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Welcome Seminar on MEMRISTOR

Memristor Seminar

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Page 1: Memristor Seminar

Welcome

Seminar on

MEMRISTOR

Page 2: Memristor Seminar

MEMRISTOR

Memristor

Memory Resistor+

Memristor

Page 3: Memristor Seminar

Defination of Memristor A memristor is formally defined as a two-

terminal elementin which the magnetic flux between the terminals is a amount of electric charge that has passed through the device.

Characterized by Memristance

Page 4: Memristor Seminar

Memristance Memristance is simply charge-dependent,

is a property to retain its resistance level even after power had been shut down.

V(t) = M(q(t))*I(t)

Unit - ohm (Ω)

Symbol

Page 5: Memristor Seminar

Emergence Of Memristic TheoryTheory was developed in 1971 by

Professor Leon Chua at University of California, Berkeley.

Found while exploring symmetry between the three fundamental passive linear circuit elements

In 2006, R.Stanley Williams developed practical model.

Page 6: Memristor Seminar

Fundamental Circuit Variables

Voltage, V (V) – work done required to bring charge from ∞ to a Electric field.

Current, I (A) – flow of electric chargeFlux, Φ(W) – rate of flow through an

areaCharge, Q (C) – energy per electron

Page 7: Memristor Seminar

Fundamental Relationships

Current is the derivative of Charge

Q= ∫I dt

Voltage is the derivative of Flux

V= ∫ dΦ/dt

Page 8: Memristor Seminar

Symmetry Of Relationships

Voltage (V)

Current(i)

Charge (q)

Flux (Φ)

Page 9: Memristor Seminar

3 Fundamental Passive Linear Elements

Capacitor,C (F)

Resistor,R (Ω)

Inductor,L (H)

Page 10: Memristor Seminar

CAPACITORS

q = C v

Page 11: Memristor Seminar

Symmetry Of Relationships

Voltage (V)

Current(i)

Charge (q)

Flux (Φ)

q=CvCapacitors q=CvCapacitorsCapacitors

Page 12: Memristor Seminar

RESISTORS

Ohm’s Lawv = R i

Page 13: Memristor Seminar

Symmetry Of Relationships

Voltage (V)

Current(i)

Charge (q)

Flux (Φ)

Resistors v=Ri

Capacitors q=CvCapacitors

Page 14: Memristor Seminar

INDUCTORS

Φ = L i

Page 15: Memristor Seminar

Symmetry Of Relationships

Voltage (V)

Current(i)

Charge (q)

Flux (Φ)

Φ = Li Inductors

??

v=dΦ/dt i=dq/dt

Resistors v=Ri

q=CvCapacitors

Page 16: Memristor Seminar

Symmetry Of Relationships

MemristorsΦ=Mq

Voltage (V)

Current(i)

Charge (q)

Flux (Φ)

Φ = Li Inductors

v=dΦ/dt i=dq/dt

Resistors v=Ri

q=CvCapacitors

Page 17: Memristor Seminar

Relationship With Other VariablesΦ = M q

dΦ/dt = M(q) dq/dt

V(t) = M(q) I

P = I² M(q)

Page 18: Memristor Seminar

Property Of Memristor Retain its resistance level even after

power had been shut down

Remember (or recall) the last resistance it had, before being shut off.

Page 19: Memristor Seminar

Memristic State Memristivity has an inverse square relationship

with thickness of the material, so smaller = better!

Nonvolatile state can be accomplished by memristors because their state is encoded by impedance (physically), not by voltage.

Page 20: Memristor Seminar

WORKING

PT PTTiOv(2-x)

TiO2

3 nm

2 nm

OxidizedReduced

(-)ve (+)ve

Applied voltage makes the oxygen vacancies (+ve) to shift towards the –ve voltage.

Page 21: Memristor Seminar

WORKINGShift between the layers in

permanent in nature.It exist even after the voltage has

been removed.Causes the permanent change in

resistance

Page 22: Memristor Seminar

V-I characteristics

Page 23: Memristor Seminar

Benefits Of Memristor TechnologyWould allow for a quicker boot up since

information is not lost when the device is turned off.

Creating a Analog Computer that works much faster than Digital ones.

Uses less energy and produces less heat.

Page 24: Memristor Seminar

What Sets Memristor Apart ?? Conventional devices use only 0 and 1;

Memristor can use anything between 0 and 1.

Faster than Flash memory. Allow digital cameras to take pictures with

no delay inbetween Innovating nanotechnology due to the fact

that it performs better the smaller it becomes.

Page 25: Memristor Seminar

THANK

YOU