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`PowerElectronics Ex.1017
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`APPLEINC./ Page 1 of 4
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`Ex.1017
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`Fundamentals of
`PowerElectronics
`
`Robert W. Erickson
`University of Colorado
`Boulder, CO
`
`Thiatwei
`
`TraA"Z£ERLESE
`
`CHAPMAN & HALL
`
`KTP International Thomson Publishing
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`Ex.1017
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`Cover desgrr Carolyn Walsitis
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`Copyright © 1997 by Chapman & Mall
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`Printed in the United States of America
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`123456789 10 XXX 01 © 9 98 97
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`Library of Congress Catalogingin-Publication Data
`
`Erickson, Robert W. (Robert Warren),
`eS ae aeee
`pincludesfBibbographical references and index.
`
`BBN 0412065410 (alk paper)
`LPower electronics.
`L Title
`TRKTSSL I ETS)
`«1997
`621317-<ic)
`
`96-38347 a
`
`British Library Cataloguing in Publication Data available
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`sechnically accurate and authoritative
`"Fudamentals of Power Electronics’ = imended 10
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`made every reasonable
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`x.1017
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`Ex.1017
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`iM
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`The Discowinwows Conduction Mode
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`Thus, we have two unknowns, V and D,, and we have two equations. The first equation, Eq. (3.19),
`was obtained by inductor volt-second balance. while the second equation, Eq. (5.27), was obtained
`using capacitor charge balance. Elimination of D, from the two equations, and solution for the voltage
`conversion ratio M(D,, K)= V/V,, yields
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`TF eiecniial
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`V,
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`a4 aftee: aK
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`!
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`(5.28)
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`where
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`K=2L/RT,
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`This is the solution of the buck converter operating in discontinuous conduction mode.
`The complete buck converter characteristics, including both continuous and discontinuous conduc-
`tion modes, are therefore
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`D
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`for K > K..
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`M*
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`i *y 1+
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`\
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`(5.29)
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`where the transistor duty cycle D is identical to the subinterval | duty cycle D, of the above derivation.
`These characteristics are plotted in Fig. 5.11, for several values of X, It can be seen that the effect
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`06
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`0.2 0.0
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`O04
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`0.0
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`0.2 :
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`O.4
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`0.6
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`0.8
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`1.0
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`D
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`Fig. $.11 Voltage conversion ratio M(D. XK). buck converter,
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`Ex.1017
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`Ex.1017
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