Physics 272 May 1 Spring 2014 http://www.phys.hawaii.edu/~philipvd/pvd_14_spring_272_uhm.html Prof. Philip von Doetinchem philipvd@hawaii.edu Phys272 - Spring 14 - von Doetinchem - 441 Summary ● Lens in air: Phys272 - Spring 14 - von Doetinchem - 442 ● ● ● ● Converging lens in front of light detector (film or chip) Lens forms an inverted image on the light detector Magnification for object at 5m Cameras: magnification Focal length [mm] Good lenses correct for paraxial approximation and dispersion Longer focal length → higher absolute magnification factor (still inverted) → image size on light detector increases Phys272 - Spring 14 - von Doetinchem - 444 Cameras: intensity ● ● ● Light intensity on the detector depends on field of view and the aperture opening Field of view scales roughly as 1/f2 Wide aperture allows more light to enter ● Adjusting is a typical function of cameras ● Eventually also the exposure time is adjusted Phys272 - Spring 14 - von Doetinchem - 445 Cameras: zoom ● ● Combination of movable converging and diverging lens make it possible to change the focal length Real zoom lenses are more complicated than that and use more than 10 lenses to correct for various aberrations Phys272 - Spring 14 - von Doetinchem - 446 Cameras: depth of focus small aperture ● large aperture Introducing an adjustable lens aperture helps increasing the depth of focus: – light rays coming from an object further away from a lens are less refracted than light rays from a closer object – Extended objects along the optic axis are in focus for a narrow (wide) region for large (small) apertures Phys272 - Spring 14 - von Doetinchem - 447 Cameras: depth of focus large aperture short depth of field object ● ● circle of confusion Out of focus: image becomes blurry The circle of confusion on the image side is the size when the objects starts to appear blurry (typical: 1 pixel of the sensor) long depth of field object small aperture circle of confusion http://graphics.stanford.edu/courses/cs178/applets/dof.html Phys272 - Spring 14 - von Doetinchem - 448 Cameras: autofocus ● Different autofocus techniques are available – Contrast detection – Assist lamp – Phase detection: ● ● ● ● Splits incoming light Analyzes different parts projected on different sensors in the same plane Chip compares intensity patterns Sensor plane is in focus when patterns are the same Source: http://en.wikipedia.org/wiki/Autofocus Phys272 - Spring 14 - von Doetinchem - 449 The Eye ● ● ● ● ● ● The eye works very much like a camera Crystalline index of refraction has index of refraction of ~1.437 Eye is filled with substance having similar optical properties as water (n=1.336) Muscles change the focal length of the eye by squeezing the lens → radius gets smaller Relaxed eye focuses on infinity Image is projected in retina → connects over optic nerve to brain Phys272 - Spring 14 - von Doetinchem - 450 Defects of vision Phys272 - Spring 14 - von Doetinchem - 451 Correcting for farsightedness ● ● How to correct the near point of a farsighted eye from 100cm to 25cm (standard value) using a contact lens? → form a virtual image of the object at 100cm: Prescriptions typically use the inverse of the focal length → a converging lens of +3.0 diopters would correct this eye Phys272 - Spring 14 - von Doetinchem - 452 Correcting for nearsightedness Phys272 - Spring 14 - von Doetinchem - 453 The magnifier ● ● ● Size of an image depends on size on retina Moving object closer than near point does not help → eye cannot focus Converging lens: – Place object at focal point – Virtual image at infinity has a much larger angular size – Lateral magnification for virtual image at infinity is not a useful quantity Phys272 - Spring 14 - von Doetinchem - 455 The microscope ● ● ● ● Image of one lens can be used as an object for the second lens → greater magnification can be reached without making the lenses too big Objects are placed closely to the focal point Short focal length of the objective and eyepiece lens cause a greater magnification Overall magnification is composed of lateral and angular magnification Phys272 - Spring 14 - von Doetinchem - 456 Telescopes ● Telescopes are used to magnify objects at large distances ● Objective lens forms a