SMT resistors
Surface mounted resistors are printed with numerical values
in a code related to that used on axial resistors. Standard-tolerance
surface-mount technology (SMT) resistors are marked with a three-digit code, in
which the first two digits are the first twosignificant digits of the value and
the third digit is the power of ten (the number of zeroes). For example:
334 = 33 × 104
ohms = 330 kilohms
222 = 22 × 102
ohms = 2.2 kilohms
473 = 47 × 103
ohms = 47 kilohms
105 = 10 × 105
ohms = 1 megohm
Resistances less than 100 ohms are written: 100, 220, 470.
The final zero represents ten to the power zero, which is 1. For example:
100 = 10 × 100
ohm = 10 ohms
220 = 22 × 100
ohm = 22 ohms
Sometimes these values are marked as 10 or 22 to prevent a
mistake.
Resistances less than 10 ohms have 'R' to indicate the
position of the decimal point (radix point). For example:
4R7 = 4.7 ohms
R300 = 0.30 ohms
0R22 = 0.22 ohms
0R01 = 0.01 ohms
Precision resistors are marked with a four-digit code, in
which the first three digits are the significant figures and the fourth is the
power of ten. For example:
1001 = 100 × 101
ohms = 1.00 kilohm
4992 = 499 × 102
ohms = 49.9 kilohm
1000 = 100 × 100
ohm = 100 ohms
000 and 0000 sometimes appear as values on surface-mount
zero-ohm links, since these have (approximately) zero resistance.
More recent surface-mount resistors are too small,
physically, to permit practical markings to be applied.
Industrial type designation
Format: [two letters]<space>[resistance value (three
digit)]<nospace>[tolerance code(numerical – one digit)] [22]
Power Rating at 70 °C
Type No. Power
rating
(watts) MIL-R-11
Style MIL-R-39008
Style
BB 1/8 RC05 RCR05
CB 1/4 RC07 RCR07
EB 1/2 RC20 RCR20
GB 1 RC32 RCR32
HB 2 RC42 RCR42
GM 3 - -
HM 4 - -
Tolerance Code
Industrial type designation Tolerance MIL Designation
5 ±5% J
2 ±20% M
1 ±10% K
- ±2% G
- ±1% F
- ±0.5% D
- ±0.25% C
- ±0.1% B
Electrical and thermal noise
Main article: Noise (electronics)
In amplifying faint signals, it is often necessary to
minimize electronic noise, particularly in the first stage of amplification. As
a dissipative element, even an ideal resistor will naturally produce a randomly
fluctuating voltage or "noise" across its terminals. This
Johnson–Nyquist noise is a fundamental noise source which depends only upon the
temperature and resistance of the resistor, and is predicted by the
fluctuation–dissipation theorem. Using a larger value of resistance produces a
larger voltage noise, whereas with a smaller value of resistance there will be more
current noise, at a given temperature.
The thermal noise of a practical resistor may also be larger
than the theoretical prediction and that increase is typically
frequency-dependent. Excess noise of a practical resistor is observed only when
current flows through it. This is specified in unit of µV/V/decade – µV of
noise per volt applied across the resistor per decade of frequency. The
µV/V/decade value is frequently given in dB so that a resistor with a noise
index of 0 dB will exhibit 1 µV (rms) of excess noise for each volt across the
resistor in each frequency decade. Excess noise is thus an example of 1/f
noise. Thick-film and carbon composition resistors generate more excess noise
than other types at low frequencies. Wire-wound and thin-film resistors are
often used for their better noise characteristics. Carbon composition resistors
can exhibit a noise index of 0 dB while bulk metal foil resistors may have a
noise index of -40 dB, usually making the excess noise of metal foil resistors
insignificant.[23] Thin film surface mount resistors typically have lower noise
and better thermal stability than thick film surface mount resistors. Excess
noise is also size-dependent: in general excess noise is reduced as the
physical size of a resistor is increased (or multiple resistors are used in
parallel), as the independently fluctuating resistances of smaller components
will tend to average out.
While not an example of "noise" per se, a resistor
may act as a thermocouple, producing a small DC voltage differential across it
due to the thermoelectric effect if its ends are at different temperatures.
This induced DC voltage can degrade the precision of instrumentation amplifiers
in particular. Such voltages appear in the junctions of the resistor leads with
the circuit board and with the resistor body. Common metal film resistors show
such an effect at a magnitude of about 20 µV/°C. Some carbon composition
resistors can exhibit thermoelectric offsets as high as 400 µV/°C, whereas
specially constructed resistors can reduce this number to 0.05 µV/°C. In
applications where the thermoelectric effect may become important, care has to
be taken to mount the resistors horizontally to avoid temperature gradients and
to mind the air flow over the board.[24]
Failure modes
The failure rate of resistors in a properly designed circuit
is low compared to other electronic components such as semiconductors and
electrolytic capacitors. Damage to resistors most often occurs due to
overheating when the average power delivered to it (as computed above) greatly
exceeds its ability to dissipate heat (specified by the resistor's power
rating). This may be due to a fault external to the circuit, but is frequently
caused by the failure of another component (such as a transistor that shorts out)
in the circuit connected to the resistor. Operating a resistor too close to its
power rating can limit the resistor's lifespan or cause a significant change in
its resistance. A safe design generally uses overrated resistors in power
applications to avoid this danger.
Low-power thin-film resistors can be damaged by long-term
high-voltage stress, even below maximum specified voltage and below maximum
power rating. This is often the case for the startup resistors feeding the SMPS
integrated circuit.[citation needed]
When overheated, carbon-film resistors may decrease or
increase in resistance.[25] Carbon film and composition resistors can fail
(open circuit) if running close to their maximum dissipation. This is also
possible but less likely with metal film and wirewound resistors.
There can also be failure of resistors due to mechanical
stress and adverse environmental factors including humidity. If not enclosed,
wirewound resistors can corrode.
Surface mount resistors have been known to fail due to the ingress
of sulfur into the internal makeup of the resistor. This sulfur chemically
reacts with the silver layer to produce non-conductive silver sulfide. The
resistor's impedance goes to infinity. Sulfur resistant and anti-corrosive
resistors are sold into automotive, industrial, and military applications. ASTM
B809 is an industry standard that tests a part's susceptibility to sulfur.
An alternative failure mode can be encountered where large
value resistors are used (hundreds of kilohms and higher). Resistors are not
only specified with a maximum power dissipation, but also for a maximum voltage
drop. Exceeding this voltage will cause the resistor to degrade slowly reducing
in resistance. The voltage dropped across large value resistors can be exceeded
before the power dissipation reaches its limiting value. Since the maximum
voltage specified for commonly encountered resistors is a few hundred volts,
this is a problem only in applications where these voltages are encountered.
Variable resistors can also degrade in a different manner,
typically involving poor contact between the wiper and the body of the
resistance. This may be due to dirt or corrosion and is typically perceived as
"crackling" as the contact resistance fluctuates; this is especially
noticed as the device is adjusted. This is similar to crackling caused by poor
contact in switches, and like switches, potentiometers are to some extent
self-cleaning: running the wiper across the resistance may improve the contact.
Potentiometers which are seldom adjusted, especially in dirty or harsh
environments, are most likely to develop this problem. When self-cleaning of
the contact is insufficient, improvement can usually be obtained through the
use of contact cleaner (also known as "tuner cleaner") spray. The
crackling noise associated with turning the shaft of a dirty potentiometer in
an audio circuit (such as the volume control) is greatly accentuated when an
undesired DC voltage is present, often indicating the failure of a DC blocking
capacitor in the circuit.

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