noise sources and effects

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    Why study noise?

    WYPR-FM 88.1 MHz

    Transmitted power 15,500 W

    Received power

    ~0.00000000000001 W

    ~19 orders ofmagnitude

    Noisesources and effects

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    Why study noise?

    Noise is one of the principle limiting factors inthe performance of communication systems.

    Electrical noise is any undesired voltages or

    currents that end up appearing at the receiveroutput. An example is static that is commonly

    encountered on broadcast

    AM radio.

    In a practical system noise is always present.

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    Types of noise

    Noise is divided into two broad categories:

    External noise is noise introduced in the

    transmission channel.

    Internal noise is noise introduced inside the

    receiver itself.

    Information or

    intelligence

    (audio, video,

    data, etc.)

    Recovered

    information

    orIntelligence

    Free space (radio), wire,

    fiber-optic cable, etc.

    Transmitter(TX)

    Communicationschannel or medium

    Receiver(RX)

    External

    noise

    Internal

    noise

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    External noise

    Industrial noise is caused by human made

    electrical sources (motors,

    generators, ignition)

    Atmospheric noise is due to naturally

    occurring disturbances in earthsatmosphere such as lightening.

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    External noise

    Extraterrestrial noise (solar noise)is electrical

    noise due to solar and cosmic activity.

    Dominates at higher frequencies and can be aserious problem in satellite communications.

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    Internal noise

    Internal noise is noise introduced inside the

    receiver.

    Three types of internal noise we will consider Thermal noise

    Semiconductor noise

    Intermodulation distortion

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    Thermal noise

    Thermal noise is caused by random motion offree electrons and vibrating ions in a

    conductor due to heat.

    Noise Power in watts is directly proportionalto Bandwidth in Hz, and the temperature in

    degrees Kelvin.Thermal noise voltage as a function of timeRandom electron motion due to heat

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    Thermal noise

    Thermal noise is also termed white noise or

    Gaussian noise.

    Just as white light contains all frequencies, white

    noise contains an equal weighting of allfrequencies.

    Frequency (Hz)

    Frequency spectrum of thermal noise

    Thermal noise voltage as a function of time

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    N KTB!N= noise power (watts)

    B =bandwidth (hertz)

    K= Boltzmanns proportionality constant

    (1.38 10-23 Joules per kelvin)

    T= absolute temperature (kelvin)

    10 log 10 log 10 log0.001 0.001

    dBm

    KTB KT N B! !

    @ 290k 174 dBm 10 log

    dBmN B!

    Thermal noise

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    2

    224

    4

    N

    N

    N

    V

    V N KTB V RKTB

    R R

    ! ! ! p !

    2V

    P VIR

    ! !

    V IR!

    The noise voltage produced by a resistorR over a bandwidthB can be calculated

    Thermal noise voltage

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    Thermal noise voltage

    Thermal noise design considerations; Since

    thermal noise is proportional to resistance,temperature, and bandwidth, receiver designsthat reduce these values will have superiorperformance.

    23

    4

    where rms noise voltage

    oltzman's constant (1.38 10 J/K)

    temperature, K ( C 27

    3)bandwidth, Hz

    resistance,

    n

    n

    v kTBR

    v

    k

    T

    B

    R

    !

    !

    ! v

    ! r !

    ! ;

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    Example Problem 1

    The bandwidth of a receiver with a 75-; input resistance is 6

    MHz. If the temperature is 29C, what is the input thermal noise

    voltage?

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    Semiconductor noise

    The other major category of internal noise

    originates from semiconductor devices such as

    diodes and transistors.

    Semiconductor noise is comprised of

    Shot noise

    Transit-time noise

    Flicker noise

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    Shot noise

    Shot noise, the largest contributor to transistor

    noise, is due to the random paths of the

    current carriers flowing in semiconductors.

    circuit symbol for a diode

    diode

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    Transit-time noise

    Transit-time noise occurs at high frequencies

    when transit time of charge carriers crossing

    the semiconductors junction approaches the

    signals period.

    This type noise increases rapidly when

    operating above the devices high-frequency

    cutoff. Time required to crosspn-junction close to period (T)

    of the signal.

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    Flicker noise

    Flicker noise results from minute variations in

    resistance in semiconductor material.

    Flicker noise is inversely proportional to

    frequency and sometimes referred to as 1/fnoise or pink noise.

    Flicker noise voltage as a function of time

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    Flicker noise

    Flicker noise is also found in resistors and

    conductors.

    Typeofresistor Noise voltagerange(QV)

    Carbon-composition 0.1-3.0

    Carbon-film 0.05-0.3

    Metal-film 0.02-0.2

    Wire-wound 0.01-0.2

    Flicker noise for various types of resistors

    metal-film

    carbon-

    composition wire-wound

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    Semiconductor noise

    Total noise voltage of semiconductor devices

    varies with frequency with different types of

    noise predominating in different regions.

