Amplifiers classes:
Car Amplifiers are clasified by 5 main classes:
Class A Amplifiers:
Although class A amps provide clear sound, they are considered to be
inefficient because they get heated very fast. Class A amplifiers also
don’t provide enough power for the effort they consume. Class A
amplifiers are ideally used for car tweeters.
Class A/B
Unlike class A amps, class A/B amps are considered to be more efficient but produce more distortion. A class A/B car amplifier
is formed when a class B style output stage is biased so that around
the crossover point both transistors are conducting. This yields more
distortion than either a proper class A or class B amplifier, however
the bias point is much less critical.
Class B amps consist of two transistors, one for each supply rail. In
properly-biased class B, only one conducts at a given time, but there is
always one conducting. Much of the bad name class B has is due to
amplifiers actually being underbiased into class C where there's a
portion of the cycle around the crossover point where neither is
conducting.
Furthermore, Class B proper biasing may be made very difficult to
achieve due to thermal stability issues (especially proper thermal
coupling and tracking between the biasing circuit and the output power
devices).
Class C amplifiers are useless for audio. They are used in RF
applications where the harmonics can be filtered out. Nonetheless, the
so called "Class G" is just the plain combining of a normal Class AB car
amplifier output stage with a Class C "booster" enabled to operate only
if high power peak are required by the load. If properly designed they
performances are equivalent to that obtained by normal class AB
amplifiers.
Class D amplifiers are a rather new phenomenon in the hifi world. They
are extremely efficient (80%) and can give a very good result. They use
pulse width modulation to amplify the signal; this lets them use the
output transistors in switch mode where they're most efficient and
dissipate the least power. Originally only for subwoofers, newer designs
have since surfaced making this technology capable of sounding very
good as a full-range amplifier.
A class D amplifier is one in which the output transistors are operated as switches. When a
transistor is off, the current through it is zero. When it is on, the voltage across it is small, ideally
zero. In each case, the power dissipation is very low. This increases the efficiency, thus requiring
less power from the power supply and smaller heat sinks for the amplifier. These are important
advantages in portable battery-powered equipment. The “D” in class-D is sometimes said to stand
for “digital.” This is not correct because the operation of the class-D amplifier is based on analog
principles. There is no digital coding of the signal. Before the advent of the class-D amplifier, the
standard classes were class-A, class-AB, class-B, and class-C. The “D” is simply the next letter in
the alphabet after “C.” Indeed, the earliest work on class-D amplifiers involved vacuum tubes and
can be traced to the early 1950s.
The high switching frequency used in class-D amplifiers is a potential source of rf interference
with other electronic equipment. The amplifiers must be properly shielded and grounded to prevent
radiation of the switching harmonics. In addition, low-pass filters must be used on all input and
output leads, including the power supply leads.
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