. The Bell System technical journal . he general shapeshown in Fig. 2. Thus the amphfication factor, {vje), varies from a largevalue for small inputs to unity for the largest amplitude (F) to be ac-commodated, so that the distribution of pulse sizes may be modifiedwithout changing the total voltage range. Fig. 2 also illustrates how uni-form quantization of the compressor output produces a tapered arrayof input steps similar to those already considered in connection withFig. 1(b). A complementary device, the expandor, employs a characteristic in-verse to that of the compressor to restore the p

GLIX-115-2CNCJT2

. The Bell System technical journal . he general shapeshown in Fig. 2. Thus the amphfication factor, {vje), varies from a largevalue for small inputs to unity for the largest amplitude (F) to be ac-commodated, so that the distribution of pulse sizes may be modifiedwithout changing the total voltage range. Fig. 2 also illustrates how uni-form quantization of the compressor output produces a tapered arrayof input steps similar to those already considered in connection withFig. 1(b). A complementary device, the expandor, employs a characteristic in-verse to that of the compressor to restore the p
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. The Bell System technical journal . he general shapeshown in Fig. 2. Thus the amphfication factor, {vje), varies from a largevalue for small inputs to unity for the largest amplitude (F) to be ac-commodated, so that the distribution of pulse sizes may be modifiedwithout changing the total voltage range. Fig. 2 also illustrates how uni-form quantization of the compressor output produces a tapered arrayof input steps similar to those already considered in connection withFig. 1(b). A complementary device, the expandor, employs a characteristic in-verse to that of the compressor to restore the p

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