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10 min read•june 18, 2024
Daniella Garcia-Loos
Saarah Hasan
Daniella Garcia-Loos
Saarah Hasan
Let’s talk about mirrors, optical devices that form images by reflecting light. We’ve all looked into a mirror and seen images of our faces and nearby objects; in this section, we’re going to analyze those images mathematically.
Plane mirrors are flat mirrors, and they’re the simplest type of mirror. Now, how is an image of an object in a mirror even formed? Well, light that’s reflected off of the object hits the mirror and reflects back into our eyes. The direction of the reflected rays determine where we perceive the image of the object to be.
We’re going to dive into the image characteristics of plane mirrors by answering the following questions:
1. Where’s the image, and how does the height of it compare with the object’s?
2. Is the image real or virtual?
3. Is the image upright or inverted?
(1) Think back to when you look at yourself in a flat mirror; it seems as if the image of yourself is behind the mirror. When you take a step sideways, the image of you also steps sideways. The image seems as far behind the mirror as the object is in front of the mirror(the law of reflection can be used to show this). In a flat mirror, the image isn’t enlarged or shrunken compared to the size of the object.
(2) First off, what does it mean for an image to be real or virtual? An image is real if the light rays actually focus at the image; the light converges and passes through the actual image location. For flat mirrors, the image is virtual: light rays don’t actually pass through the image location on the other side of the mirror.
(3) Once again, re-imagine looking at yourself in a flat mirror. Your image isn’t upside down; it’s upright. Question 3 answered.
Check out this interactive to really solidify your understanding of plane mirrors.
Concave and convex mirrors are spherical mirrors, mirrors that are specifically curved so that their surfaces form part of a sphere.
The focal length is one-half of the the radius of curvature:
f=R/2
The image above was a concave mirror; the reflective side is caved in towards the center of curvature. The following image is a convex mirror; the reflective side curves away from the center of curvature.
Ray tracing is an essential tool that helps us determine the location of the image. We draw representative light rays in a diagram along with the object and the mirror: the point at which the reflected rays intersect is the location of the image. Let’s go over some of the ray tracing rules:
Here are the steps for ray tracing for mirrors:
Concave Mirrors:
Convex Mirrors:
With ray tracing, if the image is on the same side of the mirror as the object, then the image is real; if it’s formed on the opposite side, it’s virtual. Other aspects of the image (its size, location, orientation) can be also determined by ray tracing. It might be a little tricky at first, but with practice, it'll get easier.
To answer our questions about images in an easier and faster way, we can use two equations. The first is the mirror equation:
1/f=1/d_o+1/d_i
To differentiate mathematically between concave and convex, we set the focal length to the following:
The second equation is the magnification equation:
M=-d_i/d_o=h_i/h_o
h_i: height of image
h_o: height of object
Keep in mind that all real images are inverted and all virtual images are upright.
Lenses are optical devices that form images by refracting light. There are 2 types of lenses: converging and diverging.
Converging (convex) lens—converges parallel light rays to a focal point on the far side.
Diverging (concave) lens—causes light rays to diverge away from a focal point on the same side as the incident rays.
Just as we did with mirrors, we can use ray tracing with lenses to get information about an image. Let’s go over the rules for ray tracing for lenses:
Here are the steps for ray tracing for lenses:
Convex Lenses:
Concave Lenses:
Lens and mirrors use the same equations! Just keep in mind that:
Some simulations to check out for lenses and mirrors:
Concave Mirror Image Formation
Converging Lens Image Formation
Diverging Lens Image Formation
1. A plane mirror produces an image that is:
A) real, inverted, and larger than the object.
B) real, upright, and the same size of the object.
C) real, upright, and smaller than the object.
D) virtual, inverted, and smaller than the object.
E) virtual, upright, and the same size as the object.
2. An object is located 0.20 meters from a converging lens which has a focal length of 0.15 meters. Relative to the object, the image formed by the lens will be:
B) real, inverted, smaller
C) real, inverted, larger
D) virtual, erect, larger
E) virtual, inverted, smaller
3. A narrow beam of monochromatic light enters a lens parallel to the optic axis, as shown in the accompanying diagram. Which arrow best represents the direction of the light after leaving the lens?
B) B
C) C
D) D
E) E
4. A beam of light traveling in glass (n_gng = 1.5) strikes a boundary with air (n_ana = 1.0) at point P. The angle of incidence is 60° as shown in the diagram. Which ray would best indicate the beam’s path after point P?
A) A
B) B
C) C
D) D
E) E
5. An object is placed 10 cm in front of the center of a concave curved mirror with a radius of curvature of 10 cm. About how far from the mirror will the real image of the object be formed?
