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Darryl Michael/GE CRD Fields and Waves Lesson 1.2 SINE WAVES ON TRANSMISSION LINES.

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Presentation on theme: "Darryl Michael/GE CRD Fields and Waves Lesson 1.2 SINE WAVES ON TRANSMISSION LINES."— Presentation transcript:

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2 Darryl Michael/GE CRD Fields and Waves Lesson 1.2 SINE WAVES ON TRANSMISSION LINES

3 Standing Wave Patterns Today’s Class: look at effects of Sine Waves on Transmission Lines generate Standing Wave Patterns - predict these when load is mismatched waves sent down the line are reflected incident and reflected waves interfere constructively and destructively standing wave occurs

4 Transmission Lines Incident Wave Reflected Wave Mismatched load Standing wave due to interference Do Experiment 1a, b and c

5 Transmission Lines - Standing Wave Derivation Phasor Form of the Wave Equation: where: General Solution:

6 Transmission Lines - Standing Wave Derivation Forward Wave Backward Wave V max occurs when Forward and Backward Waves are in Phase V min occurs when Forward and Backward Waves are out of Phase CONSTRUCTIVE INTERFERENCE DESTRUCTIVE INTERFERENCE TIME DOMAIN Do Problem 1a

7 Transmission Lines - Standing Wave Derivation Distance between Max and Min is /2 Assume, are real for the moment (will be complex if load is complex Forward Phase is = Backward Phase is = Difference in Phase is = Varies by 2  (distance between maxima) Show this

8 Reflection Coefficient Derivation Define the Reflection Coefficient: Maximum Amplitude when in Phase: Similarly: Standing Wave Ratio (SWR) =

9 Reflection Coefficient Derivation Let z=0 at the LOAD Need a relationship between current and voltage:

10 Reflection Coefficient Derivation

11 At LOAD: Use derived terms of V and I at z=0 (position of the LOAD) OR Note that

12 Standing Wave Pattern Do Problem 1a - 1c From experiment 1b, Maximum occurs at LOAD for Minimum occurs at LOAD for In general, Max at LOAD Min at LOAD IF Z L is REAL

13 Standing Wave Pattern Do Experiment 2 What does, look like? When Z L is complex, so is  L Define: if z =0 at LOAD

14 Standing Wave Pattern If z=L at LOAD and z=0 at SOURCE, When Phase = , FIRST MINIMUM occurs Other MINs are displaced by /2


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