labactivity2gggggggggawdsaaaveusall
TRANSCRIPT
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
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ECE 126
Introduction to Analog Integrated Circuits Design
Lab 2: Common Source Amplifer with
Resistor Load and Source Degeneration
Submitted by:
Ceferino Kevin A. Tan
BSECE 4
Submitted to:
rof. Allenn dela Cerna !o"aton
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
Step 1:
*ollo"ing t+e circuit of ,gure 4.(& simulate t+e -in-outDC transfer curve as it "as obtained in ,gure 4.$ and
t+e fre/uency res#onse as in ,gure 4.0.
Relation o !inand !out
C"DE
ste#(a1tan
.lib 2C:3syno#sys3rf'(.l2
TT
m( vout g gnd gnd nc+
l5'.(u "5'.6u
vdd vdd gnd (.v
vin g gnd '.%v
r( vout vdd ('7cload vout gnd ('#
.o#
.o#tion #ost #robe
.dc vin ' $ '.'(
.#robe v8vout9
.end
#"$ "utput
subc7t
element ':m(
model ':nc+.($region Saturati
id 00.'$'u
ibs .6(e$(
ibd 0.$44'n
vgs %''.''''m
vds (.46
vbs '.
vt+ )0.$00m
vdsat (0.%$m
vod (6'.%'6%m
beta (.(%m
gam e; 6.4%64m gm $4).$0)u
%igure 1T+e -in-outgra#+ s+o"s +o" t+e out#ut voltage8ya
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
%re&uenc' Response
C"DE
ste#(b1tan
.lib 2C:3syno#sys3rf'(.l2 TT
m( vout vin gnd gnd nc+ l5'.(u
"5'.6u
vdd vdd gnd (.v
vin vin vg ac (
vg vg gnd '.%
r( vout vdd ('7
cload vout gnd ('#
.o#
.#robe v8vout9
.o#tion #ost #robe
.#lot ac vdb8vout9
.ac dec ('' (' ('g.meas ac >B "+en vdb8vout9 5 '
.alter
vg vg gnd '.4
.alter
vg vg gnd (
.alter
vg vg gnd (.)
.end
%igure 2T+e gainfre/uency res#onse gra#+. At t+e bias #oint -inDC5'.%-& t+e DC
gain of t+e circuit is 0.$$(6 dB. *rom to# to bottom& t+e >ainBand"idt+s are:4.066(?@=&0.)(66?@=& A& A.
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
Step 2:
C+ange t+e value of in ,gure 4.( and simulate t+e resulting "aveforms of ,gure
4.4& t+en list t+e results as in table 4.( and com#are t+em "it+ +and calculation
results.
C"DESte#$1tan
.lib 2C:3syno#sys3rf'(.l2
TT
m( vout vin gnd gnd
nc+ l5'.(u "5'.6u
vdd vdd gnd (.v
vin vin vg ac (
vg vg gnd '.%
r( vout vdd $'7
cload vout gnd ('#
.o#
.#robe v8vout9
.o#tion #ost #robe
.#lot ac vdb8vout9
.ac dec ('' (' ('g
.meas ac >B "+en
vdb8vout9 5 '
.alter
vg vg gnd .4r( vout vdd (7
.alter
vg vg gnd (
r( vout vdd ($7
.alter
vg vg gnd (.)
r( vout vdd 0'7
.end
#"$ "utput
subc7t
element ':m(
model
':nc+.($
region
Saturati
id
0(.$$0u
ibs .$'e$(
ibd
$'0.'''#
vgs
%''.''''m
vds
(.(%))
vbs '.
vt+
)4'.($6m vdsat
(0.)(6(m
vod
().%(4m
beta
(.(%m
gam e;
6.4%)m
gm
$0%.')6u
gds
6.$%0u
gmb
66.6%0$u
cdtot
%4.%((a cgtot
(.'4$'f
cstot
(.))f
cbtot
(.46)f
cgs
%$'.(%(a
cgd
$(6.6$')a
subc7t
element ':m(
model
':nc+.($
region
Cuto;
id
4).'6n
ibs (.$'e
$$
ibd
4%'.'$('#
vgs
4''.''''m vds
(.%(%
vbs '.
