Announcements Review Chromatic Dispersion Aberrations Optical Instruments Sections 25.1 - 25.3 Optical Instruments The Camera Final Questions Announcements Review Chromatic Dispersion Aberrations The Camera Reading Assignment Read sections 25.4 - 25.5 Homework Assignment 8 Homework for Chapter 23 at due at the beginning of class today Homework Assignment 9 Homework for Chapter 25 (due at the beginning of class on Wednesday, October 27) Q: 3, 6, 14 P: 16, 24 Optical Instruments Final Questions Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions Question A diverging lens has a focal length of 10.0 cm. An object is placed 30.0 cm from the lens. Find the image distance and describe the image. Optical Instruments Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions Question A diverging lens has a focal length of 10.0 cm. An object is placed 30.0 cm from the lens. Find the image distance and describe the image. Answer Because the lens is a diverging lens, its focal length is negative Because the lens is diverging, we expect it to form an upright, reduced, virtual image for any object position Using the thin lens equation 1/p + 1/q = 1/f and solving for q we find that q 1 1 = = −7.50 cm − q p −1 = 1 1 − −10.0 cm 30.0 cm −1 The magnification of the image is M =− q p −7.50 cm =− 30.0 cm = +0.250 This result confirms that the image is virtual, smaller than the object, and upright Optical Instruments Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions The human eye The human eye focuses light and produces sharp images (much like a lens or a camera, though much more complex) Only three types of color-sensitive cells are present in the retina (red, green, and blue cones) If the red and green cones are stimulated simultaneously, the brain interprets what is seen as yellow If all three types of cones are stimulated simultaneously, white light is seen White light The color white is the perception that is evoked by light that stimulates all three types of color sensitive cone cells in the human eye The sun and incandescent lightbulbs are sources of white light Reflection, transmission, and absorption When light strikes an object, it may either (1) by reflected by the surface of the object, (2) be transmitted through the object (refraction) or (3) be absorbed by the object The color of the objects that we see are largely due to the way these objects reflect or transmit light to our eyes The color of an object is in the light that shines upon it and is ultimately reflected or transmitted to our eyes For example, if an object absorbs all of the frequencies of visible light except for the frequency associated with green light, then the object will appear green Optical Instruments Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions Chromatic dispersion An important property of the index of refraction n is that, for a given material, the index varies with the wavelength of the light passing through the material This behavior is called chromatic dispersion Because n is a function of the wavelength, Snell’s law of refraction indicates that light of different wavelengths is refracted at different angles when incident on a material The index of refraction generally decreases with increasing wavelength (in other words, violet light refracts more than red light does when passing into a material) Optical Instruments Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions Lens aberrations Our analysis of mirror and lenses assumes that rays make small angles with the principal axis and that the lenses are thin When these approximations do not hold, imperfect images (aberrations) are formed There are three types of aberrations in optics: spherical, chromatic, and astronomical Optical Instruments Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions Lens aberrations Our analysis of mirror and lenses assumes that rays make small angles with the principal axis and that the lenses are thin When these approximations do not hold, imperfect images (aberrations) are formed There are three types of aberrations in optics: spherical, chromatic, and astronomical Spherical aberration Spherical aberration is caused by spherical lenses or mirrors Spherical aberration occurs because the focal points of rays far from the principal axis of a spherical lens (or mirror) are different from the focal points of rays passing near the axis Spherical aberration results in a blurry image Optical Instruments Announcements Optical Instruments Review Chromatic Dispersion Aberrations The Camera Final Questions Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions Lens aberrations Our analysis of mirror and lenses assumes that rays make small angles with the principal axis and that the lenses are thin When these approximations do not hold, imperfect images (aberrations) are formed There are two types of aberrations in optics: spherical and chromatic Spherical aberration Spherical aberration is caused by spherical lenses or mirrors Spherical aberration occurs because the focal points of rays far from the principal axis of a spherical lens (or mirror) are different from the focal points of rays passing near the axis Spherical aberration results in a blurry image Chromatic aberration Lenses refract light differently based on their wavelength As white light passes through a lenses, the individual colors (red, orange, yellow, etc.) will not focus