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Physics 401, Fall 2016. Eugene V. Colla

Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

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Page 1: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

Physics 401, Fall 2016.Eugene V. Colla

Page 2: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

• Transients. Definition.

• Transients in RLC

• Resonance in RLC

• Data analysis. Origin. Fitting.

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Page 3: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

3

Page 4: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

transient ( physics ) a short-lived oscillation in a

system caused by a sudden change of voltage or

current or load

a transient response or natural response is the

response of a system to a change from equilibrium.

System under

study

4

Page 5: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

R

L

C

Vscope

Resistance R [Ohm]

Capacitance C [mF] (10-6F)

Inductance L [mH] (10-3H)

5

Page 6: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

R

L

C

V(t)scope

VR VL

VC

According the Kirchhoff’s law VR+VL+VC=V(t)

-1.0 -0.5 0.0 0.5 1.00.0

0.5

1.0

V(t

)

time

V0

2

2

d d q(t)L q(t) +R q(t) + = 0

dt dt C*See Lab write-up for details

*

(1)

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Page 7: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

The solution of this differential

equation can be found in the form ( ) est

q t A

This will convert (1) in

quadratic equation

Rs s

L LC

21

0

,

,

R Rs a b

L L LC

R Ra b

L L LC

2

1 2

2

1

2 2

1

2 2

with solutions:

b2>0 over-damped solution

b2=0 critically damped solution

b2<0 under-damped solution

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Page 8: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

b2>0

( ) e at bt bt

q t A e B e1 1

In this case the solution will be aperiodic

exponential decay function with no

oscillations:

( ) ( ) ( )at bt bt at bt btdq

i t ae A e B e be A e B e

dt1 1 1 1

8

2 2 40

Lb R

C

Page 9: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

Taken in account the initial conditions: q(0)=q0 and i(0)=0

( ) cosh sinhat

aq t q e bt bt

b0

( )( ) a b tq a b

i t e

b

2 2

0

2

This is exponential decay function

-( - )

( - )

a b t

a b t

q ae

b

0

11

2

9

b2>0

Page 10: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

b2=0

For this case the general solution can be found as

q(t)=(A2+B2t)e-at. Applying the same initial condition

the current can be written as i=–a2q0te-at

Critical damped case shows the

fastest decay with no oscillations

2 2 40

Lb R

C

Critically-damped

conditions for our

network2

Ra

Land

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Page 11: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

b2=0

In this experiment R=300 ohms,

C=1mF, L=33.43mH.

The output resistance of Wavetek is 50 ohms and

resistance of coil was measured as 8.7 ohms, so actual

resistance of the network is Ra=300+50+8.7=358.7

Decay coefficient 𝒂 =𝑹

𝟐𝑳=

𝟑𝟓𝟖.𝟕

𝟐∗𝟑𝟑.𝟒𝟑𝑬−𝟑≈ 𝟓𝟑𝟔𝟓

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Page 12: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

Now the experimental results:

Calculated decay

coefficient ~5385,

Obtained from fitting -

~5820.

Possible reason – it is

still slightly over damped

Calculated b2 is

b2=2.99e7-2.90e7>0

Vc ~q, fiiting function: Vc=Vco(1+at)e-at

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b2=0

Page 13: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

If b2<0 we will have oscillating solution. Omitting the details (see

Lab write-up) we have the equations for charge and current as:

,

cos sin sin( )

sin

;

at at

at

a aq(t) q e bt bt q e bt

b b

a bi(t) q e bt

b

R R Ra b f

L L LC LC L

2

0 0 2

2 2

0

2 2

1

1 1 1

2 2 2 2

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Page 14: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

Log decrement can be defined as 𝜹 = 𝒍𝒏𝒒(𝒕𝒎𝒂𝒙

𝒒(𝒕𝒎𝒂𝒙+𝑻𝟏)=

𝒍𝒏𝒆−𝒂𝒕𝒎𝒂𝒙

𝒆−𝒂(𝒕𝒎𝒂𝒙+𝑻𝟏)= 𝒂𝑻𝟏, where T1=1/f1

Quality factor can be

defined as 𝑸 = 𝟐𝝅𝑬

∆𝑬,

For RLC 𝑸 =𝝎𝟏𝑳

𝑹=

𝝅

𝜹

From this plot d≈0.67

Q≈4.7 -1 0 1 2 3 4 5 6 7 8 9 10

-6

-3

0

3

6

3.529

1.809

0.929620.47494

VC (

q/C

) (V

)

time (ms)

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Page 15: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

1. Pick peaks

2. Envelope

3. Nonlinear fitting-1 0 1 2 3 4 5 6 7 8 9 10

-6

-3

0

3

6

0.00115

0.0023

0.003460.00463

VC (

q/C

) (V

)

time (ms)

f=862Hz

-1 0 1 2 3 4 5 6 7 8 9 10-6

-3

0

3

6

VC (

q/C

) (V

)

time (ms)

f=862Hz

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Page 16: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

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Page 17: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

Time domain trace

Points found using “Find peaks”

Envelope curve

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Page 18: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

Fitting the “envelope data” to

exponential decay function

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Page 19: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

Zero crossing points

0ffsetManual evaluation of the

period of the oscillations

in( )at

q(t) Ae s t offset

Limited accuracy

Results can be

effected by DC offset

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Page 20: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

C

in( )

( )U

at

q(t) Ae s t

q t

C

Use Origin standard

function

Category: Waveform

Function: SineDamp

Fitting function ; y0,A,t0 xc, w – fitting parameters

From fitting you can get: and

20

at

0

1T w

f

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Page 21: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

in( )at

q(t) Ae s t

Limited

Data plot + fitting curve

Residuals - criteria

of quality of fitting

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Page 22: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

in( )at

q(t) Ae s t

Final results

Rf

T LC L

2 2

21 1 1

2 2

22

Page 23: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

R2

L

C

VCV(t)

100 1000 100000

2

4

6

8

10

12

14 1904.83204

UC

f (Hz)

f=1500Hz

𝑸 =𝒇

𝜟𝒇=𝟏𝟗𝟎𝟒

𝟏𝟓𝟎𝟎= 𝟏. 𝟐𝟔

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Page 24: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

Open template

button

\\engr-file-03\phyinst\APL Courses\PHYCS401\Common\Origin templates

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Page 25: Physics 401, Fall 2016....Physics 401, Fall 2016. Eugene V. Colla • Transients. Definition. • Transients in RLC • Resonance in RLC • Data analysis. Origin. Fitting. 2 3 transient

Very short and simple manual which covers

only main general operations with Origin.

Document located on server and there is a

link from P401 WEB page

There are also manuals from OriginLab.

Video Tutorials at the

site of the company

http://www.originlab.com/index.aspx?go=SUPPORT/VideoTutorials

Do not forget about

Origin Help

\\engr-file-03\phyinst\APL Courses\PHYCS401\Common\Origin manuals

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