal lengths.
Dragging the focal points to the other side of the lens will change the lens from converging to diverging and vice versa.

Curved Mirrors

Anamorfosi
A reflective surface acting as a diverging (convex) mirror.

There are two types of curved mirrors:

Principle rays

Simulation - Converging and Diverging Mirrors: The Principle Rays

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Drag to move the object, mirror, and to change the focal length.
Dragging the focal point to the other side of the mirror will change the mirror from converging to diverging and vice versa.
Click on "Switch Rays" to show one ray at a time.
This simulation focuses on showing the rules regarding the principle rays so the image is purposely omitted. See the next simulation to learn how to find the image.
The symbols for the converging mirror (left) and diverging mirror (right) in a ray diagram. The symbols allow you to draw the mirrors accurately using rulers.

The same equations apply for curved mirrors.

Lateral magnification:

$$ m = \frac{h_i}{h_o} = -\frac{i}{p} $$
The lens equation:
$$ \frac{1}{p} + \frac{1}{i} = \frac{1}{f} $$
Always ensure the focal length obeys the rule: $$ \left\{ \begin{eqnarray} f &\gt& 0 \hspace{1cm} \text{(converging mirror)} \\ f &\lt& 0 \hspace{1cm} \text{(diverging mirror)} \end{eqnarray} \right. $$ The image distance obeys the sign convention: $$ \left\{ \begin{eqnarray} i &\gt& 0 \hspace{1cm} \text{(image left of (in front of) the mirror)} \\ i &\lt& 0 \hspace{1cm} \text{(image right of (behind) the mirror)} \end{eqnarray} \right. $$

Simulation - Converging and Diverging Mirrors: Finding the Image

Canvas not supported
Drag to move the object, mirror, and to change the focal length.
Dragging the focal point to the other side of the mirror will change the mirror from converging to diverging and vice versa.
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002 2014 03 15 Spiegel
View of a diverging mirror. The image is upright, diminished, and virtual.
© Friedrich Haag / Wikimedia Commons

Applications

Myopia and lens correction
Short-sightedness (myopia). Image is formed in front of the retina, but can be corrected by a diverging lens.
Hypermetropia color
Far-sightedness (hyperopia). Image is formed behind the retina, but can be corrected by a converging lens.
OpenStax Astronomy refracting and reflecting telescopes
Refracting vs reflecting telescopes. All major telescopes of today are of the reflecting type.
NewtonsTelescopeReplica
Newton's reflecting telescope.

Sign Conventions & Notations

Sign conventions
Converging lens Diverging lens Converging mirror Diverging mirror
Other name Convex lens Concave lens Concave mirror Convex mirror
$f$ $+$ $-$ $+$ $-$
$i$ when image on the left $-$ $-$ $+$ $+$
$i$ when image on the right $+$ $+$ $-$ $-$
Notations
Name Symbol Meaning
Focal point $F$ the point where rays parallel to the principle axis converge
Focal length $f$ distance between $F$ and the lens
Object distance $p$ distance between the object and the lens
Image distance $i$ distance between the image and the lens
Center of curvature $2F$ or $C$ center of the sphere of which the curved mirror is part of
Radius of curvature $2f$ or $R$ distance between $2F$ and the mirror