lecture 6 higher order filters using inductor emulation

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Lecture 6 Higher Order Filters Using Inductor Emulation

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Page 1: Lecture 6 Higher Order Filters Using Inductor Emulation

Lecture 6

Higher Order Filters UsingInductor Emulation

Page 2: Lecture 6 Higher Order Filters Using Inductor Emulation

Inductor Emulation Using Two-port Network

GIC (General Impedance Converter)

GII (General Impedance Inverter)

Page 3: Lecture 6 Higher Order Filters Using Inductor Emulation

GyratorPositive Impedance Inverter

Floating inductor

Page 4: Lecture 6 Higher Order Filters Using Inductor Emulation

Gyrator Example

Gyration resistance=1/g1=1/g2=R

Page 5: Lecture 6 Higher Order Filters Using Inductor Emulation

Riordan Gyrator

Page 6: Lecture 6 Higher Order Filters Using Inductor Emulation

Example

For Gyration resistance=1kΩ

Page 7: Lecture 6 Higher Order Filters Using Inductor Emulation

Antoniou GIC

Page 8: Lecture 6 Higher Order Filters Using Inductor Emulation

Antoniou GIC

Inductance emulation is optimum in case of no floating inductorsi.e., LC high-pass filters

Page 9: Lecture 6 Higher Order Filters Using Inductor Emulation

Example

3rd Order LPF

6th Order BPF

Page 10: Lecture 6 Higher Order Filters Using Inductor Emulation

Bruton’s transformation

Page 11: Lecture 6 Higher Order Filters Using Inductor Emulation

FDNR

Bruton’s inductor simulation based on FDNR

Most suitable for LC LPF with minimum cap realization

Page 12: Lecture 6 Higher Order Filters Using Inductor Emulation

Filter Performance & Design Trade-offs

Transfer function (ω0 , Q or BW, Gain, out-of-band attenuation, etc.)

Sensitivity (component variations, parasitics)

Dynamic range (DR)Maximum input signal (linearity)Minimum input signal (noise)

Power dissipation & Area

Page 13: Lecture 6 Higher Order Filters Using Inductor Emulation

Maximum signal (supply limited)

Page 14: Lecture 6 Higher Order Filters Using Inductor Emulation

Voltage swing scaling

Page 15: Lecture 6 Higher Order Filters Using Inductor Emulation

Power dissipation

For nth order

Page 16: Lecture 6 Higher Order Filters Using Inductor Emulation

• Thermal noise of a resistor

The thermal noise of a resistor R can be modeled by a series voltage source, with the

one-sided spectral density

2nV = Sv(f) = 4kTR, f 0,

where k = 1.3810 23 J/K is the Boltzmann constant and Sv(f) is expressed in V2/Hz.

Minimum signal (noise limited)

Page 17: Lecture 6 Higher Order Filters Using Inductor Emulation

• Example: low-pass filter

We compute the transfer function from VR to Vout: 1

1

RCs

sV

V

R

out

From the theorem, we have 14

14 2222

2

fCRkTRf

V

VfSfS

R

outRout

.

The total noise power at the output:

C

kT

u

uu

C

kTdf

fCR

kTRP outn

0tan

2

14

4 1

0 2222, (V2)

Page 18: Lecture 6 Higher Order Filters Using Inductor Emulation

Simple Example

Large R, Small C Large noise, parasitic sensitive

Large C, Small R Large power, large area