1. Dispersion
The spreading of light into its color components is called dispersion.
When light enters a prism, the refracted ray is bent towards the normal, and when it leaves the prism, it is refracted away from the normal.

2. Dispersion
The refractive index of glass depends on the wavelength of light (see p. 809)
This means that different colors get bent by different amounts and depart a prism traveling in different directions… resulting in a rainbow

3. The physics of rainbows
Rainbows occur because light is refracted as it enters and leaves a water droplet.
the index of refraction depends on the color (wavelength), so each color is bent a different amount.

4. The physics of rainbows
From each droplet we see only one color, since it is the only ray traveling in the direction to our eye.
But every droplet reflects at the same angle for a given color (wavelength)
The position of the droplet, relative to our eye, determines which color we see.

5. Thin Lenses
Lenses are made of transparent materials that refract light in such a way that an image of the source of the light is formed.
We assume that the lens is so thin compared to the focal length (f) that it makes no difference whether f is measured between the focal point and either surface of the lens, or the center of the lens.

6. Converging Lens
Converging lens: paraxial rays (rays near the principle axis) that are parallel to the principal axis converge to the focal point F after passing through the lens.
For an object that is infinitely far away, the image is formed at the focal point (F)

7. Diverging Lens
Diverging lens: causes infinite parallel rays to diverge after exiting the lens.
Paraxial rays that are parallel to the principal axis appear to originate from a single point on the axis after passing through the lens.
This point is the focal point (F) and its distance from the lens is the focal length (f)

8. Diverging Lens
Diverging lens: causes infinite parallel rays to diverge after exiting the lens.
Paraxial rays that are parallel to the principal axis appear to originate from a single point on the axis after passing through the lens.
This point is the focal point (F) and its distance from the lens is the focal length (f)

9. Ray Tracing to find images
Just like with curved mirrors, we can use ray tracing to locate the image formed by thin lenses.

10. Ray Tracing to find images
Just like with curved mirrors, we can use ray tracing to locate the image formed by thin lenses.

11. The thin lens equation
1 𝑑𝑜 + 1 𝑑𝑖 = 1 𝑓
𝑚= ℎ𝑖 ℎ𝑜 =− 𝑑𝑖 𝑑𝑜

12. Sign Conventions for lenses
f is + for converging lens
f is – for diverging lens
di is + for a real image formed to the right of the lens
di is – for a virtual image formed to the left of the lens
m is + if image is upright
m is – if image is inverted

13. Example 1 Converging Lens
A person 1.70 m tall is standing 2.50m in front of a digital camera. The camera uses a converging lens whose focal length is m.
Find the image distance and determine whether the image is real or virtual.
Find the magnification and the height of the image.

14. Example 1 Converging Lens
A person 1.70 m tall is standing 2.50m in front of a digital camera. The camera uses a converging lens whose focal length is m.
Find the image distance and determine whether the image is real or virtual.
Find the magnification and the height of the image.

15. Example 2 Diverging Lens
An object is placed 7.10cm to the left of a diverging lens whose focal length is f=-5.08cm
Find the image distance and determine whether the image is real or virtual
Obtain the magnification

16. Assignment
Problems p. 837 #44, 46, 50, 51, 55