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Aspects of VR-LRC use @

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Aspects of VR-LRC use _at_ 'Transilvania' University in cooperation with Siemens PSE ... One can notice that closer to UGS = -0,3V asymptotic trend isn't obvious ... – PowerPoint PPT presentation

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Title: Aspects of VR-LRC use @


1
  • Aspects of VR-LRC use _at_ Transilvania University
    in cooperation with Siemens PSE
  • - practical guide for remote measurement (real
    and simulated)
  • of n-channel junction field effect transistors -
  • Florin SANDU
    Szilard CSEREY
  • Individualized Learning Enhanced by Virtual
    Reality IDENTITY
  • Agreement number 229930-CP-1-2006-1-RO-MINERVA-M
    Contractual Authority EU Education Audiovisual
    and Culture Executive Agency

2
  • Data sheet for the transistor used

3
STEP 1 Selecting NJFET measurement
  • Accessing the remote lab

The address for measurements and data
sheets http//vlab.unitbv.ro/velab/
4
  • STEP 2 Selecting the browser ( /mobile
    alternative )
  • For a normal browser one can choose the second
    option ( / the measurement can also be done with
    a JavaScript enabled mobile phone by selecting
    the third option)

5
  • STEP 3 Selecting the experiment
  • The page displays several options for
    measurement,
  • from which it was chosen the one for NJFET

6
  • STEP 4 Entering the stimuli
  • After entering the stimuli values in the text
    boxes, if you push the Measure button you will
    obtain the results both from the PSpice
    simulation and the real remote measurement done
    in the Lab.

7
  • STEP 5 Retrieving experimental data
  • After waiting about 15 seconds the result file
    will be printed on the page.

8
  • The .xls version of the results

UGS UDS U2 ID
-3.00E-01 0.00E00 0.00E00 0
-3.00E-01 9.77E-03 5.00E-01 8.75419E-05
-3.00E-01 1.95E-02 1.00E00 0.000175084
-3.00E-01 2.44E-02 1.50E00 0.000263497
-3.00E-01 3.42E-02 2.00E00 0.000351039
-3.00E-01 4.39E-02 2.50E00 0.000438581
-3.00E-01 5.37E-02 3.00E00 0.000526123
-3.00E-01 6.84E-02 3.50E00 0.000612793
-3.00E-01 7.81E-02 4.00E00 0.000700335
-3.00E-01 9.28E-02 4.50E00 0.000787005
-3.00E-01 1.07E-01 5.00E00 0.000873675
-3.00E-01 1.27E-01 5.50E00 0.000959473
Using .xls file you can make your own XLS charts
from measured data
9
  • Comparison between the data sheet and the .xls
    sample
  • We are going to use this example

10
Static Characteristics
DATA SHEET
MEASURED
Obs. Breakdown voltage -0.5V
  • UGS -0,3V -0,4V -0,5V -0,6V
  • One can notice that closer to UGS -0,3V
    asymptotic trend isn't obvious
  • Closer to UGS -0,7V, smaller current values
    are more affected by discretization errors

11
This measurement is intended to find the point of
convergence of the ID(UDS) asymptotes (for
constant UGS)
DATA SHEET
MEASURED
UGS -0.4 -0.42 -0.44 and -0.46V  
12
  • For UGS -0.42 -0.44 and -0.46V, only (three
    sets of) points to the right were chosen and
    "trend lines" determined
  • From the equation y mxn, the ration -n/m gave
    3 estimates of the convergence point, approx. (0
    - 43,7V)

UGS -0.42V n 0.000345213316 m
0.000008205356 U(convergence) -n/m
-42.07170487 UGS -0.44V n
0.00024277885 m 0.00000557362
U(convergence) -n/m -43.55855799 UGS
-0.46V n 0.00016389815 m 0.00000373679
U(convergence) -n/m -43.86067989
13
Breakdown voltage
Up(aprox.) - 0.0304 / ( 2 0.0287 ) -0.52962
14
m 0.1466 n 0.0816
Up -n/m -0.55662
15
  • Multiple VD measurement with fixed U2 , (max)
    10V (that grants SATURATION)

16
Multiple VD measurement with fixed U2 , (max)
10V (that grants SATURATION)
Limit line 10V / 9,8kW 1,02 mA
17
Multiple VD measurement with fixed U2 , (max)
10V (that grants SATURATION)
Limit line 10V / 9,8kW 1,02 mA
Parabolic ID, saturated (UGS)
18
Multiple VD measurement with fixed U2 , (max)
10V (that grants SATURATION)
Limit line SQRT(1,02)
Linear SQRT( ID, saturated ) (UGS)
19
Multiple VD measurement with fixed U2 , (max)
10V (that grants SATURATION)
SQRT( IDSS) 0,072 IDSS 5,1 mA
Parameters check on measured values close to
UGS,bias -0,3V
UP - 0,46 V
SMALL SIGNAL PARAMETER computed in UGS,bias
-0,3V
20
  • Multiple VD measurement ( VG - 0,1V -
    0,2V - 0,3V - 0,4V ) ( U2 0V 0,5 V
    9,5V )

2nd SMALL SIGNAL PARAMETER measured in UGS,bias
-0,3V rd 56,7 kW

21
Multiple VD measurement ( VG - 0,295V -
0,3V - 0,305V ) ( U2 8,5V )
The result , respectively, VD 2,87V
3,225V 3,567V MEASURED gain, Au (
3,567V 2,87V ) / 0,305V ( 0,295V )
69,7
On the SMALL SIGNAL EQUIVALENT CIRCUIT it
results COMPUTED gain, Au 8,44mS . ( 9,8 kW
II 56,7 kW ) 70,5
22
  • Comparison to PSpice simulation

23
Comparison to PSpice simulation
24
Comparison to PSpice simulation
25
Determining UP and IDSS using graphical methods
(1)
  • Comparison to MatLab simulation
  • Using continuous current measurements of VD, ID
    can be obtained by a simple calculus
    ID(E-VD)/9.8kO
  • IDSS is equal to ID when VG0
  • UP represents the gate source cut-off voltage
    (for lower Drain voltages ID0)
  • Both IDSS and UP values are determined through
    graphical methods (use of cubic spline
    interpolation)
  • The obtained (NOT measured) values are
  • UP 0.4998 V and IDSS 1.0179 mA (for
    VSupply10 V)

26
Determining UP and IDSS using graphical methods
(2)
Measured UGS values - Interpolation Curve
27
Alternating current calculus and measurements
  • The alternating current input signal is simulated
    through symmetrical variations of UGS around a
    given value (in this case -0.3 V with 0.05 V
    variation margin)
  • VD is measured several times for a more accurate
    value in all three cases (UGS -0.295 V , -0.3 V
    and -0,305 V)
  • The first voltage gain is obtained using the
    following formula

28
Alternating current calculus and measurements
  • In order to be able to calculate the theoretical
    gain, gm must be determined. This is done by
    finding the slope of ID(UGS) using mathematical
    analysis. Thus,

Because ID(UGS) is obtained by measurements
(later points being approximated), it is not
possible to calculate a lime. Therefore
discrete values are given to ?V and then , by
gradually reducing it down to 0.
29
Alternating current calculus and measurements
The resulted value of gm is around 6.7 mS.
30
Alternating current calculus and measurements
  • The theoretical gain is AU2 -gmR -6.7 mS 9.8
    kO -65.66 (rd ? 8)
  • Compared to AU1, this value is smaller due to
    approximations in later calculus (like gm).
  • Note All the graphical representations have been
    plotted in Matlab 5.2
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