A) 0 cm
B) 5 cm
C) 10 cm
D) 20 cm
E) No image is formed
6. A diverging lens produces an image of a real object. This image is
A) virtual, larger than the object, and upright
B) virtual, smaller than the object, and upright
C) virtual, smaller than the object, and inverted
D) real, smaller than the object, and inverted
7. An illuminated object is placed 0.30 meter from a lens whose focal length is –0.15 meter. The image is
A) inverted, real, and 0.30 meter from the lens on the opposite side from the object
B) upright, virtual, and 0.30 meter from the lens on the opposite side from the object
C) upright, real, and 0.10 meter from the lens on the same side as the object
D) upright, virtual, and 0.10 meter from the lens on the same side as the object
Use the Figure above for questions 8 and 9. An object O is located at point P to the left of a converging lens, as shown in the figure. F_1F1 and F_2F2 are the focal points of the lens.
8. If the focal length of the lens is 0.40 m and point P is 0.30 m to the left of the lens, where is the image of the object located?
A) 1.2 m to the left of the lens B) 0.17 m to the left of the lens C) At the lens D) 0.17 m to the right of the lens E) 1.2 m to the right of the lens
9. Which of the following characterizes the image when the object is in the position shown?
A) Real, inverted, and smaller than the object B) Real, upright, and larger than the object C) Real, inverted, and larger than the object D) Virtual, upright, and larger than the object E) Virtual, upright, and smaller than the object
10. A physics student places an object 6.0 cm from a converging lens of focal length 9.0 cm. What is the magnitude of the magnification of the image produced?
A) 0.6
B) 1.5
C) 2.0
D) 3.0
E) 3.6
Answers:
E: Plane mirrors always makes virtual, same size, upright images
C: Using the math, 1/f = 1/do + 1/di, and M = – di / do … di +0.6 M = – 3 …
E: A horizontal beam approaching a converging lens bends and converges through the focal point
E: Generally when we go from more–less we should always check the critical angle first rather than assuming the ray will refract and bend away. Choice D might be correct, but not until we first check the critical angle for total internal reflection. Use ni sin θc = nr sin (90), ni=1.5, nr=1θc = 41.8°. Since our incoming angle (60) is larger than the critical angle, total internal reflection will occur and you will get choice E.
C: The focal point is = R/2. Then use the math 1/f = 1/do + 1/di … and di = 10
E: Fact about diverging lens.
D: Using the math, 1/f = 1/do + 1/di, and M = – di / do … di = – 0.10 m, M = +0.33
A: Using the math, 1/f = 1/do + 1/di, di = –1.2. Its virtual so its on the same side as the object, which puts the image on the left side of the lens
D: This is a magnifying glass, which can be memorized or the math can be done to prove the answer
D: Using the math, 1/f = 1/do + 1/di, di = –18 … then M = – di / do … M = 3
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10 min read•june 18, 2024
Daniella Garcia-Loos
Saarah Hasan
Daniella Garcia-Loos
Saarah Hasan
Let’s talk about mirrors, optical devices that form images by reflecting light. We’ve all looked into a mirror and seen images of our faces and nearby objects; in this section, we’re going to analyze those images mathematically.
Plane mirrors are flat mirrors, and they’re the simplest type of mirror. Now, how is an image of an object in a mirror even formed? Well, light that’s reflected off of the object hits the mirror and reflects back into our eyes. The direction of the reflected rays determine where we perceive the image of the object to be.
We’re going to dive into the image characteristics of plane mirrors by answering the following questions:
1. Where’s the image, and how does the height of it compare with the object’s?
2. Is the image real or virtual?
3. Is the image upright or inverted?
(1) Think back to when you look at yourself in a flat mirror; it seems as if the image of yourself is behind the mirror. When you take a step sideways, the image of you also steps sideways. The image seems as far behind the mirror as the object is in front of the mirror(the law of reflection can be used to show this). In a flat mirror, the image isn’t enlarged or shrunken compared to the size of the object.
(2) First off, what does it mean for an image to be real or virtual? An image is real if the light rays actually focus at the image; the light converges and passes through the actual image location. For flat mirrors, the image is virtual: light rays don’t actually pass through the image location on the other side of the mirror.
(3) Once again, re-imagine looking at yourself in a flat mirror. Your image isn’t upside down; it’s upright. Question 3 answered.
Check out this interactive to really solidify your understanding of plane mirrors.
Concave and convex mirrors are spherical mirrors, mirrors that are specifically curved so that their surfaces form part of a sphere.
The focal length is one-half of the the radius of curvature:
f=R/2
The image above was a concave mirror; the reflective side is caved in towards the center of curvature. The following image is a convex mirror; the reflective side curves away from the center of curvature.
Ray tracing is an essential tool that helps us determine the location of the image. We draw representative light rays in a diagram along with the object and the mirror: the point at which the reflected rays intersect is the location of the image. Let’s go over some of the ray tracing rules:
Here are the steps for ray tracing for mirrors:
Concave Mirrors:
Convex Mirrors:
With ray tracing, if the image is on the same side of the mirror as the object, then the image is real; if it’s formed on the opposite side, it’s virtual. Other aspects of the image (its size, location, orientation) can be also determined by ray tracing. It might be a little tricky at first, but with practice, it'll get easier.
