Capacitance Measurement

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    Capacitance Measurement

    Apr. 2012

    All Rights Reserved, Copyright Samsung Electro-Mechanics Co., Ltd.

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    CONTENTS Confidential

    1. Introduction

    2. LCR meters and Measurement Principle

    2-1. LCR meters

    2-2. Measurement Theory

    - .

    3. Characteristics of MLCC

    - . empera ure arac er s cs

    3-2. DC Bias Characteristics3-3. AC Voltage Characteristics

    3-4. Aging Characteristics

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    3-5. DC Bias Aging Characteristics

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    1. Introduction Confidential

    A capacitor is an electrical device that can store energy in the electric field between a pair of closely spaced

    conducting plates. Capacitance value means the measure of how much charge a capacitor can store at a certain

    vo age. apac ance o s ou e measure un er appropr a e measur ng con ons suc as empera ure,

    voltage (AC/DC), and frequency. Especially, when you measure a high dielectric MLCC (Class II: X7R, X6S, X5R,

    Y5V) by LCR meter, you may be careful to obtain a reasonable capacitance using specified measurement conditions.

    Before measurement, the equipment should be used with correct meter setting and have the capability required for

    accura e capac ance measuremen . e ac ua measuremen con ons o capac ance o ass an s are

    shown in tables below. The temperature used for these conditions is 25 degree.

    Nominal Capacitance Frequency Voltage(AC) Voltage(DC)

    1,000pF 1MHz 10% 0.5~5Vrms No Bias

    ,> 1,000pF 1KHz 10%

    CLASS II

    Nominal Capacitance Frequency Voltage(AC) Voltage(DC)

    10uF 1KHz 10% 1.0 0.2Vrms No Bias

    * 10uF 1KHz 10% 0.5 0.1Vrms

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    > 10uF 120Hz 20% 0.5 0.1Vrms

    * Exceptions: Please check the specification on the web site

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    2-1. LCR meters Confidential

    LCR meters are used for measurement of the capacitance and dissipation factor of MLCCs.

    Typical LCR meters are shown in Table including 4288A, 4268A, 4284A, and E4980A by Agilent Technologies Corp.

    LCR Meter Overview Application

    4288A

    1kHz/1MHz

    High-speed sorting tests of ceramic

    capacitors.

    Class I

    Class II

    Meteru

    4268A

    120Hz/1kHz

    Constant test level for high value ceramic

    capacitor tests.

    Class II

    Capacitance

    Meter*Auto level control (ALC)

    4284A Wide frequency Range Class I

    LCR Meter4284A : 20Hz to 1 MHz

    E4980A : 20Hz to 2 MHz

    Auto level control (ALC)

    Class II

    Option 001.

    power and DC bias enhancement (+/- 40V)

    E4980A

    Precision

    LCR Meter

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    ALC: The automatic level control (ALC) feature adjusts the voltage across the DUT to the same level as the signal voltage level

    setting. By this feature, you can maintain a constant level of voltage of measurement signals applied to the DUT. Technical overview is available at www.agilent.com

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    2-2. Measurement Theory Confidential

    When the AC voltage (V) is applied to the DUT and the AC current (I) is flowing through the DUT, the impedance

    (|Z|) can be calculated according to the Ohms raw (|Z|=V/I). The measurement circuit depends on the frequency.

    So, there are two methods (Auto Balance Bridge and RF I-V). It also depends on the type of fixture.

    DUT

    I

    V

    R: ResistanceAV

    Source Voltage Current

    X: Reactance

    IZI: Absolute value of impedance

    : Phase of impedance

    o age

    I

    V

    Z

    Fig. Circuit model

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    2-2. Measurement Theory Confidential

    Energy loss is zero in the ideal capacitor. But, real capacitor has dielectric loss and electrode loss by the parasitic

    resistance. Loss of ca acitor is shown b the dela in of hase an le between AC volta e and current.

    DF (Dissipation Factor) is described as tan. Here, means delayed phase angle.

    XESRZ

    j

    Inductive

    (High freq.)