vt+
)0.0)%(m
vdsat
4).%$06m
vod
(0.0)%(m
beta(.0(m
gam e;
6.46%m
gm
('.(%0)u
gds
(6%.4$$n
gmb
$.)()u
cdtot
%'4.'6%a
cgtot
66%.)(4$a
cstot
)0.46)6a cbtot
(.404f
cgs
$$).)a
cgd
$(%.60a
subc7t
element ':m(model
':nc+.($
region
Saturati
id
(').%%u
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
ibs $.%%4e
$'
ibd
0.''%0a
vgs
(.''''vds
)$.4))0m
vbs '.
vt+
)4$.'()$m
vdsat
$)(.)0(0m
vod
4)%.4m
beta
(.)0m
gam e;
6.4)6m
gm
$.('6)u
gds
0$.')$u
gmb
4.$''u
cdtot
$.6$6'a cgtot
(.'%46f
cstot
(.)6f
cbtot
(.)6%)f
cgs
%66.$$a
cgd
$(.6$0a
subc7t
element ':m(
model
':nc+.($
region
!inear
id
).'')%u
ibs (.)$0e
$' ibd
$.6(a
vgs
(.)'''
vds
).$0m
vbs '.
vt+
)40.0()m
vdsat
0).$6m
vod
)6.6()m
beta
(.66)m
gam e;
6.40'm
gm
0%.()'4u
gds
%.'40u gmb
().04)4u
cdtot
(.)%4f
cgtot
(.$$)'f
cstot
(.%6)f
cbtot
(.%'0'f
cgs
)).''0'a
cgd
)(.(%(a
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
%igure (AC analysis "it+ di;erent values of (. otice t+at t+e curve for "+en
-g5'.%v and 5$'7 no" +as t+e +ig+est gain& but #ractically still +as a smaller >.B.
t+an for -g5(v and 5($7.
(879 out879 -g8-9A 8>ain in
dB90dB 8@=9 >.B. 8@=9
$'70.40$(6
4('.% ($.) (7 0.66$%?
(7 A '.4 (4. A A
($7$.64%4
40( %.$ (.4? 4.$'?
0'7 A (.) $%. A A
)able 1S+o"s t+e c+ange in gain and >B for "+en t+e resistance (and t+e in#ut
voltage -gis varied.
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
*and Calculations or step 2
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
Step (:
*ollo"ing t+e circuit of ,gure 4.)& simulate t+e -in
-outDC transfer curve as in ,gure 4.6 and t+e
fre/uency res#onse as in ,gure 4.%.
Relation o !inand !out
C"DE
ste#0a1tan
.lib 2C:3syno#sys3rf'(.l2
TT
m( vout g vs vs nc+
l5'.(u "5'.6u
vdd vdd gnd (.v
vin g gnd '.6v
r( vout vdd ('7
r$ vs gnd ('7
cload vout gnd ('#
.o#
.o#tion #ost #robe
.dc vin ' $ '.'(
.#robe v8vout9
.end
#"$ Result
subc7t
element ':m(
model ':nc+.($
region Saturati
id 6.'''u
ibs (.)(e$(
ibd 0.$'$%n
vgs )0.$m
vds (.6%
vbs '.
vt+ )0.6%m
vdsat %$.(04(m
vod (.$'0m
beta (.040m
gam e; 6.460m
gm '.440(u
gds (.%4$)u
gmb $).(6)u
%igure +-in-outDC c+aracteristic curve for CS "it+ source degeneration. ote t+at
"e +ave a muc+ smaller slo#e magnitude at t+e saturation region.
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
10/28
Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
%re&uenc' Response
C"DE
ste#0b1tan
.lib 2C:3syno#sys3rf'(.l2
TT
m( vout vg vs vs nc+
l5'.(u
"5'.6u
vdd vdd gnd (.v
vin vin gnd ac (
vg vg vin '.%
r( vout vdd ('7
r$ vs gnd (7
cload vout gnd ('#
.o#
.#robe v8vout9
.o#tion #ost #robe
.#lot ac vdb8vout9
.ac dec ('' (' ('g
.meas ac >B "+en
vdb8vout9 5 '
.end
#"$ Result
subc7t
element ':m(
model ':nc+.($
region Saturati
id $6.%)6u
ibs %.'6%e$(
ibd 0.66)4n
vgs 6%0.($'%m vds (.)'40
vbs '.
vt+ )0.(('m
vdsat ($%.((m
vod (00.$%m
beta (.$(%m
gam e; 6.4%4m
gm $$6.(4')u
gds ).$4%u
gmb 6$.)4u
gb5 $.4'4'E'6
%igure ,AC analysis of CS am#li,er "it+ source degeneration. lacing a source
resistance of (7 +as resulted in a ne" DC gain of 4.(dB. Fur >.B. value8+ig+lig+ted
above9 is given by $.4'4'?@=.