on the same point Violet, with a short wavelength bends more than red and focuses closer to the lens than red Optical Instruments Announcements Optical Instruments Review Chromatic Dispersion Aberrations The Camera Final Questions Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions The camera A camera is an optical instrument that consists of a light-tight chamber, a converging lens that produces a real image, and a light-sensitive film on which the image is formed In a digital camera, the film is replaced by a charge-coupled device (CCD) which digitizes that image A camera is focused by varying the distance between the lens and the CCD The shutter, which is positioned behind the lens, is a device that is opened for selected time intervals (exposure times) You can photograph moving objects by using short exposure times You can photograph dark scenes (low light levels) by using long exposure times 1 s, 1 s, 1 s, and 1 s Typical exposure times are 30 60 125 250 Optical Instruments Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions The eye Like a camera, the eye focuses light and produces a sharp image The eye focuses on an object by quickly varying the shape of the pliable lens (accommodation) The near point is the closest distance for which the lens can accommodate to focus light on the retina This distance usually increases with age (at age 20, its about 25 cm) The far point is the greatest distance for which the lens of the relaxed eye can focus light on the retina A person with normal vision can see very distant objects (we approximate this distance as infinite) Optical Instruments Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions Hyperopia (farsightedness) Hyperopia (or farsightedness) is a defect of vision caused by an imperfection in the eye causing difficulty focusing on near objects A farsighted person can usually see faraway objects clearly (but not nearby objects) The near point of a farsighted person is much farther away than normal The refracting power in the cornea and lens of a farsighted person is insufficient to focus the light from nearby objects Farsightedness can be corrected by placing a converging lens in front of the eye Optical Instruments Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions Hyperopia (farsightedness) Hyperopia (or farsightedness) is a defect of vision caused by an imperfection in the eye causing difficulty focusing on near objects A farsighted person can usually see faraway objects clearly (but not nearby objects) The near point of a farsighted person is much farther away than normal The refracting power in the cornea and lens of a farsighted person is insufficient to focus the light from nearby objects Farsightedness can be corrected by placing a converging lens in front of the eye Myopia (nearsightedness) Myopia (or nearsightedness) is a defect of vision caused by an imperfection in the eye causing difficulty focusing on distant objects A nearsighted person can usually see nearby objects clearly (but not faraway objects) The far point of a farsighted person is not infinity Rays from distant objects converge to focus in front of the retina; they then continue past that point, diverging before they final reach the retina nearsightedness can be corrected by placing a diverging lens in front of the eye Optical Instruments Announcements Optical Instruments Review Chromatic Dispersion Aberrations The Camera Final Questions Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions Question The accommodation limits for a nearsighted person’s eyes are 18.0 cm and 80.0 cm. When he wears glasses, he can see faraway objects clearly. At what minimum distance is he able to see objects clearly? (Assume that the glasses are very close to his eyes.) Optical Instruments Announcements Review Chromatic Dispersion Aberrations The Camera Final Questions Question The accommodation limits for a nearsighted person’s eyes are 18.0 cm and 80.0 cm. When he wears glasses, he can see faraway objects clearly. At what minimum distance is he able to see objects clearly? (Assume that the glasses are very close to his eyes.) Answer To correct nearsightedness, the man should place diverging lenses (his glasses) in front of his eyes With his glasses on, when he looks at a faraway object (infinitely far away), we want the virtual image formed by the glasses to be 80.0 cm away (why? ) Using the thin lens equation 1/f = 1/p + 1/q where p = ∞ and q = −80.0 cm, we find that the focal length f of the diverging lens in his glasses is f = −80.0 cm Now that we know the focal length of the lens in his glasses, we can find the minimum distance at which he can see objects clearly When an object is at some minimum distance pmin , we want the virtual image formed by the glasses to be 18.0 cm away Therefore, using the thins lens equation and solving for pmin we find that pmin = = 1 1 − f q −1 = 1 1 − −80.0 cm −18.0 cm −1 23.2 cm Notice that in correcting his nearsighted problem, the glasses also increased his near point Optical Instruments Announcements Review Chromatic Dispersion Aberrations The Camera Reading Assignment Read sections 25.4 - 25.5 Homework Assignment 8 Homework for Chapter 23 at due at the beginning of class today Homework Assignment 9 Homework for Chapter 25 (due at the beginning of class on Wednesday, October 27) Q: 3, 6, 14 P: 16, 24 Optical Instruments Final Questions