    CLXc

    cc

    1

    X

    Z

    ESR

    ZXZESR

    1

    sin,cos

    Capacitive

    XQESR

    -

    Real (R).

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    Fig . Impedance characteristics of general Capacitor

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    2-3. ALC (Automatic Level Control) Function Confidential

    The automatic level control (ALC) feature adjusts the voltage across the DUT to the same level as the signal

    voltage level setting. By this feature, you can maintain a constant level of voltage of measurement signals applied

    to the DUT. The ALC feature uses a monitorable feedback circuit to iterate a feedback loop as shown in figure.

    The feedback loop consists of level measurement and level change. The time is required for level adjustment.

    Feedback loo

    DUT

    V

    Source

    RHIGH LOW

    o age

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    Fig. Circuit model from Users Guide provided by Agilent Technologies

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    2-3. ALC Function Confidential

    The automatic level control (ALC) feature adjusts the voltage across the DUT to the same level as the signal

    voltage level setting. When ALC function is off, the capacitance was measured as ~43F and when ALC function

    ~, . .

    and off was ~6 F. However, we cant see the difference at AC voltage of 0.5V when looking at the figure of

    capacitance change. Therefore, the correct capacitance value can be obtained by using ALC function.

    40

    ALC (on)

    ALC (off)50.0

    55.0

    0

    20

    (%)

    35.0

    40.0

    45.0

    ap(uF)

    -40

    -20

    20.0

    25.0

    30.0C

    ALC (on)

    ALC (off)

    Fig. Capacitance of 0603 X5R 47F with AC voltage Fig. Capacitance change of 0603 X5R 47F with AC voltage

    . . .

    AC voltage(V)

    . . .

    AC voltage(V)

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    for ALC on and off (Agilent 4284A, 120Hz) for ALC on and off (Agilent 4284A, 120Hz)

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    3-1. Temperature Characteristics Temp vs.CConfidential

    Temperature coefficient of capacitance (TCC) can be described as the change of capacitance dependent on

    temperature in MLCCs. There are several TCC categories found in Class I and II. TCC of Class I and II MLCCs are

    shown in figure. Class I MLCCs are composed of paraelectric material and show simple TCC behaviors. It has a

    near var a on n capac ance w empera ure. e c ange n capac ance w empera ure s expresse near y

    as parts per million per degree centigrade (PPM/).

    Class II MLCCs such as X5R and X7R show irregular and high change in capacitance with temperature. This is due

    to the ferroelectric nature of the dielectric material of barium titanate (BaTiO3). The change in capacitance with

    empera ure s expresse as a percen c ange over a spec e empera ure range. or examp e, means a

    the capacitance can change by +/-15% across a temperature range of -55 to 125.

    40% C

    Table. Temperature characteristics of Class I and II MLCCs

    Class

    Temperature

    Coefficient

    Dielectric

    Constant

    Operating

    Tem erature

    Capacitance

    Chan e20

    +85 oC

    +125oC

    +22%+105oC

    Class I C0G 6 ~ 400 -55 ~ +125 0 30ppm/

    X5R -55 ~ +85 15%

    --- C0G

    Class II1,000 ~

    20,000

    X6S -55 ~ +105 22%

    X7R -55 ~ +125 15%

    Y5V -30 ~ +85 -82 ~ +22%-20

    X7RX5R-15%

    -22%

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    Fig. Capacitance change of X5R, X7R, Y5V, C0G with temperature

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    3-2. DC Bias characteristics DC bias vs. CConfidential

    DC bias is an important electrical parameter affecting the capacitance of MLCCs. DC bias characteristics can be

    described as the phenomena of capacitance loss in Class II with increasing DC voltage. This behavior is dependent

    on the dielectric formulation, microstructure, and internal construction of MLCC as well as DC voltage load.

    ass s are ase on a 3 w erroe ec r c po es an as m s e po e movemen s resu ng n

    reduction of the dielectric constant and capacitance.

    The DC bias characteristics of C0G, X5R, X7R, and Y5V MLCCs are shown in figure. Class I MLCC, C0G shows the

    stable capacitance value because of its paraelectric structure without dipoles although its relative dielectric constant

    .]

    s or ers o magn u e ower an ass suc as , , an . n case o , s ows e mos severe

    degradation despite of the highest dielectric constant. X5R/X7R have high dielectric constants which are preferred

    for high capacitance applications.

