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  • 參數(shù)資料
    型號: RT8011APF
    廠商: Richtek Technology Corporation
    英文描述: 2A, 4MHz, Synchronous Step-Down Regulator
    中文描述: 第2A,4MHz,同步降壓型穩(wěn)壓器
    文件頁數(shù): 11/17頁
    文件大?。?/td> 424K
    代理商: RT8011APF
    RT8011/A
    11
    DS8011/A-00 August 2006
    www.richtek.com
    Application Information
    The basic RT8011/A application circuit is shown in Typical
    Application Circuit. External component selection is
    determined by the maximum load current and begins with
    the selection of the inductor value and operating frequency
    followed by C
    IN
    and C
    OUT
    .
    Operating Frequency
    Selection of the operating frequency is a tradeoff between
    efficiency and component size. High frequency operation
    allows the use of smaller inductor and capacitor values.
    Operation at lower frequency improves efficiency by
    reducing internal gate charge and switching losses but
    requires larger inductance and/or capacitance to maintain
    low output ripple voltage.
    The operating frequency of the RT8011/A is determined
    by an external resistor that is connected between the RT
    pin and ground. The value of the resistor sets the ramp
    current that is used to charge and discharge an internal
    timing capacitor within the oscillator. The RT resistor value
    can be determined by examining the frequency vs. RT
    curve. Although frequencies as high as 4MHz are possible,
    the minimum on-time of the RT8011/A imposes a minimum
    limit on the operating duty cycle. The minimum on-time
    is typically 110ns. Therefore, the minimum duty cycle is
    equal to 100 x 110ns x f(Hz).
    Inductor Selection
    For a given input and output voltage, the inductor value
    and operating frequency determine the ripple current. The
    ripple current
    Δ
    I
    L
    increases with higher V
    IN
    and decreases
    with higher inductance.
    ×
    IN
    V
    L
    f
    Having a lower ripple current reduces the ESR losses in
    the output capacitors and the output voltage ripple. Highest
    efficiency operation is achieved at low frequency with small
    ripple current. This, however, requires a large inductor. A
    reasonable starting point for selecting the ripple current
    is
    Δ
    I = 0.4(I
    MAX
    ). The largest ripple current occurs at the
    highest V
    IN
    . To guarantee that the ripple current stays
    below a specified maximum, the inductor value should be
    chosen according to the following equation :
    IN(MAX)
    L(MAX)
    1
    =
    Δ
    OUT
    V
    OUT
    V
    L
    I
    Δ
    ×
    =
    OUT
    V
    OUT
    I
    V
    1
    f
    V
    L
    Inductor Core Selection
    Once the value for L is known, the type of inductor must
    be selected. High efficiency converters generally cannot
    afford the core loss found in low cost powdered iron cores,
    forcing the use of more expensive ferrite or mollypermalloy
    cores. Actual core loss is independent of core size for a
    fixed inductor value but it is very dependent on the
    inductance selected. As the inductance increases, core
    losses decrease. Unfortunately, increased inductance
    requires more turns of wire and therefore copper losses
    will increase.
    Ferrite designs have very low core losses and are preferred
    at high switching frequencies, so design goals can
    concentrate on copper loss and preventing saturation.
    Ferrite core material saturates
    hard
    , which means that
    inductance collapses abruptly when the peak design
    current is exceeded.
    This result in an abrupt increase in inductor ripple current
    and consequent output voltage ripple.
    Do not allow the core to saturate!
    The transition from low current operation begins when the
    peak inductor current falls below the minimum peak
    current. Lower inductor values result in higher ripple current
    which causes this to occur at lower load currents. This
    causes a dip in efficiency in the upper range of low current
    operation.
    Figure 5
    0
    0.5
    1
    1.5
    2
    2.5
    3
    3.5
    4
    4.5
    0
    100 200 300 400 500 600 700 800 900 100
    0
    )
    R
    RT
    (k
    Ω
    F
    RT = 154k for 2MHz
    RT = 332k for 1MHz
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