real, reduced image of the object on the sky ● Objects are very far → image nearly perfectly at focal point ● first image serves as object for the eyepiece lens → if at focal point of eyepiece → observer can see the magnified virtual object at infinity Phys272 - Spring 14 - von Doetinchem - 457 Telescopes: Hubble in space ● ● ● Large magnification requires a large focal length f1 Large focal length → lower intensity → large collecting area needed Modern telescopes are reflecting telescopes Phys272 - Spring 14 - von Doetinchem - 458 Telescopes: Hubble in space Hubble Ultra deep field: At this time the universe was only 800 Million years old ● ● ● Large magnification requires a large focal length f1 Large focal length → lower intensity → large collecting area needed Modern telescopes are reflecting telescopes Phys272 - Spring 14 - von Doetinchem - 459 Telescopes: Keck on Mauna Kea Phys272 - Spring 14 - von Doetinchem - 460 Review ● ● ● ● Reflection and refraction at a plane surface: – Important difference between virtual and real image – Only for a real image the light rays actually cross the image point Magnifcation: is defined in lateral and angular direction Focal point describes the point where parallel light rays converge in a concave mirror (light rays emerging from the focal point of a convex mirror are parallel after reflection) Thin lens find wide applications and consist of the combination of two spherical refracting surfaces Phys272 - Spring 14 - von Doetinchem - 461 Physics 272 Review of second part Spring 2014 http://www.phys.hawaii.edu/~philipvd/pvd_14_spring_272_uhm.html Prof. Philip von Doetinchem philipvd@hawaii.edu Phys272 - Spring 14 - von Doetinchem - 462 Final May 15 ● Thursday 5/15: 9:45am-11:45am, WAT112 ● Will focus on chapters 28-34 of the textbook – Is the exam cumulative? ● ● ● ● No supplemental materials allowed: – ● The final will cover all chapters 21-34 Bu the focus is on chapters 28-34 (understanding of chapters 21-27 is essential) For instance: understanding of electric fields (ch21) is absolutely essential for understanding electromagnetic waves (ch32) Just bring paper and calculator Study suggestions: – Make sure to understand old homework: mastering physics and hand-in – The final exam will again have conceptual questions that do not require long calculations, but qualitative understanding: ● Work with “test your understanding” questions and discussion questions from the book Phys272 - Spring 14 - von Doetinchem - 463 Maxwell's equations of electromagnetism ● ● Gauss's law for electric fields (surface integral) – Electric field is related to total charge in an enclosed surface – Electric charges are sources of magnetic fields Gauss's law for magnetism (surface integral) – No magnetic monopoles exist → magnetic flux through closed surface is always zero Phys272 - Spring 14 - von Doetinchem - 464 Maxwell's equations of electromagnetism ● Ampere's law (line integral) – ● Conducting and displacement current act as sources of magnetic fields Faraday's law (line integral) – A changing magnetic field or magnetic flux induces an electric field Phys272 - Spring 14 - von Doetinchem - 465 Moving charges as sources of magnetic fields ● Magnetic field of a moving charge: ● Magnetic field of a conductor (law of Biot-Savart) ● Magnetic field of a long, straight, current-carrying conductor Phys272 - Spring 14 - von Doetinchem - 466 Forces between two moving protons ● ● ● Two protons moving in the same direction. Magnetic force on the upper proton from the magnetic field of the lower proton: attractive Magnetic force on the lower proton from the magnetic field of the upper proton: attractive Phys272 - Spring 14 - von Doetinchem - 467 Magnetic field on the axis of a coil ● Magnetic field on axis of the loop along the x axis at a certain distance x using Biot-Savart Phys272 - Spring 14 - von Doetinchem - 468 Magnetic field on the axis of a coil ● ● ● ● Stack a number of N loops on top of each other Assume that each loop is planar and that the loops are very closely spaced Also assume that the distance from the center of each loop is the same to the point along the coil axis under study Superposition principle at work: Phys272 - Spring 14 - von Doetinchem - 469