By Prof. Dr. Ralf Kories, Prof. Dr. Heinz Schmidt-Walter (auth.)
ISBN-10: 354043965X
ISBN-13: 9783540439653
ISBN-10: 3642556299
ISBN-13: 9783642556296
This extraordinary resource of quick available and punctiliously chosen info comprises: *Fundamentals of DC and AC *Electric and magnetic Fields*Networks *Signals & platforms *Digital & Analog Electronics and *Power offers. The Pocket Reference comprises the fundamentals of electric engineering and electronics in one, logically-organized, compact quantity. Key good points to consider:
Each bankruptcy is a self-contained unit, incorporating vital phrases and definitions, symbols and devices, formulation, principles and theorems, plus many examples and functions.
More than 500 diagrams and figures plus 60 tables and frames make crucial details speedy and simple to discover.
Appendices record worthwhile mathematical kin in a notation geared to electric engineering, in addition to comprise dozens of important tables.
No different reference resource concentrates loads sensible basic into one of these compact and beneficial package deal for execs and scholars.
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Extra resources for Electrical Engineering: A Pocket Reference
Example text
42. 65) To determine the coefficients K1 and K2 in the general solution two specific values are required for vout (t). 66) t=0 The solutions of the inhomogeneous differential equation are: 1. Overdamped case D > 1: vout (t) = vout (t)homogeneous + vout, special = K1 eλ1 t + K2 eλ2 t + vS , λ1,2 = −Dω0 ± ω0 D 2 − 1 K1 and K2 can be determined from the initial conditions: first the derivative dvout (t)/ dt is calculated, then t = 0 is inserted in vout (t) and in dvout (t)/ dt. This results in two equations for K1 and K2 .
The voltage V in this model is given by the difference between two potentials (Fig. 3a). 6) Areas of equal potential are called equipotential surfaces. The electric field strength and the electric flux density vectors are perpendicular to these surfaces. An infinitesimal surface element d A of the equipotential surface is a vector that is perpendicular to the surface. The direction of the vector d A is the same as the direction of the electric field strength (Fig. 3b). 42 2 Electric Fields Fig. 3. 4 Electrostatic Induction Electrostatic induction is the shift of the mobile charges in a conductor that has been placed in an electric field.
27. 45) R23 = R2 + R3 + In a delta–star transformation: R1 = † In American literature the term Wye may be used instead of star. 1 Voltage Divider If the same current flows through two resistors (Fig. 28), then: V1 V2 V I= = = R1 R2 R1 + R2 Fig. 28. 46) • In a series combination the individual voltages are proportional to the resistances they appear across. This also holds for series combinations of more than two resistors. 2 Current Divider If the same voltage is applied across two conductances or resistances (Fig.
Electrical Engineering: A Pocket Reference by Prof. Dr. Ralf Kories, Prof. Dr. Heinz Schmidt-Walter (auth.)
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