Practice: What is the distance, d, between the incoming and outgoing rays?

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Ray Nature Of Light | 11 mins | 0 completed | Learn |

Reflection Of Light | 12 mins | 0 completed | Learn Summary |

Refraction Of Light | 32 mins | 0 completed | Learn Summary |

Total Internal Reflection | 13 mins | 0 completed | Learn Summary |

Ray Diagrams For Mirrors | 36 mins | 0 completed | Learn |

Mirror Equation | 20 mins | 0 completed | Learn |

Refraction At Spherical Surfaces | 10 mins | 0 completed | Learn |

Ray Diagrams For Lenses | 23 mins | 0 completed | Learn |

Thin Lens And Lens Maker Equations | 25 mins | 0 completed | Learn |

Concept #1: Reflection of Light

**Transcript**

Hey guys, in this video we're going to talk about the reflection of light off of a boundary between two media, let's get to it. Now remember when a wave encounters a boundary it can do one of two things, it can either reflect off of that boundary or it can transmit through that boundary and propagate in the new media in reality waves are going to do a little bit of both now for light boundary's are typically referred to or media I should say are typically referred to as one of two things they can either be reflective like the surface of a mirror and mainly only allow reflection or they can be transparent like glass and mainly allow transmission. For now we want to talk about reflective surfaces alright light reflects off of a boundary in the same manner as a ball undergoing an elastic collision with a wall, if we have a ball at some point with some momentum right here and some direction when it hits the wall it's going to conserve that momentum but it's going to go in the opposite direction, and it's going to enter with some angle and it's going to leave with some other angle light is going to do the same thing if I draw a ray of lights encountering a boundary between two media that ray is going to leave at some angle we have something called the Law of reflection which holds for the elastic collision just like it holds for reflection of light that states that that reflected angle is actually the same as the incident angle the angle with which it hits the boundary. Now just as a side note this isn't going to be important right now but this is going to be very important later whenever light encounters a boundary we always measure the angle relative to the normal direction, relative to some line that is perpendicular to the boundary right, this is the normal just like the normal force is perpendicular, the normal direction is perpendicular to a surface.

Let's do an example, we want to find the missing angle theta using the law of reflection, so this light ray is incident at 65 degrees it undergoes reflection right here which means that the outgoing angle is also going to be 65 degrees that's just what the law of reflection says. Now notice this is the normal to this surface which means that it's at a 90 degree angle from the surface so this angle right here is going to be the complementary angle to 65 degrees which is 25 degrees. Right because they have to add up to 90, now notice we have a triangle right here that looks like this here is our 25 degree angle, here's our 125 degree angle and here is an unknown angle. Let me minimise myself, remember that the sum of all the internal angles within a triangle has to be 180 so 25 degrees plus 120 degrees plus this unknown angle has to be 180 degrees. That means that this unknown angle is actually 35 degrees. So that tells us what this angle is this angle is 35 degrees. Now once again this line right here is the normal to the second surface which means that its perpendicular to the second surface so this angle right here is going to be the complimentary angle to 35 degrees right, the angle that when added to 35 degrees equals 90 and that is 55 degrees. So what is theta have to be? Well the law of reflection says it has to be the same as that incident angle which on the second surface is 55 degrees so theta therefore is 55 degrees. Alright guys that wraps up our discussion on the reflection of light and the law of reflection. Thanks for watching.

Example #1: Hanging Mirror

θ=38.7°

**Transcript**

Hey guys lets do an example, a flat mirror hangs 0.2 meters off the ground. If a person 1.8 meters tall stands 2 meters from the mirror, which we called X that can be seen in the mirror? The geometry for this problem is already set up all we have to do is use the law of reflection to figure it out. So this light ray is coming up off the ground from this point encountering the mirror at its lowest points and then leaving in this direction to your eyes which are going to be here, what we have to do is use the law of reflection to figure out what angle properly adjust that light ray so that meets you at exactly 1.8 meters off the ground. Here is the normal because we always use the normal when measuring angles so this is our incident angle theta 1 and this is our reflected angle theta 1 prime and remember that those two are equal now notice if I were to continue this normal line right here we form a triangle right the triangle that we form is 2 meters wide, how tall is it ? well it's not 1.8 meters tall because the mirror the bottom of this point right here is 0.2 meters off the ground so it's actually 1.8 minus 0.2 which is 1.6 meters and this angle right here is theta 1 prime, which is the angle that we're interested in finding. So clearly we can just use trigonometry to find this we can use the tangent and we consider the tangent of theta 1 prime is going to be the opposite edge which is 1.6 meters divided by the adjacent edge which is 2 and that tells us that theta 1 prime is just 51.3 degrees. So now we know that this angle is 51.3 degrees so this angle too is 51.3 degrees.