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
11/28
Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
Step +:
C+ange t+e value of sin ,gure 4.) and simulate t+e resulting "aveforms of ,gure
4.G list t+e results as in table 4.$. T+en& com#are t+em "it+ +and calculation
results.
C"DE
Ste#41tan
.lib 2C:3syno#sys3rf'(.l2
TT
m( vout vg vs vs nc+
l5'.(u
"5'.6u
vdd vdd gnd (.vvin vin gnd ac (
vg vg vin '.%
r( vout vdd ('7
r$ vs gnd )''
cload vout gnd ('#
.o#
.#robe v8vout9
.o#tion #ost #robe
.#lot ac vdb8vout9
.ac dec ('' (' ('g
.meas ac >B "+en
vdb8vout9 5 '
.alter
vg vg vin '.
r$ vs gnd (.)7
.alter
vg vg vin '.6
r$ vs gnd $7
.end
#"$ Results
subc7t
element ':m(
model ':nc+.($
region Saturati
id $.)(6u
ibs %.%%e$(
ibd 0.)'0n vgs 6).$'%4m
vds (.44
vbs '.
vt+ )0.$0)0m
vdsat (00.0($m
vod (4).%$(m
beta (.$''m
gam e; 6.4%))m
gm $0).$$$0u
gds ).)(%u gmb 6).0($u
cdtot %$0.%'$a
cgtot (.'0%f
cstot (.))0'f
cbtot (.4%(%f
cgs %(4.'$'6a
cgd $(6.6(6a
subc7t
element ':m(
model ':nc+.($
region Saturati
id 4(.6((u
ibs (.'4e$' ibd (.')'n
vgs %0%.)%(0m
vds (.0$(4
vbs '.
vt+ )0.%$'%m
vdsat ()6.'0((m
vod (%.)'6m
beta (.((m
gam e; 6.4%6m
gm $60.0)u gds %.(')u
gmb %0.6()%u
cdtot %06.)00'a
cgtot (.')''f
cstot (.)6f
cbtot (.406f
cgs %0'.46'a
cgd $(6.)6a
subc7t
element ':m(
model ':nc+.($
region Saturati
id ('.0('u ibs $.%04e$(
ibd ).'(%n
vgs )%.$'%m
vds (.6%)$
vbs '.
vt+ )0.64)m
vdsat 6.$'m
vod 4'.)(04m
beta (.0(%m
gam e; 6.4%'4m gm (00.6(u
gds $.666u
gmb 0%.()46u
cdtot %((.0'6a
cgtot 00.(0()a
cstot (.0%'f
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
cbtot (.4)60f cgs )%.'0%)a cgd $(6.'(a
%igure 6AC analysis of a CS am#li,er "it+ source degeneration: -arying source
resistance s. 8To# to bottom9 H 8-g&s9: 8'.%&)'' 9&8'.&()'' 9&8'.6&$'''9.
$879 -g8-9 out879A 8>ain in
dB90dB 8@=9 >.B. 8@=9
'.) '.%).0'$60$
6.'( (.6%? $.((?
(.) '.%.$(60')$
).'$ (.6%? $.466%?
$ '.6 ($.'$)(0$$ '.$)4 (.6$? '.0?
)able 2s+o"s t+e variation of t+e gain& cuto; fre/uency& and >.B. "+en value of s
is c+anged. T+e value of outis not c+anged even "it+ t+e addition of a source
resistance s8+tt#:"+ites.sdsmt.educlassesee0$'notes0$'!ecture0$.#df9. See
t+at t+e cuto; fre/uency does not c+ange even "+en t+e gain does.
ou can see t+at +aving a source resistance "ill result in a very little di;erence in
cuto; fre/uencies for all curves.
