1 / 24

Lecture 22: July 15 th 2009

Lecture 22: July 15 th 2009. Physics for Scientists and Engineers II. Momentum and Radiation Pressure. + + + +. Antennas. The Half Wave Antenna. Source of alternating voltage having frequency f = c / l. Conducting rods. - - - -. + + + +. - - - -.

saskia
Download Presentation

Lecture 22: July 15 th 2009

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Lecture 22: July 15th 2009 Physics for Scientists and Engineers II Physics for Scientists and Engineers II , Summer Semester 2009

  2. Momentum and Radiation Pressure Physics for Scientists and Engineers II , Summer Semester 2009

  3. + + + + Antennas The Half Wave Antenna Source of alternating voltage having frequency f = c / l Conducting rods - - - - Physics for Scientists and Engineers II , Summer Semester 2009

  4. + + + + - - - - Driving the resonance frequency of the antenna ----??? Snapshot in time: Separation of charges creates an electric field like that of a dipole:  Given the name “Dipole antenna” Physics for Scientists and Engineers II , Summer Semester 2009

  5. + + + + - - - - Driving the resonance frequency of the antenna Snapshot in time: Physics for Scientists and Engineers II , Summer Semester 2009

  6. Voltage and Current Distribution V I V I V I V I Physics for Scientists and Engineers II , Summer Semester 2009

  7. Driving the resonance frequency of the antenna V I Physics for Scientists and Engineers II , Summer Semester 2009

  8. + + + + + + + + - - - - The “near field” (dipole field) behavior - - - - Physics for Scientists and Engineers II , Summer Semester 2009

  9. The “far field” behavior Physics for Scientists and Engineers II , Summer Semester 2009

  10. Angular dependence of radiation intensity Physics for Scientists and Engineers II , Summer Semester 2009

  11. Angular dependence of radiation intensity Sender Sender Sender Physics for Scientists and Engineers II , Summer Semester 2009

  12. Electromagnetic Spectrum Physics for Scientists and Engineers II , Summer Semester 2009

  13. The Nature of Light Newton: Light = Stream of Particles (can explain reflection and refraction) 1678 Christian Huygens : Showed that a wave model of light can also explain reflection and refraction. 1801 Thomas Young: Experimental demonstration of the wave nature of light (Double slit experiment  “Interference” effects) Maxwell: Light = high frequency electromagnetic wave Hertz: Confirms existence of electromagnetic waves …..but also discovers the photoelectric effect (contradicts the wave model, which predicts: more light intensity = more energy transferred to electrons) Einstein 1905: Proposes that energy of light wave is present in particles called photons. E=hf is the energy of a photon (explains photoelectric effect). Physics for Scientists and Engineers II , Summer Semester 2009

  14. Measuring the speed of light Galileo: Using lanterns between mountains didn’t work. The light is too fast. 1675: Ole Roemer found that the period of revolution of the moon Io around Jupiter depends on whether the earth is receding from or moving towards Jupiter (longer period when earth is receding). From these data Huygens calculated c > 2.3 x 108 m/s 1849: Fizeau’s method (toothed wheel): c = 3.1 x 108 m/s Currently accepted value: c = 2.997 9 x 108 m/s Physics for Scientists and Engineers II , Summer Semester 2009

  15. Eclipse Time Delay of Io in the shadow of Jupiter Roemer’s method Jupiter Io being eclipsed by Jupiter Sun In this position, the time of the eclipse is delayed by many minutes compared to the opposite position of the earth. Physics for Scientists and Engineers II , Summer Semester 2009

  16. Ray Approximation in Geometric Optics • Geometrical Optics • The study of the propagation of light under these assumptions: • In a uniform medium light travels in a straight line. • Light changes direction in a medium with non-uniform optical properties, • or at the interface between two media. The “Ray approximation”: Wave moving through a medium travels in a straight line in the direction of it’s rays. Rays Wave fronts Physics for Scientists and Engineers II , Summer Semester 2009

  17. Ray Approximation in Geometric Optics Encountering barriers (like an opening in a wall): The ray approximation is valid if l << d, where d is the size of the opening. Wave continues in a straight line Diffraction occurs Opening acts like a point source of a wave. Physics for Scientists and Engineers II , Summer Semester 2009

  18. Reflection of Light/Wave Incident Ray Reflected Ray Normal Physics for Scientists and Engineers II , Summer Semester 2009

  19. Specular and Diffuse Reflection Specular reflection “Smooth surface” Diffuse reflection Physics for Scientists and Engineers II , Summer Semester 2009

  20. The Wave under Refraction Reflected Ray Incident Ray Normal Air Glass Refracted Ray Angle of Refraction Physics for Scientists and Engineers II , Summer Semester 2009

  21. The Wave under Refraction Incident Ray, Reflected Ray, and Refracted ray are all in one plane. Physics for Scientists and Engineers II , Summer Semester 2009

  22. The Wave under Refraction Reflected Ray Incident Ray Normal Glass Air Refracted Ray Angle of Refraction Physics for Scientists and Engineers II , Summer Semester 2009

  23. Index of Refraction – not yet covered in class but needed for HW 16 Wavelength in vacuum Wavelength in medium Physics for Scientists and Engineers II , Summer Semester 2009

  24. Snell’s Law of Refraction – not yet covered in class but needed for HW 16. Snell’s Law of Refraction Physics for Scientists and Engineers II , Summer Semester 2009

More Related