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Now the output voltage has its negative peaks clamped to zero, since the entire waveform is shifted upward by Vpeak volts Note that in either case, the diode clamp has the effect of introducing a DC component in a waveform that does not originally have one It is also possible to shift the input waveform by a voltage different from Vpeak by connecting a battery, VDC , in series with the diode, provided that VDC < Vpeak (833)

The McGraw Hill Companies, 2001

Known Quantities: vS (t) = 5 cos( t) Find: The value of VDC in the circuit in the lower half of Figure 869 Assumptions: Use the ideal diode model Analysis: With reference to the circuit in the lower half of Figure 869, we observe that

Fig 343: Triangle used to calculate ;

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once the capacitor has charged to Vpeak VDC , the output voltage will be given by: vout = vS Vpeak + VDC Since VDC must be smaller than Vpeak (otherwise the diode would never conduct!), this circuit would never permit raising the DC level of vout To resolve this problem, we must invert both the diode and the battery, as shown in the circuit of Figure 871 Now the output voltage is given by: vout = vS + Vpeak VDC To have a DC level of 3 V, we choose VDC = 2 V The resulting waveforms are shown in Figure 872

They then made synthetic messenger RNAs by using mixtures of the various diphosphate nucleotides in known proportions. Table 11.3 gives an example. From their experiments, it was possible to determine the bases used in many of the code words, but not their speci c order. For example, cysteine, leucine, and valine are all coded by two Us and a G, but the experiment could not sort out the order of these bases (5 -UUG-3 , 5 -UGU-3 , or 5 -GUU-3 ) for any one of them. Determining the order required an extra step in sophistication that is, being able to synthesize known trinucleotides.

10 5 3 0

5 10 0 01 02 03 04 05 06 t (s) 07 08 09 1

Severo Ochoa (1905 1993).

Photodiodes Another property of semiconductor materials that nds common application in measurement systems is their response to light energy In appropriately fabricated diodes, called photodiodes, when light reaches the depletion region of a pn junction, photons cause hole-electron pairs to be generated by a process called photo-ionization This effect can be achieved by using a surface material that is transparent to light As a consequence, the reverse saturation current depends on the light intensity (ie, on the number of incident photons), in addition to the other factors mentioned earlier, in Section 82 In a photodiode, the reverse current is given by (I0 + Ip ), where Ip is the additional current generated by photoionization The result is depicted in the family of curves of Figure 873, where the diode characteristic is shifted downward by an amount related to the additional current generated by photo-ionization Figure 873 depicts the appearance of the i-v characteristic of a photodiode for various values of Ip , where the i-v curve is shifted to lower values for progressively larger values of Ip The circuit symbol is depicted in Figure 874

(43)

(Courtesy of Dr. Severo Ochoa.)

002 0015 001 Amps 0005 0 0005 001 1 0 05 1 Volts L1 : diode operation ; L2 : solar cell ; L3 : photosensor 05 + v i Light L2 L3 L1

Also displayed in Figure 873 are three load lines, which depict the three modes of operation of a photodiode Curve L1 represents normal diode operation, under forward bias Note that the operating point of the device is in the positive i, positive v ( rst) quadrant of the i-v plane; thus, the diode dissipates positive

Marshall W. Nirenberg.)

8

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