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Published byRoy Owen Modified over 9 years ago
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Intensity I (W m-2)m-2)
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Intensity = Power I = P A Area
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Inverse square law I d 2 = A A I d2d2 B B
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Photoelectric effect frequency current fofo
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Energy of photons E = h f h is Planck’s constant
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Intensity of photons I = N h f N is number of photons per second
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Work function Minimum energy to release electron from a surface (E = h fo)fo)
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Kinetic Energy E = h f - h fofo Energy above minimum appears as kinetic
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Emission spectra violet red W2W2 W1W1 W0W0
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Emission spectra W2 W2 – W1 W1 = h f Electron ‘jumps’ from excited level to lower level
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Emission spectra Bright emission lines - more electrons
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Absorption spectra Photon of energy h f W2W2 W1W1
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Absorption spectra W2 W2 = W1 W1 + h f Electron absorbs radiation and ‘jumps’ to excited level
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Spontaneous emission random process
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Stimulated emission Photon (energy h f)f) can cause atom to emit photon (energy h f) in phase and same direction
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Laser Stimulating photon (hf) E1E1 E0E0
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Laser Monochromatic Coherent Intense
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Semiconductors n-type p-type
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n-type Conduction by negative electrons
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p-type Conduction by ‘positive’ holes
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Forward-biased p-type diode conducts n-type electrons
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Reverse-biased p-type diode does not conduct n-type
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Diode Forward-biased diode electron and hole recombine Photon (heat) emitted
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LED Forward-biased diode electron and hole recombine Photon (light) emitted
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photodiode Photovoltaic mode supplies power e.g. solar cell
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photodiode Photoconductive mode (reverse bias) light sensor
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MOSFET drain n-region implant n-channel enhancement MOSFET oxide layer gate source n-channel p-type substrate
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MOSFET Can switch on a load. Apply gate voltage V GS to turn ‘on’ MOSFET
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D load n-channel enhancement MOSFET G S IoIo 0 V + V V GS
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MOSFET Can also be used as an AMPLIFIER
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