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1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

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Page 1: 1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

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Interconnect and PackagingLecture 3: Skin Effect

Chung-Kuan ChengUC San Diego

Page 2: 1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

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Outlines

I. Transmission Line Model

II. Spectrum of Configurations

III. Skin Effect

IV. Coaxial Cable

Page 3: 1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

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I. Transmission Line Model

RΔl LΔlCΔl

RΔl LΔl

CΔl …

i(z,t)

RΔl LΔl RΔl LΔl

Voltage drops through serial resistance and inductance

Current reduces through shunt capacitance

Resistance increases due to skin effect

Shunt conductance is caused by loss tangent

Page 4: 1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

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I. Interconnect Model

• Telegrapher’s equation:

),(),(),(

),(),(

),(

tzGVdt

tzdVC

dz

tzdIdt

tzdILtzRI

dz

tzdV

• Propagation Constant:

jCjGLjR ))((

• Wave Propagation:

//,),( 0 tzveVtzV tjzjz

• Characteristic Impedance

)/()( CjGLjRZ

Page 5: 1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

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I. Interconnect Model

LCRGRGRCLGLCj

LCRGRGRCLGLCj

2222224

2222224

)(])()[()(2

1

)(])()[()(2

1

• Propagation Constant:

• Wave Propagation:

//,),( 0 tzveVtzV tjzjz

• Characteristic Impedance

)/()( CjGLjRZ

jCjGLjR ))((

Page 6: 1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

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I. Interconnect Model (Constants)

8.376/mH /104 7

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II. Spectrum of Configurations jCjGLjR ))((

RLGC R L G C

0001 ( jwC ) Capacitance

0010 ( G ) Shunt

0011 ( G + jwC ) Leaky Capacitance

0100 ( jwL ) Inductance

0101 ( jwL )( jwC ) Lossless LC Line

0110 ( jwL )( G ) Skin Effect Derivation

0111 ( jwL )( G + jwC ) Skin Effect + Permitivity

1000 ( R ) Resistance

1001 ( R )( jwC ) RC Line

1010 ( R )( G ) Leaky Resistance

1011 ( R )( G + jwC ) Leaky RC Line

1100 ( R + jwL ) Lossy Inductance

1101 ( R + jwL )( jwC ) Lossy LC Line

1110 ( R + jwL )( G ) Lossy and Leaky Inductance

1111 ( R + jwL )( G + jwC ) Transmission Line

Page 8: 1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

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III. Skin Effect

2

22

))((

LGj

LG

LGj

CjGLjR

Skin Depth

(Equivalent Depth of Uniform Current)

Assuming that resistance and capacitanceare negligible.

Page 9: 1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

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III. Skin EffectBoundary condition:•Charges at the boundary shield the electric field.•Thus, capacitance C does not change with frequency.

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IV. Coaxial Cable

02,

2),

11(

2

1

Z

R

baR

776.3/

/1/ln0

0Zab

baabda

d

)/ln(60

2

)/ln(0 ab

abZ

r

Page 11: 1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

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IV. Coaxial Cable: Inductance

abL

rdra

IbrLI

a

/ln28

2),(0 2

2

abI

raa

I

drr

Idr

a

Ir

rbr

b

a

a

r

/ln2

)(4

22),(

222

2

2

Page 12: 1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

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IV. Coaxial Cable: Inductance

iLR

2

11,

2

1

2

20

ppR

ppL

p

Irdr

p

IIL

i

i

Page 13: 1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

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IV. Coaxial Cable: Inductance

)/()(

/)(

)(

2

)(

1

0

jj

mjaI

jaI

aZi

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IV. Coaxial Cable: Impedance

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IV. Coaxial Cable: Impedance22ACDC RRR

Page 16: 1 Interconnect and Packaging Lecture 3: Skin Effect Chung-Kuan Cheng UC San Diego

Skin Effect

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