EE114_HW1_Solution

EE114_HW1_Solution - BEIN— Auf 08/06 z< Salmon to...

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Unformatted text preview: BEIN— Auf 08/06] z< Salmon to HW #1 >> 1. Accorfihnj to s‘thlcz Ionj channel macleis ; ._ K °1 ID “ 7:2" (V66— Vt) cl) - ‘ W Where K 15 “Cox 3 VGS1=I5V » ID': 200 “A VC‘SQ: 1 V >§ ID; = I ' ‘9 ID: ___ (Vqs.——- V17) MN 9. D‘; QVG‘SQH VT) SubgthMtknj ' tke numbers Ur = U 5 —* Vt W k‘ W Cl'uvcn U3 0”“; V515 — I01 I 200 — JE— (15~O-$)R HA '- R EE114 HW#1 Solution Analog Integrated Circuit Design September 25, 2008 Problem 2 Textbook Problem 2.18: SIS FIE (a)S (b) Solution 1: We will study the given structure as a three-terminal device and consider its behavior under dif— ferent bias conditions: 1. VGS < Vt: Obviously, in this case both devices are off and there is no current flowing from source to drain, therefore, the behaviors of both structures are the same. 2. VGS > Vt and VDS < VGS — Vt: it is straightforward to show that given these conditions both transistors will be in triode region. M1 is on and has to be in triode. M2 cannot be off because if M2 is off the current through M1 must be zero, which means that V1351 is zero (remember that M1 is on.). ' If V1331 is zero then VGS2 would be equal to Vasl, and therefore our initial assumption that VG52 is smaller that Vt is invalid. Now that we know both transistors are in triode, we have: W . i v2 11 = uncomL—1((Vas - vavpm — 13231) (*) W V2 12 = #nComL—Z ((VGS — VDSI *- Vt)VDS2 # 13252) we also have: i I1 = 12 = I and VDS = VDSl + VDS2 thus: W V — V 2 I = MnCoxL— ((VG'S' * VDSl - Vt)(VDs — V1351) — (BS—212$) 2 W V2 V2 = ,unCom_((VGS — Vt)VDS - ~Q§ -VD51(VGS — Vt) + D51) L2 2 2 \_._____\,._—/ From = —W—”nC:;L_1 Simplifying this equation a little bit we get: L1 _ W V53 [(1 + 13—2) - MnCoz—i; ((VGS — Vt)VDS — T) _ W V55 : I — HnCom L1 + L2 ((VGS "‘ Vt)VDS _ lof?? EE‘14 HW#1 Solution Analog Integrated Circuit Design September 25, 2008 which is the same result as a single transistor with a channel length of L1 + L2 in triode region. 3. VGS > Vt and VDs > V05 — Vt: In this case M1 is in triode and M2 is in forward active region. To prove this let us assume that M1 is in active region too, hence we have: Vas — Vt < V1351 => VGS“VDSI<Vt—> Mgisoff \—v—/ VGSZ which shows that our initial assumption of M1 being in active region has been wrong. The other possibility, i.e., both M1 and M2 being in triode can also be shown to be impossible using the same method. Now given that M1 is in triode and M2 is in active region we can write down the equations as follows: 1 W 2 12 = iflncozf; (VGS — VDSI ~ Vt) W » V2 II : MnComfl((VGS "' VDVDSI _ D251) Since the current passing through both devices is the same, we can get the following equation: (L1 + L2)Vr2>31 — 2(L1 + L2)(VGs — Vt)VDSI + L1(VGs - V92 = 0 which after a little bit of math crunching leads to: V1331: VGS — V i ———(VGS ‘ Vt) V L3 + Lle t L1 +L2 iM VL2 VLl + L2 :VGS‘l/t—VDSI= therefore, 1 W l W __ _ _ _ ‘_ 2 : _ _________ __ 2 I — 2pn00$ L2 (VGS Vt VDSl) 2NnCom L1 + L2 (VGS which is again equivalent to the equation for a transistor with a channel length of L1 + L2 in forward active region. So we have proved that the given structure has exactly the same behavior as a single transistor with the effective channel length of L1 + L2 in all operating conditions. 2of?? EE'14 HW#1 Solution Analog Integrated Circuit Design September 25, 2008 Solution 2: Another elegant way to solve this problem is to put on your device hats and think of it as a solid—state structure. The following figure shows the cross—sectional view of the given structure. As depicted in this figure, the overall structure looks like a transistor with an effective channel length of L1 + L2. This happens because all the electrons that enter the channel at 81 have to go through both channels. Note that the diffusion area in between (D1 or S2) does not affect carriers movement since it is assumed to be highly—doped. Furthermore, the transistor on the left cannot be in forward active