So we have a new triangle right here, let me minimise myself we have a new triangle now this lower triangle, where this angle the incident angle is 51.3 degrees this height is 0.2 meters and this length is X. What's this angle going to be? Well this is what's known as an alternate interior angle to 51.3 and all alternate interior angles are the same so this is going to be 51.3 degrees. Alright so once again we can use the tangent to find what X should be we can just say then that the tangents of 51.3 degrees equals the opposite which is 0.2 meters divided by the adjacent which is X or that X is 0.2 over the tangent of 51.3 degrees and finally that X is just 0.25 meters. Just using geometry and trigonometry we can answer this question the crux of the physics is that V these angles right here are the same and that's the law of reflection. Alright guys thanks for watching.

Practice: What is the distance, d, between the incoming and outgoing rays?

0 of 3 completed

A 1.7 m tall person stands 1 m in front of a flat, reflective surface. What is the minimum height of this surface that would allow them to see their entire body in the reflection?

In the following figure, a light ray is incident on a reflective surface as shown. How far apart are the incident ray and the ray reflected off of the vertical surface? Hint: the two rays are parallel.

Two mirrors are set up at right angles to each other. A ray of light is incident on mirror 1 with an angle of incidence of 60°. What is the angle of reflection for mirror 2?
A. 60°
B. 30°
C. 90°
D. 15°
E. 45°

The reflecting surfaces of two intersecting flat mirrors are at an angle of 54°, as shown in the figure. A light ray strikes the horizontal mirror at an angle of 57° respect to the mirror’s surface. Calculate the angle Φ.

A light ray is incident on a reflecting surface. If the light ray makes a 25° angle with respect to the normal to the surface, what is the exact angle (in degrees) made by the reflected ray relative to the normal?

A light ray leaves point A in Figure 1, reflects from the mirror, and reaches point B. a) How far below the top edge does the ray strike the mirror? b) What if the distance from point B to the mirror was reduced by 5 cm?

a) If light rays actually converge to the image point, the image is said to be a (virtual/real?) Image and the image distance is positive. b) If the rays diverge, they should be extended backward with dashed lines to the common image point where they appear to meet. The image is said to be a (virtual/real?) image.

Which of the following statements are true concerning the reflection of light?Check all that apply.The angle of incidence is equal to the angle of reflection only when a ray of light strikes a plane mirror.The reflection of light from a smooth surface is called specular reflection.The reflection of light from a rough surface is called diffuse reflection.For diffuse reflection, the angle of incidence is greater than the angle of reflection.For specular reflection, the angle of incidence is less than the angle of reflection.

The mirror in the figure reflects a horizontal laser beam by 60What is the angle (phi)?

Which of the following statements are true for an image formed by a plane mirror?a) The image always appears to be located the same distance behind the mirror as the object is located in front of the mirror. b) The image formed by a plane mirror is always a real image. c) The image is always larger than the object. d) The image formed by a plane mirror is always an upright image. e) The image formed by a plane mirror is always an inverted image. f) The image formed by a plane mirror is always a virtual image.

A light ray is incident on a reflecting surface. If the light ray makes a 25° angle with respect to the normal to the surface, what is the exact angle (in degrees) made by the reflected ray relative to the normal?

Which of the following statements are true concerning the reflection of light? Check all that apply. a. For diffuse reflection, the angle of incidence is greater than the angle of reflection. b. The angle of incidence is equal to the angle of reflection only when a ray of light strikes a plane mirror. c. The reflection of light from a rough surface is called diffuse reflection. d. For specular reflection, the angle of incidence is less than the angle of reflection. e. The reflection of light from a smooth surface is called specular reflection.

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