    X5R / X7R

    C0G

    ange[a

    rb

    citancec

    10 20 30 40 50

    DC voltage [V]

    Cap

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    Fig. Capacitance change of X5R, X7R, Y5V, C0G with DC voltage

    (HP 4284A, 25oC, 1.0Vrms, 1kHz (X7R, Y5V) / 1MHz (C0G))

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    AC voltage vs. C3-3. AC voltage characteristics Confidential

    AC voltage characteristics can be described as the phenomena of capacitance change in Class II with increasing

    AC voltage. Class I MLCCs composed of paraelectric material do not show this phenomenon. The AC voltage

    c arac er s cs o ass s are s own n gure. n ass s, s ows e more severe c ange w

    AC voltage than X5R/X7R. This is due to the non-linear characteristics in voltage-polarization curve of ferroelectric

    materials. Thus, the slope in the curve increases and the capacitance increases as AC voltage increases.

    40 40

    0

    (%) 0

    (%)

    -

    -20

    -

    -20

    0.0 0.5 1.0

    AC voltage(V)

    0.0 0.5 1.0

    AC voltage(V)

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    . , .

    with AC voltage (Agilent 4284A, 1kHz)

    . , .

    with AC voltage (Agilent 4284A, 120Hz)

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    3-4. Aging Characteristics Time vs. CConfidential

    Aging is a time dependent phenomenon encountered in Class II MLCCs. Class I MLCCs do not show agingdue to the paraelectric nature of the composed material. However, Class II MLCCs such as X5R, X7R, and

    Y5V have ferroelectric dielectrics based on BaTiO3 and the capacitance is decreased logarithmically over time.

    Figure shows the aging behavior of Class I and II MLCCs with different temperature characteristics. Aging rate

    increases with dielectric constant of the material. C0G shows a constant capacitance value independent of

    time due to its paraelectric characteristics while Y5V the highest capacitance value and X5R/X7R have an

    intermediate aging rate. Aging is intrinsically reversible. The capacitance can be recovered after heattreatment. MLCCs can be returned to ferroelectric structure by heating above the Curie point (at least 1 hr at

    Ct = C0 (1 - k log10 t)Ct = Capacitance value, t hours after the start of aging

    C0= Initial capacitance value, k = Aging constant, t = Aging time

    150) and cooling to room temperature.

    C0G

    X7R/X5Rgrate[%

    ]

    C0G

    X7R/X5R-10 Slope (k) 2~5%

    Y5V

    picalagin

    Y5V

    -20

    -30

    Slope (k) 5%~

    1 2 3

    Time [log10t hr]

    4 50 1 2 3

    Time [log10t hr]

    T

    4 5

    -40

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    Fig. Typical aging rate of X7R/X5R, Y5V, C0G with aging timeDe-aging : Decreased capacitance is recovered after heat treatment ( above 150)

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    3-5. DC Bias Aging Characteristics DC bias, Time vs. CConfidential

    In order to increase the capacitance density of MLCCs, the dielectric layer thickness should be reduced and thismeans the increase in the electric field applied to dielectric layers. The aging characteristics under DC biasbecomes more important in the high-end products with ultra thin dielectric layers. DC bias aging characteristics

    observed in the working condition. The effective capacitance can be described as the capacitance observed inworking condition. The effective capacitance is more important than the nominal capacitance because thenominal capacitance is dependent on DC-bias, temperature and time. Better effective capacitance can be

    obtained by the improvement of DC-bias and aging characteristics.

    34

    34

    30

    32

    ce(uF)

    ce(F)

    32

    30

    24

    26

    Capacita

    Capacitan

    26

    24

    1 10 100 1000 1000020

    Time (hr)

    20

    1 10 100 1000 10000

    Time (hr)

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    Fig. Capacitance of 0805 X5R47uF, 6.3V with time in the measurement condition of85, 1.2V(DC) (E4980A, 1kHz)

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