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Introduction to Health Physics: Fourth Edition - Ruang Baca FMIPA UB

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where<br />

Impedance<br />

t = time after closing the switch (in seconds),<br />

R = resistance (in ohms),<br />

C = capacitance (in farads),<br />

VC = voltage across capaci<strong>to</strong>r, and<br />

V = battery voltage.<br />

REVIEW OF PHYSICAL PRINCIPLES 41<br />

The product RC is called the time constant of the circuit and represents the time<br />

(in seconds) after closing the switch, until the current decreases <strong>to</strong> 1/e, or 37%<br />

of the initial current, and the voltage increases <strong>to</strong> V0(1 − 1/e), or 67% of its final<br />

voltage. A charged capaci<strong>to</strong>r in a circuit with a series resis<strong>to</strong>r may be considered<br />

as the equivalent of a battery whose voltage, Vi, is the voltage across the capaci<strong>to</strong>r.<br />

When such a circuit is closed, the capaci<strong>to</strong>r will discharge through the resis<strong>to</strong>r and<br />

the capaci<strong>to</strong>r’s voltage, VC , will decrease according <strong>to</strong><br />

Vc = Vie −t/RC , (2.67)<br />

and the charge on each plate of the capaci<strong>to</strong>r is given by<br />

Q = CVC. (2.68)<br />

While electric current in a circuit is transmitted as electrons flow through conducting<br />

wires, electromagnetic waves are transmitted as disturbances in the electromagnetic<br />

fields established in various media, including a vacuum (free space). The electric<br />

and magnetic components of the field may be considered the analogs of voltage and<br />

current in an electrical circuit. The impedance Z of an alternating current is given<br />

by Ohm’s law:<br />

Z = V<br />

, (2.69)<br />

i<br />

where i is the current flow due <strong>to</strong> the voltage V . By analogy, the impedance of a<br />

medium through which an electromagnetic wave is propagated is given by<br />

Z = ε0<br />

, (2.70)<br />

H0<br />

where ε0 and H0 are the electric and magnetic field strengths respectively. Using the<br />

relationship given by Eq. (2.55),<br />

√ √<br />

H0 μ = ε0 ∈,<br />

we can rewrite Eq. (2.70) as<br />

Z =<br />

<br />

μ<br />

. (2.71)<br />

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