Addition of a source resistance "ill result in a lo"ering of -gs"it+ res#ect to -i. Also&
t+is "ill result in a lo"ering of t+e smallsignal voltage gain as can be seen in t+e ;:
Av=gmRD
1+gmRs
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
Des#ite t+ese dra"bac7s& t+e source
resistanceJs maor bene,t is t+at t+e small
signal voltage gain "ill be made muc+ less
de#endent on t+e ?FS*ET transconductance.
ote t+at for CS "it+ S.D.& t+e out#utim#edance is given by t+e e/uations to t+e
rig+t:
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
*and Calculations or step +
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
15/28
Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
Step ,:
C+ange t+e value of sin ,gure 4.)& and simulate t+e "aveforms of ,gure 4.(' to
observe t+e relations+i# bet"een Idsand -in.
C"DE
ste#)1tan
.lib 2C:3syno#sys3rf'(.l2
TT
m( vout vg vs vs nc+
l5'.(u "5'.6u
vdd vdd gnd (.v
vin vin gnd ac (
vg vg vin '.%
r( vout vdd ('7
r$ vs gnd )''
cload vout gnd ('#
.o#
.o#tion #ost #robe
.dc vg ' (. '.'(
.#robe i(8m(9
.alter
r$ vs gnd (7
.alter
r$ vs gnd (.)7
.alter
r$ vs gnd '7
.end
#"$ Results
subc7t
element ':m(
model
':nc+.($
region
Saturati
id
$.)(6u
ibs %.%%e
$( ibd
0.)'0n
vgs
6).$'%4m
vds
(.44
vbs '.
vt+
)0.$0)0m
vdsat(00.0($m
vod
(4).%$(m
beta
(.$''m
gam e;
6.4%))m
gm
$0).$$$0u
gds
).)(%u
gmb
6).0($u
cdtot
%$0.%'$a
cgtot(.'0%f
cstot
(.))0'f
cbtot
(.4%(%f
cgs
%(4.'$'6a
cgd
$(6.6(6a
subc7t
element ':m(
model
':nc+.($
region
Saturati
id
$6.%)6u
ibs %.'6%e
$(
ibd
0.66)4n
vgs
6%0.($'%m
vds
(.)'40
vbs '.vt+
)0.(('m
vdsat
($%.((m
vod
(00.$%m
beta
(.$(%m
gam e;
6.4%4m gm
$$6.(4')u
gds
).$4%u
gmb
6$.)4u
cdtot
%$$.'40a
cgtot
(.'004f
cstot
(.)4%(f
cbtot
(.4%'%f
cgs
%'.$(((a
cgd$(6.60'%a
subc7t
element ':m(
model
':nc+.($
region
Saturati
id
$4.60(u ibs 6.4(e
$(
ibd
0.%)n
vgs
66$.6%m
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
vds
(.)(6(
vbs '.
vt+
)0.()6(m
vdsat($0.04%m
vod
($0.(06m
beta
(.$0'm
gam e;
6.4%4$m
gm
$(%.%)0u
gds
4.6)0u
gmb
6'.))0'u
cdtot
%$(.%$a
cgtot
(.'$f
cstot
(.)4('f cbtot
(.4%''f
cgs
%'$.04)0a
cgd
$(6.64$$a
subc7t
element ':m(
model
':nc+.($
region
Saturati
id
00.'$'u
ibs .6(e
$(
ibd
0.$44'n vgs
%''.''''m
vds
(.46
vbs '.
vt+
)0.$00m
vdsat
(0.%$m
vod
(6'.%'6%m
beta
(.(%m
gam e;
6.4%64m
gm
$4).$0)u
gds
).6$u gmb
6.$'((u
cdtot
%$).$')a
cgtot
(.'4$$f
cstot
(.))6f
cbtot
(.4%$f
cgs
%(.$'%a
cgd
$(6.6'0a
%igure -*rom to# to bottom are t+e curves for "+en t+e source resistance8in
F+ms9 is '& )''& ('''& ()''.
