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1 Thin Lens Light refracts on the interface of two media, following Snell’s law of refraction: Light bends through a triangular prism: θ 1 and θ 2 are.

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Presentation on theme: "1 Thin Lens Light refracts on the interface of two media, following Snell’s law of refraction: Light bends through a triangular prism: θ 1 and θ 2 are."— Presentation transcript:

1 1 Thin Lens Light refracts on the interface of two media, following Snell’s law of refraction: Light bends through a triangular prism: θ 1 and θ 2 are both with respect to the normal of the interface. The parameters n 1 and n 2 are call the index of medium 1 and 2 respectively. Medium 1 Medium 2 θ1θ1 θ2θ2 Light converges

2 2 Thin Lens Light bends through an upside-down triangular prism: Light diverges The back traces of the diverging light meet at one point.

3 3 Thin lens Converging thin lens:  All light rays parallel to the principal axis meet at the focal point on the other side of the lens (far focal point).  The focal points on either side of the lens are equal distance from the center of the lens. This distance is called the focal length and it is a positive value.  It is considered that the thin lens has no thickness. And it is of represented by a double out-going arrowed line. Converging thin lens

4 4 Thin lenses Diverging thin lens:  All light rays parallel to the principal axis diverge, but their back traces meet at the focal point on the same side of the lens (near focal point).  The focal points on either side of the lens are equal distance from the center of the lens. This distance is called the focal length and is a negative value.  It is considered that the thin lens has no thickness. And it is of represented by a double inward-going arrowed line. Diverging thin lens

5 5 Find image with a thin lens Converging lens Ray 1: Parallel to axis, then passes through far focal point Ray 2: Passes unchanged through center of lens Ray 3: Passes through near focal point, then parallel to axis

6 6 Find image with a thin lens Converging lens F F f Object hoho dodo Real image, inverted, smaller hihi didi

7 7 Find image with a thin lens Converging lens F F f 2f Real, inverted, smaller F F f 2f Real, inverted, same size

8 8 Find image with a thin lens Converging lens F F f 2f Real, inverted, larger F F f 2f No image

9 9 Find image with a thin lens Converging lens F F f 2f Virtual, upright, larger Like in the converging mirror case, there are 5 possible object locations that produce different images. Diverging lens, Like in the diverging mirror case, no matter where the object is placed, you always get a virtual, upright and smaller image.

10 10 Find image with a thin lens Diverging lens Ray 1 Parallel to axis, virtual ray passes through near focal point Ray 2 Straight through center of lens Ray 3 Virtual ray through far focal point, virtual ray parallel to axis

11 11 Find image with a thin lens Diverging lens F F f Object hoho dodo Virtual image, upright, smaller hihi didi

12 12 Analytical calculations Thin lens equation. hoho hihi

13 13 Analytical calculations In the mirror case, there is a formula connects the radius and focal length: Here the value of the radius is always positive. Converging mirror Diverging mirror

14 14 Analytical calculations Lens maker’s equation: The formula for a lens in vacuum (air): n : index of refraction of the lens material. R 1 : radius of near surface. R 2 : radius of far surface. The near or far surface is with respect to the focal point F. Near side is surface 1, far side is surface 2. The sign of the radius is then defined as “ + ” if the center is on the far side; “ - ” if the center is on the near side. In this convention, positive f means converging lens, negative f means diverging lens. F near surface far surface

15 15 Analytical calculations Lens maker’s equation: The formula for a lens (n lens ) in medium n medium : R 1 : radius of near surface. R 2 : radius of far surface. F near surface far surface n medium

16 16 More sign conventions

17 17 Sign convention table

18 18 Example 1 Find the image distance. /m d i = 1.0 m

19 19 Example 2 Prove for a thin lens, the focal length on both side of the lens is the same.

20 20 Example 3 A thin lens has a focal lens of f a = 5 mm in air. The index of refraction of the lens material is 1.53. If this lens is placed in water (n = 1.33), what will the lens’ focal length in water?

21 21 Example 4 A thin lens has a near surface with a radius of curvature of −5.00 cm and a far surface with a radius of curvature of +7.00 cm. (a) Is the lens converging or diverging? (b) What is the focal length of the lens if the index of refraction of the material is 1.74?

22 22 Example 5 A small light bulb is placed a distance d from a screen. You have a converging lens with a focal length of f. There are two possible distances from the bulb at which you could place the lens to create a sharp image on the screen. (a) Derive an equation for the distance z between the two positions that includes only d and f. (b) Use this equation to show that the distance d between an object and a real image formed by a converging lens must always be greater than or equal to four times the focal length f.


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