Ohm’s law is
stated as V=IR, and it is fundamental to all electronics. Ohm’s law can be
applied to a single component, to any group of components, or to a complete
circuit. When the current flowing through any portion of a circuit is known,
the voltage dropped across that portion of the circuit is obtained by
multiplying the current times the resistance (Equation 2–1).
V = IR
In Figure 2–1,
Ohm’s law is applied to the total circuit. The current, (I) flows through the
total resistance (R), and the voltage (V) is dropped across R.
Figure 2–1. Ohm’s Law Applied to the Total
Circuit
In Figure 2–2,
Ohm’s law is applied to a single component. The current (IR) flows through the resistor
(R) and the voltage (VR) is dropped across R. Notice, the same formula is used
to calculate the voltage drop across R even though it is only a part of the
circuit.
Figure 2–2. Ohm’s Law Applied to a Component
Kirchoff’s
voltage law states that the sum of the voltage drops in a series circuit equals
the sum of the voltage sources. Otherwise, the source (or sources) voltage must
be dropped across the passive components. When taking sums keep in mind that
the sum is an algebraic quantity. Kirchoff’s voltage law is illustrated in
Figure 2–3 and Equations 2–2 and 2–3.
Figure 2–3. Kirchoff’s Voltage Law
Kirchoff’s
current law states: the sum of the currents entering a junction equals the sum
of the currents leaving a junction. It makes no difference if a current flows
from a current source, through a component, or through a wire, because all
currents are treated identically. Kirchoff’s current law is illustrated in
Figure 2–4 and Equations 2–4 and 2–5.
Figure 2–4. Kirchoff’s Current Law
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