region because once channel 1 pinches off the other transistor will definitely turn off (for similar reasons as mentioned in the previous part). In other words the left transistor can only operate in triode region. Putting all these together you can easily conclude that this structure is just a transistor whose channel is the sum of two smaller channels of length L1 and L2. One can write integrals similar to those in the lecture notes to find the characteristic function to be: 1 W I = — — — 2 2Nn00m L1 + L2 (VGS G1) G2 P—substrate 3of?? 3 ' ACCOVCMUS to a;ch 3 (‘eCA 3) D “Hm: \oxje sxjnm transfer function of CS $‘bage as; 4 H < o? 0 DD’“ JEVCOK ('WT\KVL——VJC) R U) \lDD To WCMA SmaH signal 3am,er skoudck Aiffcrenkia’cc \oo‘fln Sidee aunt Vi 8V0 Av 2 avl Z — PCOX {Vii/)R VOV W‘h‘xck \5 conas-tant OVER tke. resu\f 03C fix: ‘oo‘t’com of swam. LJF. We're \ookhqj for ,\{03 Point COVYC$POhA§nlj to the eAjc: of kher resion {‘or {‘OHOUJEHS C3 amPh fier VDD = 5V Vole! W '1: RC3 Vm \Acox, :- SQ D V0 - Vi G E "THC, ,ConA'Hciom och fig: CABC of {31er region; \IGD .: \1 t H) . 3 Before ‘t‘nc Acvice enters ’Crioéc: ragionq if OPCrfl’tcS m SQJCufat§on . So we. con wri’cq ~, \I K (v m \l 1‘1 R' «3) ‘10 = DD —* 7 63 ‘t V; Subs-Ei‘tu'b'xrxj \LL m (33 from (32) K a m &‘ —— 5“» X 81: X 50% \]O + \10 ~— ESV —— o {5) @Nen \I; ‘IS founcl JCO ‘06: *- Tc Aoubha (“J/\ch our resu‘fi. We ca\CU\od:e ‘an: ID thl [00K at all operatihj Pom‘hts; ID -— ROZSO‘LE X "‘13; = $9 W\ 5V + $56M 1%‘2 _\/R:37‘—7¢V 5. First we stout off \03 'E‘méinj new DC operating Po‘m‘b of the Girauhfi Long ckaw‘ncA egrucx‘ckon Kn ‘kflOc‘c rcflkon Soussz D. \I To =2 K. Hwy—Vflvasfl :5. ) m vi \lo ‘KVLJ ‘lmFMC’S: ' at \IO =—‘- \IDD “— R ID K \ comgmm \ooJck eas= \pb . , ;' __ 0 w \10 : \IDD ~RK (kw—Vt) \IO & ) k5) FWGaWLS ;n numbers -. b V 9‘ ._...._ —-— 0 V0 2: 5 19(X1r32 O a > a so- 5Vo_‘._H\/O+5=O 1 1.55 . / 5 ( >a> \IO 2: 2:). Vasfivta<vés @X 0» 65 —~——> Trs’oéc / _' DC OPera‘tifij Po‘m’c \/o —- 0‘ Q5 «1‘ <Of out—Pch Maia, ) WA > D T __ LL55BA _LD _. LtESNX erooo-m:3 "the. DC. opcra-hnj Po‘mts of ft“: We can finci J(The. circa-NC , Small signal 3cm L33 Afferenf‘iaffij aquation (3) . A ___ 'avo . " 9v; W 6V6 __ < av “__ “ o ._ —R \/ o ._ \I f. 8V; K O + 8V; W‘ V” O 6V1) » AV ( \— ram/0+ RKCVL“VT)\ :: “RKVO V‘>~ [\V =2 —‘ \——‘R\<\/O+\— RK Ur—Vfl vL__\/t :1V K :2 10K |<=<lo><5033=115§ »_ AV : '— 1OKX1-flf/‘Lé— X O'GSV 1———' tox1x0 ~65 + ‘0)“ [email protected] Mtema’cwe So \u-tion ; (10¢ com use Smali—signal mode! 0f device in trioJe th.OY\ “to , firm/J 5mall- Siljnaf gain. In triode region, according 'to basic equation: ID 2-— HCOX KVas—Vt-“if—S— )Vos we com model the device wifix Jame Parametem , 81; @ 3m, Ms Bias Point @ a =—— 310 as avps gift 30,5 : [\ACox. (VG5—“V—tfivDS) Equivalent SmaH’ 519 nai aim in“: aox‘jox 0-65 gm: o-esms 30‘s = S~OX50X \1-065) M AV : {00 : ~— 9m ; (Vi flds__g___&~ ( A :2 __ 0.65 w w >2? V 035+ 0'1: AV“ ‘q’K‘ \/ (Dom. 2 O ‘V 31>. \l;)max : LCJDV Corresponcls to \IOIMgm C,min = “V ’Vo'm‘w“ V ._E:co‘c’c_.earuq-Hon for output voltage: Q.) V0 : \IDD “ '39: “Cox, five—v9 R \:‘> \lo an —‘ 5 w )4le ' _..'\_. ' V3- 4 l a. O,ma>g ’— KER >§ ‘ \lomnoxxo : \lodues Preéic’caA ‘03 quH— Ssgna‘i O«\0~\5$\$: . VODC : QV'BV ’00 :1: [\V ' : *‘ 5 X : "O‘SV 00,4max. : \/O + V0 : 3V ’00,an : V0* \)0 I a” V . __ «Ck — “ 0/0 error m o,mi“’\— \ 1:5?59V‘ K100 =1 1193—6 GO Rn \) __ — X‘OO : Z :(7‘. @ 5ma\\__5~\3fla\ aquimGn't’ MGAGR '- ® Circu‘l'k for DC operatknj Poinf_; >> [\V‘ :2 = Sawfly-{‘1 (I) "W . 3 __ a Accorchnj to \Ohj Canhct MOcJ€( —— VOV blag)» >-—’.>— Pw‘ 2: = + Vol: DC (H WW 1 & vov ——-—«—-.. vi ,= +SM4R‘ X ESMQVRR W M ’RVD‘ : Mgmafia _“ x02 I Vov EL ___~ {RSXQ Ava _. W. W5 .. 5.33 m 2 W114: ...
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This note was uploaded on 11/09/2009 for the course EE 114 taught by Professor Murmann during the Fall '08 term at Stanford.

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EE114_HW1_Solution - BEIN— Auf 08/06 z< Salmon to...

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