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
-ital e/uation >m5
1
( 1gm )+Rs for a CS am#li,er "it+ source degeneration. T+us&"+en "e increase s& "e decrease t+e slo#e of our Ids-gsgra#+& "+ic+ im#lies t+at
"e "ill #roduce a muc+ smaller out#ut current for a given in#ut DC voltage "+enour source resistance is increased. Since Av5>mD& Avis no" given by Av5
RD
( 1gm )+Rs .
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
Step 6:
*ollo"ing t+e am#li,er con,guration of ,gure
4.((& t+e in#ut signal is an ideal sinusoidal "ave
"it+ '.')v am#litude& and t+e fre/uency is
(''7@=. erform t+e **T analysis to - into get t+efre/uency s#ectrum li7e ,gure 4.($
C"DE
ste#61tan
.lib
2C:3syno#sys3rf'
(.l2 TT
m( vout vg vs
vs nc+ l5'.(u
"5'.6u
vdd vdd gnd (.
vin vin gnd
sin8' '.') (''7
' ' '9
vg vg vin '.%
r( vout vdd ('7
r$ vs gnd )''
cload vout gnd
('#
.o#
.o#tion #ost
#robe
.tran 6$)n
('.$4m
.;t v8vg9
start5'
sto#5('.$4m
n#5(604
.end
#"$ Results
subc7t
element ':m(
model
':nc+.($
region
Saturati
id
$.)(6u
ibs %.%%e
$(
ibd
0.)'0n
vgs
6).$'%4m
vds (.44
vbs '.
vt+
)0.$0)0m
vdsat
(00.0($m
vod
(4).%$(m
beta
(.$''m
gam e;
6.4%))m
gm
$0).$$$0u
gds
).)(%u
gmb
6).0($u
cdtot
%$0.%'$a
cgtot
(.'0%f
cstot
(.))0'f
cbtot
(.4%(%f
cgs
%(4.'$'6a
cgd
$(6.6(6a
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
%igure .*ast*ourier Transform of t+e -in. T+e result s+ould s+o" no +armonic
com#onent e
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
Step -:
erform t+e **T Analysis to -outin t+e circuit of ,gure 4.(( "+ile c+anging t+e value
of sto get t+e fre/uency s#ectrum li7e in ,gure 4.(0(6. !ist t+e results of ,gure
4.(0(6 li7e in table 4.0.
C"DE
Ste#%1tan
.lib
2C:3syno#sys3rf'
(.l2 TT
m( vout vg vs
vs nc+ l5'.(u
"5'.6u
vdd vdd gnd (.
vin vin gnd
sin8' '.') (''7
' ' '9
vg vg vin '.%
r( vout vdd ('7
r$ vs gnd '
cload vout gnd
('#
.o#
.o#tion #ost
#robe
.tran 6$)n
('.$4m
.;t v8vout9
start5'
sto#5('.$4m
n#5(604
.alter
r$ vs gnd )''
.alter
r$ vs gnd (7
.alter
r$ vs gnd (.)7
.end
#"$ Results
subc7t Rs/0
element ':m(
model
':nc+.($
region
Saturati
id
00.'$'u
ibs .6(e
$(
ibd
0.$44'n
vgs
%''.''''m
vds
(.46
vbs '.
vt+)0.$00m
vdsat
(0.%$m
vod
(6'.%'6%m
beta
(.(%m
gam e;
6.4%64m
gm
$4).$0)u
gds
).6$u
gmb
6.$'((u cdtot
%$).$')a
cgtot
(.'4$$f
cstot
(.))6f
cbtot
(.4%$f
cgs
%(.$'%a cgd
$(6.6'0a
subc7t
Rs/,00
element ':m(
model
':nc+.($
region
Saturati
id
$.)(6u
ibs %.%%e
$(
ibd0.)'0n
vgs
6).$'%4m
vds
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vbs '.
vt+
)0.$0)0m
vdsat
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(4).%$(m
beta
(.$''m
gam e;
6.4%))m
gm
$0).$$$0u
gds
).)(%u
gmb
6).0($u
cdtot
%$0.%'$a
cgtot
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cgs
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cgd
$(6.6(6a
subc7t
Rs/1000
element ':m(
model
':nc+.($
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
region
Saturati
id
$6.%)6u
ibs %.'6%e
$( ibd
0.66)4n
vgs
6%0.($'%m
vds
(.)'40
vbs '.