To answer our questions about images in an easier and faster way, we can use two equations. The first is the mirror equation:
1/f=1/d_o+1/d_i
To differentiate mathematically between concave and convex, we set the focal length to the following:
The second equation is the magnification equation:
M=-d_i/d_o=h_i/h_o
h_i: height of image
h_o: height of object
Keep in mind that all real images are inverted and all virtual images are upright.
Lenses are optical devices that form images by refracting light. There are 2 types of lenses: converging and diverging.
Converging (convex) lens—converges parallel light rays to a focal point on the far side.
Diverging (concave) lens—causes light rays to diverge away from a focal point on the same side as the incident rays.
Just as we did with mirrors, we can use ray tracing with lenses to get information about an image. Let’s go over the rules for ray tracing for lenses:
Here are the steps for ray tracing for lenses:
Convex Lenses:
Concave Lenses:
Lens and mirrors use the same equations! Just keep in mind that:
Some simulations to check out for lenses and mirrors:
Concave Mirror Image Formation
Converging Lens Image Formation
Diverging Lens Image Formation
1. A plane mirror produces an image that is:
A) real, inverted, and larger than the object.
B) real, upright, and the same size of the object.
C) real, upright, and smaller than the object.
D) virtual, inverted, and smaller than the object.
E) virtual, upright, and the same size as the object.
2. An object is located 0.20 meters from a converging lens which has a focal length of 0.15 meters. Relative to the object, the image formed by the lens will be:
B) real, inverted, smaller
C) real, inverted, larger
D) virtual, erect, larger
E) virtual, inverted, smaller
3. A narrow beam of monochromatic light enters a lens parallel to the optic axis, as shown in the accompanying diagram. Which arrow best represents the direction of the light after leaving the lens?
B) B
C) C
D) D
E) E
4. A beam of light traveling in glass (n_gng = 1.5) strikes a boundary with air (n_ana = 1.0) at point P. The angle of incidence is 60° as shown in the diagram. Which ray would best indicate the beam’s path after point P?
A) A
B) B
C) C
D) D
E) E
5. An object is placed 10 cm in front of the center of a concave curved mirror with a radius of curvature of 10 cm. About how far from the mirror will the real image of the object be formed?
A) 0 cm
B) 5 cm
C) 10 cm
D) 20 cm
E) No image is formed
6. A diverging lens produces an image of a real object. This image is
A) virtual, larger than the object, and upright
B) virtual, smaller than the object, and upright
C) virtual, smaller than the object, and inverted
D) real, smaller than the object, and inverted
7. An illuminated object is placed 0.30 meter from a lens whose focal length is –0.15 meter. The image is
A) inverted, real, and 0.30 meter from the lens on the opposite side from the object
B) upright, virtual, and 0.30 meter from the lens on the opposite side from the object
C) upright, real, and 0.10 meter from the lens on the same side as the object
D) upright, virtual, and 0.10 meter from the lens on the same side as the object
Use the Figure above for questions 8 and 9. An object O is located at point P to the left of a converging lens, as shown in the figure. F_1F1 and F_2F2 are the focal points of the lens.
8. If the focal length of the lens is 0.40 m and point P is 0.30 m to the left of the lens, where is the image of the object located?
A) 1.2 m to the left of the lens B) 0.17 m to the left of the lens C) At the lens D) 0.17 m to the right of the lens E) 1.2 m to the right of the lens
9. Which of the following characterizes the image when the object is in the position shown?
A) Real, inverted, and smaller than the object B) Real, upright, and larger than the object C) Real, inverted, and larger than the object D) Virtual, upright, and larger than the object E) Virtual, upright, and smaller than the object
10. A physics student places an object 6.0 cm from a converging lens of focal length 9.0 cm. What is the magnitude of the magnification of the image produced?
A) 0.6
B) 1.5
C) 2.0
D) 3.0
E) 3.6
Answers:
E: Plane mirrors always makes virtual, same size, upright images
C: Using the math, 1/f = 1/do + 1/di, and M = – di / do … di +0.6 M = – 3 …
E: A horizontal beam approaching a converging lens bends and converges through the focal point
E: Generally when we go from more–less we should always check the critical angle first rather than assuming the ray will refract and bend away. Choice D might be correct, but not until we first check the critical angle for total internal reflection. Use ni sin θc = nr sin (90), ni=1.5, nr=1θc = 41.8°. Since our incoming angle (60) is larger than the critical angle, total internal reflection will occur and you will get choice E.
C: The focal point is = R/2. Then use the math 1/f = 1/do + 1/di … and di = 10
E: Fact about diverging lens.
D: Using the math, 1/f = 1/do + 1/di, and M = – di / do … di = – 0.10 m, M = +0.33
A: Using the math, 1/f = 1/do + 1/di, di = –1.2. Its virtual so its on the same side as the object, which puts the image on the left side of the lens
D: This is a magnifying glass, which can be memorized or the math can be done to prove the answer
D: Using the math, 1/f = 1/do + 1/di, di = –18 … then M = – di / do … M = 3
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