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    Measuring noise

    To quantify the effect of noise on a signal, we

    use the signal-to-noise (S/N) ratio or SNR.

    A strong signal and weak noise results in a high

    S/N ratio.

    A weak signal and strong noise results in a low S/N

    ratio.

    signal without noise 20 d S/N ratio 10 d S/N ratio

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    Signal-to-noise ratio

    Signal to noise ratio can be expressed in terms

    of voltage or power. signal voltage (rms)noise voltage (rms)

    or here signal po er (W)

    noise po er (W)

    s

    ns s

    sn n

    n

    V

    VS V S P

    PN V N P

    P

    ! !

    ! ! ! !

    +

    signal

    (Vs orPs)

    noise

    (Vn

    orPn)

    signal plus noise

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    Signal-to-noise (decibels)

    Signal to noise ratio is most commonly

    reported in decibels

    / ratio (d ) using voltage: d 20log

    / ratio (d ) using power: d 10log

    s

    n

    s

    n

    V

    S NV

    PS N

    P

    !

    !

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    Noise ratio (NR)

    We often need to quantify how much noise a

    device adds to a signal as it passes through

    the device.

    One measure is the noise ratio (NR) which is

    simply the ratio of input S/N to output S/N.

    amplifier

    output signalinput signal

    / inputNR

    / output

    S N

    S N!

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    Noise figure (NF)

    When the noise ratio (NR) is expressed in

    decibels, its called the noise figure (NF).

    Since the output S/N ratio will be less than theinput, the NR > 1 and NF > 0.

    For an ideal device, NR = 1.0 and NF = 0 dB.

    In practice, NF less than 2 dB is excellent.

    amplifier

    output signalinput signal

    10log [dB]!

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    Noise Ratio (NR) and Noise Figure (NF)

    NF = 10 log (NR)

    NF (dB) = (SNR)input (dB) (SNR)output (dB)

    output

    input

    SNR

    SNRNR !

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    Example Problem 2

    A transistor amplifier has a measured S/N power ratio of

    10,000 at its input and 5,624 at its output.

    (a) Calculate the NR.

    (b) Calculate the NF.

    amplifier

    output signalinput signal

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    Noise in cascaded stages

    The total noise performance of a cascade ofamplifiers depends upon the noise ratio andpower gain of each stage.

    The total noise performance of multiple stagesis given by Friis formula

    whereAi the power gain andNR

    inoise ratio of the i th stage.

    signal input output

    A1, NR1 A2, NR2 A3, NR3

    2 31

    1 1 2 1 2 1

    NR 1 NR 1 NR 1NR NR n

    n A A A A A A

    ! L

    L

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    Example Problem 3

    The gain of the three stages of an amplifier are 8.45 dB, 10.79

    dB, and 20 dB. The noise figures associated with these stages

    are 2.04 dB, 3.0 dB, and 9.29 dB. What is the overall NR and NF

    for this cascade of amplifiers?

    signal input output

    A1 =8.45 d

    NF1 =2.04 d

    A2 =10.79 d

    NF2 =3.0 d

    A3 =20.0 d

    NF3 =9.29 d

    NF

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    Implications of Friis formula

    The total noise performance of a receiver is

    invariably determined by the very first stage.

    Beyond the first and second stage, noise is nolonger a problem.

    signal input output

    A1, NR1A2, NR2 A3, NR3

    2 31

    1 1 2 1 2 1

    NR 1 NR 1 NR 1NR NR n

    n A A A A A A

    ! L

    L

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    Noise Temperature

    N

    N KTB T KB

    ! p !

    T= environmental temperature (290 Kelvin)

    N= noise power (watts)

    K= Boltzmanns constant (1.38 10-23 J/K)

    B = total noise factor (hertz)

    1

    e

    T T F!

    Te= equivalent noise temperature

    T= environmental temperature (290 Kelvin)

    F = noise factor (dimensionless)

    1e

    TF

    T!

    1F u

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    Hartley-Shannon Theorem:

    Significance of SNR

    Hartley-Shannon Theorem (also called

    Shannons Limit) states that the maximumdata rate for a communications channel is

    determined by a channels bandwidth and

    SNR.

    A SNR of zero dB means that noise power

    equals the signal power.

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    Noise Effects on Communications

    Data

    May be satisfactory in the presence of whitenoise but impulse noise will destroy a data signal

    BER (Bit Error Rate) is used as a performancemeasure in digital systems

    Voice

    White noise (continuous disturbance) can bebothersome to humans but impulse noise can beacceptable for speech communications

    SNR (Signal-to-Noise Ratio) is used as aperformance measure in analog systems