35
PHYS225 Lecture 3 Electronic Circuits

PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

  • Upload
    lamphuc

  • View
    222

  • Download
    2

Embed Size (px)

Citation preview

Page 1: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

PHYS225Lecture 3

Electronic Circuits

Page 2: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Course Web Page

• http://people.physics.tamu.edu/depoy/PHYS225.html

• Up now

• Contains

– All lecture notes (PDF)

– All assignments

– Useful links

Page 3: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Last lecture

• Devices not like a resistor– Zener diode

– Tunnel diode

– Capacitor

• Signals– Sinusoid

• Frequency, phase, and amplitude

– Fourier transform• Can be used to characterize complex signals

Page 4: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Sinusoidal • Time variable signal

• Characterized by– Frequency

– Phase

– Amplitude

Page 5: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Sinusoidal

• Many sinusoids of top of each other– Many frequencies, phases, amplitudes added

• Fourier transform to sort out

Page 6: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Fourier transforms

Page 7: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Fourier transforms

Page 8: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Other kinds of signals

Page 9: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

These have Fourier transforms too

Page 10: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Lots of combinations

Page 11: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Pulses

Page 12: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Machines available to generate these signals

• Function generator

• Pulse generator

• Signal generators

• Generally characterized by frequency, shape of pulse, etc.

Page 13: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Circuits with capacitors• Capacitors

– Q = CV– I = C dV/dT

• Current is proportional to rate of change of potential• Change in potential proportional to current

– Power stored as energy in internal electric field• Can get it back again later

• Parallel capacitance add– C = C1 + C2 + C3 + …

• Serial capacitors add like parallel resistors– 1/C = 1/C1 + 1/C2 + 1/C3 + …

• Many different kinds of capacitors– Each has unique and useful properties

Page 14: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Capacitors

Battery

Capacitor

Unit = Farad

Pico Farad - pF = 10-12FMicro Farad - uF = 10-6F

Page 15: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Capacitor types

Ceramic disk

Monolithic ceramic

Dipped silvered-mica

Mylar or polyester

Aluminum electrolytic (+/-)

Tantalum (+/-)

Ceramic disk Monolithic ceramic Dipped siver-mica Mylar Mylar

Solid tantalum, polarized Radial aluminum electrolytic Axial aluminum electrolytic

Page 16: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Capacitors

• Capacitance is determined by 3 factors– Plate surface area– Plate spacing– Insulating material (dielectric)

Page 17: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Capacitor ratings

Physical size of capacitors is related to voltage handling ability – WVDC – working voltage DC

Temperature coefficient may also be important –can be + or – or nearly zero

Temperature coefficient depends upon dielectric material

Page 18: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Circuits with capacitors

Potential across capacitor changes when a current flows through it

Page 19: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Circuits with capacitors

• C dV/dt = I = -V/R

• V = A e-t/RC

• Capacitors will “charge up” over time after application of an initial voltage

– Approaches the applied potential

• Will also “discharge” over time if the applied potential is reduced

Page 20: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Capacitor Charging

Page 21: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Capacitor Discharge

Page 22: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

RC time constant

Page 23: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

RC time constant• Product of RC in a simple circuit

– For R in ohms and C in farads, RC is in seconds

• 1 µF across 1KΩ = 1 ms

– Characteristic time of response for the circuit

• Sets “frequency response” of circuit

– How quickly circuit responds

– How much of which frequencies get through the circuit

Page 24: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Some applications

Time-delay circuit:Can induce a delay in a signal

Page 25: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Another application

I = C d/dt(Vin – V) = V/R

V = RC d/dt(Vin – V)

For small changes in dV/dtV ≈ RC dVin/dt

Circuit differentiates the incoming signal

For square wave input, output is a series of pulses

Page 26: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional
Page 27: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Unintentional capacitive coupling

Page 28: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Circuits with capacitors

• Integrators

– V << Vin

• Ramp generators

– If provide constant current,

• Voltage continues to increase

• All sometimes useful

Page 29: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Inductors

• V = L dI/dt; L is inductance– A simple coil of wire!

• Putting a voltage across an inductor causes the current to ramp

• Power stored in as energy in the magnetic field• 1 V across 1 henry produces 1 amp• Rare to use, but useful in some circumstances

– RF “chokes”– Transformers

• Two closely coupled inductors

Page 30: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Inductors

Values specified in henries (H), millihenries (mH) and microhenries (μH)

A coil of wire that may be wound on a core of air or other non-magnetic material, or on a magnetic core such as iron powder or ferrite.

Two coils magnetically coupled form a transformer.

Page 31: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

31

Inductor types

Molded inductor & air-wound inductor Adjustable air-wound inductor

Ferrite core toroidal transformer Iron powder toroidal inductorAir wound inductor

Page 32: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Inductor ratings

Wire gauge and physical size of the coil determine the current handling capacity.

Core material will have a temperature dependence. Air is best, followed by iron powder, then ferrites.

Page 33: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Transformers

• Two closely coupled coils

• AC voltage applied across one will appear across the other at a different voltage

– Change depends on ratio of the number of turns in the coil

• Power is conserved

– So if voltage goes up, current will go down

• Generally very efficient

Page 34: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Transformer

Page 35: PHYS225 Lecture 3 - Physics and Astronomy at TAMUpeople.physics.tamu.edu/depoy/phys225/Notes/lecture3.pdf · Lecture 3 Electronic Circuits. ... •Change in potential proportional

Transformers

• Useful to change “line” power to something else

– At the heart of everything used to power computers, cell phones, etc.

• Isolate circuit from actual connection to the power line