ELECTRIC CIRCUITS ECSE2010 Spring 2003 Class 28 - PowerPoint PPT Presentation

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ELECTRIC CIRCUITS ECSE2010 Spring 2003 Class 28

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Ideal Transformers: Primary and Secondary Windings; No Loss. Turns Ratio, N = N2 / N1 ... ACTIVITY 28-2. ACTIVITY 28-2. Two Transformers. Refer to Middle Section ... – PowerPoint PPT presentation

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Title: ELECTRIC CIRCUITS ECSE2010 Spring 2003 Class 28


1
ELECTRIC CIRCUITSECSE-2010Spring 2003Class 28

2
ASSIGNMENTS DUE
  • Today (Thursday)
  • Activities 28-2, 28-1 (In Class)
  • Next Monday
  • Homework 10 Due
  • Activities 29-1, 29-2 (In Class)
  • Next Tuesday/Wednesday
  • Activity 30-1 (In Class)

3
REVIEW
  • Ideal Transformers
  • Primary and Secondary Windings No Loss
  • Turns Ratio, N N2 / N1
  • Dot Convention N gt - N if opposite
  • Transformer Rules V2 N V1
  • I2 I1 / N
  • Refer to Primary ZL gt ZL / N2
  • Refer to Secondary VS gt N VS
  • ZS gt N2 ZS

4
IDEAL TRANSFORMER
5
IDEAL TRANSFORMER
6
IDEAL TRANSFORMER
7
IDEAL TRANSFORMER
8
IDEAL TRANSFORMER
9
IDEAL TRANSFORMER CKT
10
REFERRAL TO PRIMARY
11
EXAMPLE
12
EXAMPLE
13
REFERRAL TO SECONDARY
14
EXAMPLE
15
EXAMPLE
16
POWER TRANSFER
17
POWER TRANSFER
  • General AC Circuit
  • Source Network gt Vs in series with Zs
  • Thevenin Equivalent Circuit
  • Load Network gt ZL
  • For PMAX to ZL
  • Want ZL Zs
  • Often Helps to Use Transformer
  • Provides another Knob

18
ACTIVITY 28-2
19
ACTIVITY 28-2
  • Two Transformers
  • Refer to Middle Section
  • T1 Refer from Primary to Secondary
  • T2 Refer from Secondary to Primary
  • Vs,RMS 640 Volts (RMS)
  • Find I, gt Calculate V1, V2
  • Calculate I1, I2, I4, V3, V4
  • Find Ptotal and Efficiency

20
ACTIVITY 28-2
21
ACTIVITY 28-2
22
ACTIVITY 28-2
23
ACTIVITY 28-2
24
ACTIVITY 28-2
25
ACTIVITY 28-2
26
ACTIVITY 28-2
27
ACTIVITY 28-2
28
ACTIVITY 28-2
29
ACTIVITY 28-2
30
ACTIVITY 28-2
31
ACTIVITY 28-2
32
ACTIVITY 28-2
33
ACTIVITY 28-2
34
ACTIVITY 28-2
35
MUTUAL INDUCTANCE
  • Consider 2 Inductors, L1, L2
  • Inductors can be in the same Circuit, or in
    different Circuits
  • Magnetic Field of L1 can link with L2 and vice
    versa
  • If Magnetic Field changes with time gt Creates
    voltages in linked coils L1, L2
  • Refer to this as Mutual Inductance, M
  • M is also measured in Henries
  • Can show that M 0 lt k lt 1

36
MUTUAL INDUCTANCE
37
MUTUAL INDUCTANCE
38
MUTUAL INDUCTANCE
39
MUTUAL INDUCTANCE
  • Consider Circuit Model
  • v1 L1 di1 / dt M di2 / dt
  • v2 L2 di2 / dt M di1 / dt
  • Note direction of i1, i2
  • Dot convention If Current goes IN to Dot
    Voltage due to Mutual Inductance is Positive
  • Replace M with (- M) if dots are on opposite ends
    of Inductors

40
TEE MODEL
  • Consider a Circuit That Looks Like a Tee
  • 3 Ideal inductors
  • No mutual inductance

41
TEE CIRCUIT
42
TEE MODEL
43
TEE MODEL
  • For a Tee Circuit
  • Ideal inductors, no mutual inductance
  • Same equations as before
  • gt Can Replace Inductors exhibiting Mutual
    Inductance with Tee Model and then do AC Steady
    State Circuit Analysis

44
TEE MODEL
45
ACTIVITY 28-1
46
ACTIVITY 28-1
  • Always Wise to Label Nodes
  • Can get lost otherwise
  • Look for Common Node
  • Node a for this circuit
  • Replace with Tee Model

47
ACTIVITY 28-1
48
ACTIVITY 28-1
  • Replace with Tee Model
  • L1 - M 2.5H j (L1 - M) j 50 ohms
  • L2 - M - .4 H j (L2 - M) - j 8 ohms
  • (Negative Inductances are not Uncommon when using
    the Tee Model)
  • M .5H j M j10 ohms
  • Put Back in Original Circuit
  • Be Careful!!

49
ACTIVITY 28-1
i2
i1
50
ACTIVITY 28-1
I2
I1
51
ACTIVITY 28-1
52
ACTIVITY 28-1
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