By Y.T. Lo

ISBN-10: 0442015925

ISBN-13: 9780442015923

ISBN-10: 0442015941

ISBN-13: 9780442015947

ISBN-10: 0442015968

ISBN-13: 9780442015961

Quantity 1: Antenna basics and Mathematical concepts opens with a dialogue of the basics and mathematical strategies for any form of paintings with antennas, together with uncomplicated rules, theorems, and formulation, and strategies. DLC: Antennas (Electronics)

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**Extra info for Antenna Handbook - Applications**

**Sample text**

5(b) shows the symbol and time variation for a sinusoidal voltage source with v = Vm cos ωt. The positive sign on the source symbol indicates instantaneous polarity of the terminal at the higher potential whenever cos ωt is positive. A sinusoidal source is generally termed an ac source because such a voltage source tends to produce an alternating current. The concept of an ideal current source, although less familiar but useful as we shall see later, is deﬁned as one whose current i is a speciﬁed function of time, regardless of the voltage across its terminals.

3) T1 + T where ρT 2 and ρT 1 are resistivities at temperatures T2 and T1 , respectively, and T is a temperature constant that depends on the conductor material. All temperatures are in degrees Celsius. , steel conductors used for shield wires). Practical resistors are manufactured in standard values, various resistance tolerances, several power ratings (as will be explained shortly), and in a number of different forms of construction. The three basic construction techniques are composition type, which uses carbon or graphite and is molded into a cylindrical shape, wire-wound type, in which a length of enamel-coated wire is wrapped around an insulating cylinder, and metal-ﬁlm type, in which a thin layer of metal is vacuum deposited.

These are voltage sources. An ideal voltage source is one whose terminal voltage v is a speciﬁed function of time, regardless of the current i through the source. 5(a). It is known as a dc source, because i = I is a direct current. 5(b) shows the symbol and time variation for a sinusoidal voltage source with v = Vm cos ωt. The positive sign on the source symbol indicates instantaneous polarity of the terminal at the higher potential whenever cos ωt is positive. A sinusoidal source is generally termed an ac source because such a voltage source tends to produce an alternating current.

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