vt+
)0.(('m
vdsat
($%.((m
vod
(00.$%m
beta
(.$(%m
gam e;
6.4%4m
gm
$$6.(4')u
gds
).$4%u
gmb
6$.)4u cdtot
%$$.'40a
cgtot
(.'004f
cstot
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cbtot
(.4%'%f
cgs
%'.$(((a
cgd
$(6.60'%a
subc7t
Rs/1,00
element ':m(
model
':nc+.($
region
Saturati
id$4.60(u
ibs 6.4(e
$(
ibd
0.%)n
vgs
66$.6%m
vds
(.)(6(
vbs '.
vt+
)0.()6(m
vdsat
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vod
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beta
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gam e;
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gm
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6'.))0'u
cdtot
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cgtot
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cstot
(.)4('f
cbtot
(.4%''f
cgs
%'$.04)0a
cgd
$(6.64$$a
%%) Anal'sis o !outwithout Rs
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
22/28
Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
%igure L+en s5'& t+e gain for t+e (st& $nd& and 0rd@armonics are $$.$'dB&
)0.('dB& %).'dB.
%%) Anal'sis o !outwith Rs/0#,
%igure 10 L+en s5)''& t+e gain for t+e (st& $nd& and 0rd@armonics are $0.6'dB&
)).('dB& '.'dB.
%%) Anal'sis o !outwith Rs/1
-
7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
23/28
Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
%igure 11L+en s5('''& t+e gain for t+e (st& $nd& and 0rd@armonics are $4.'dB&
)6.%'dB& (.('dB.
%%) Anal'sis o !outwith Rs/1#,
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
24/28
Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
%igure 12L+en s5()''& t+e gain for t+e (st& $nd& and 0rd@armonics are H$6.''dB&
).('dB& (.)'dB.
s879 -inDC8-9 -inAC8-9 A8dB9 -out8dB9
$nd
@armonic
8dB9
0rd
@armonic
8dB9
'
'.% '.')
%.$ $$.$' )0.(' %).'
'.)'' 6.'( $0.6' )).(' '.'
( 4.' $4.' )6.%' (.('
(.) 0.4 $6.'' ).(' (.)'
)able (S+o"s +o" t+e gains for t+e (st& $nd& and 0rd+armonics c+ange "+en t+e
value of sis c+anged. >enerally& increasing t+e svalue "ill result in t+e gains for
t+e $nd
and 0rd
+armonics to a##roac+ some common value.
34ES)5"S
(. @o" to increase t+e gain of CS am#li,er "it+ resistive loadM E
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
25/28
Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
ote t+at increasing t+e L! ratio increases t+e slo#e of t+e Ids-dsgra#+ of
our n?FS 8as observed in t+e #revious lab activity9. T+erefore& "e increase
gmalong "it+ it& conse/uently& "e get a muc+ +ig+er gain magnitude.
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
26/28
Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
$. e#lace sin ,gure 4.(( "it+ a diodeconnected n?FS. Nsing t+e ste#s "e
follo"ed before& "+at is t+e DC gain of t+is circuitM
%igure 1(T+e DC gain for t+e net"or7 "it+ a diodeconnected n?FS8of t+e
same as#ect ratio as main n?FS9 is no" 0.%'dB.
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7/25/2019 LabActivity2GGGGGGGGGAWDSAAAVEUSALL
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
0. Nsing t+e con,guration of /uestion $& #erform t+e **T Analysis of -inand -out
to get t+e fre/uency s#ectrum of t+ese "aves. L+at +a##ens to t+e circuit
linearityM Is t+ere any di;erence "it+ ,gure 4.((M
%%) o !in
%igure 1+ote t+at for t+e **T of t+e in#ut voltage& "e see no signi,cant
di;erence com#ared to t+e net"or7 "it+ source resistance instead of t+e
diodeconnected n?FS in t+e source.
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Ceferino Kevin A. Tan BSECE 4 Se#tember $%& $'()
%%) o !out
%igure 1, ote t+at for t+e **T of t+e out#ut voltage -out& "e "e see no
signi,cant di;erence com#ared to t+e net"or7 "it+ source resistance instead
of t+e diodeconnected n?FS in t+e source.