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AC Generators - Electricity and Optics - Lecture Slides, Slides of Electrical Engineering

You can find here lecture series for complete Electricity and Optics course. All related topics are explained in slides. This lecture slides contain: Ac Generators, Alternating Current in a Resistor, Power Dissipated, Average Value, Root-Mean-Square, Standard Alternating Voltage, Ac Power Distribution, Power Grid, Inductors, Capacitors

Typology: Slides

2012/2013

Uploaded on 08/20/2013

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LECTURE 19
AC Generators
AC Circuits
Start by considering simple circuits
with one element (R, C, or L) in
addition to the driving emf.
It will lead to Oscillations and Driven RLC
circuits
8/16/12 2
Alternating Current Generators (DEMO)
(N = 2 for this coil)
8/16/12 3
Alternating Current Generators
= t+$ position of n
wrt B
m $
00 maximum
positive
0
900 0 maximum
positive
1800 maximum
negative 0
2700 0 maximum
negative
8/16/12 4
Alternating Current in a Resistor
pf3
pf4
pf5

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LECTURE 19

  • AC Generators
  • AC Circuits
  • Start by considering simple circuits

with one element ( R , C , or L ) in

addition to the driving emf.

  • It will lead to Oscillations and Driven RLC

circuits

8/16/12 2

Alternating Current Generators (DEMO)

(N = 2 for this coil) 8/16/12 3

Alternating Current Generators

 = t+$ position of n wrt Bm $ 00 maximum positive 0

900 0 maximum

positive

1800 maximum

negative

2700 0 maximum

negative (^) 8/16/12 4

Alternating Current in a Resistor

8/16/12 5

Power Dissipated in a Resistor

Average value Peak value 8/16/12 6

Average value of cos^2 t

cos

sin

cos

cos d

cos 2 d

d

cos

d

1 cos 2

d

cos d

cos

Let t.

2 4 2 0 4 0 2 0 2 2 0 2 0 2 0 2 0 2 2

π π π π π π π

8/16/12 7

Root-mean-square (rms) values

8/16/12 8

Standard Alternating Voltage in the US

+peak

-peak

8/16/12 13

Inductors in AC Circuits

8/16/12 14

Inductors in AC Circuits

⎟ ⎠ ⎞ ⎜ ⎝ =^ ⎛^ ω −π ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ π θ= θ − = ω = ω 2 I I cos t , 2 Sincesin cos I I sin t V V cos t peak peak L L, peak 8/16/12 15

Relationship between Irms & Vrms

Irms = VL , rms XL

where XL = ω L is the inductive reactance.

  1. XL is similar to R in Irms = VR , rms R
  1. SI unit for XL : Ω (ohm)
  2. Average power delivered to an inductor in an ac circuit is zero. 8/16/12 16

Capacitors in AC Circuits

8/16/12 17

Capacitors in AC Circuits

⎟ ⎠ ⎞ ⎜ ⎝ ⎛ π = ω + ⎟ ⎠ ⎞ ⎜ ⎝ θ=−^ ⎛^ θ +π =− ω = ω 2 I I cos t , 2 Sincesin cos I I sin t V V cos t peak peak C C, peak 8/16/12 18

Relationship between Irms & VC,rms

Irms = VC , rms XC where XC =

ω C is the capacitive reactance

  1. XC is similar to R in Irms = VR , rms R
  1. SI unit for XC : Ω (ohm)
  2. Average power delivered to a capacitor in an ac circuit is zero. 8/16/12 19

Phasors

  • A phasor is a “vector” whose magnitude is the maximum value of a quantity (eg V or I ) and which rotates counterclockwise in a 2-d plane with angular velocity . Recall uniform circular motion: The projections of r (on the vertical y axis) execute sinusoidal oscillation.

x

y y

y = r sin ω t

x = r cos ω t

Angular speed: phasors rotate counter clockwise about the origin with an angular speed of . Length: represents the amplitude of the AC quantity Projection: on the vertical axis represents the value of the AC quantity at time t. Rotation angle: phase of the AC quantity at time t. 8/16/12 20

Phasors for R

  • V in phase with I VR = RIR = ε m sin ω t

IR =

ε m

R

sin ω t