Synapses with short-term plasticity are optimal estimators of presynaptic membrane potentials: supplementary note
|
|
- Terence Lawson
- 5 years ago
- Views:
Transcription
1 Synapses wih shor-erm plasiciy are opimal esimaors of presynapic membrane poenials: supplemenary noe Jean-Pascal Pfiser, Peer Dayan, Máé Lengyel Supplemenary Noe 1 The local possynapic poenial In he main ex we pursue he hypohesis ha synapses undergoing STP esimae he somaic membrane poenial of he presynapic cell, wih a quaniy we called he local possynapic poenial represening he resuls of his esimaion process. In his secion we define he local possynapic poenial formally. We also explain how experimenal daa, and in paricular hose recorded in STP experimens, perain o i, and how i relaes o single neuron compuaions. 1.1 Biophysical definiion Consider isolaing he i h synapic comparmen from he res of he dendriic ree. If we also ignore any non-synapic currens, he dynamics of is poenial would follow he simple differenial equaion: C m dv (i d = vres v (i R m + I (i syn( where v res is he resing membrane poenial, C m and R m are he membrane capaciance and resisance, respecively, and I syn( (i describes he curren enering hrough synapic channels. We call v (i he local possynapic poenial. (S1 1.2 Experimenal measuremen Of course, v (i is an idealizaion ha will no be expressed in eiher he dendriic or he somaic membrane poenial under normal condiions, for a leas wo reasons. Firs, he rue membrane poenial of he local dendriic comparmen, v (i, follows a differen equaion: C m dv (i d = vres v (i R m + I (i syn(+i (i oher ( (S2 where I (i oher ( includes oher curren conribuions ha are no he leak curren, nor he synapic curren. This includes currens propagaed from oher pars of he dendriic ree, and acive currens generaed wihin he same comparmen. Second, v (i is no expressed in he somaic membrane poenial of he pos-synapic neuron, v (soma, because he inervening dendrie filers he synapic signal, and he soma inegraes i wih he local possynapic poenials creaed by he many oher simulaneously acive inpus ha he pos-synapic neuron is likely o receive. Therefore, alhough v (i is a useful heoreical consruc for undersanding single neuron compuaion (as long as Eq. S4 holds, see below, i may no be a quaniy ha is immediaely apparen in membrane poenial recordings. Forunaely for our purposes, STP experimens provide very differen condiions from hose presen in he funcional circui 1, and hese make he experimenal assessmen of v (i amenable. 1
2 Pfiser e al. Synapses as opimal esimaors In such experimens, which are ofen in viro 2, normally only a single synapse, or a small subse of synapses is simulaed. This has wo effecs: he somaic membrane poenial depends only on he possynapic poenial in one dendriic comparmen, and he local dendriic membrane poenial is kep in he subhreshold regime which minimises he effecs of acive conducances (i.e. I (i oher 0. Overall, hese effecs resul in he somaic membrane poenial reflecing he local possynapic poenial well excep for he consequences of dendriic filering. Filering will mosly affec he ime consan and absolue ampliude of he somaic signal. We herefore fi only he relaive changes in somaic ampliudes (Fig. 3 of he main paper, which should be less affeced by his. Neverheless, a sronger experimenal es of he heory would require local dendriic recordings under such minimal simulaion condiions. 1.3 Compuaional use A common assumpion in models of neural circui aciviy is ha neurons need o compue some (poenially high-dimensional and complicaed funcions of heir inpus 3,4. In erms of (subhreshold somaic membrane poenials, one can formalise his as ( v (soma = F u (1,u (2,..., u (M (S3 where u (i is he somaic membrane poenial of presynapic neuron i (ou of M, v (soma is he somaic membrane poenial of he possynapic cell, and F is he non-linear funcion i compues on is inpus which depends on dendriic processing and oher inracellular processes. (Noe ha Eq. S3 can be rewrien in erms of pre- and possynapic firing raes, which are hemselves also some non-linear funcions of membrane poenials, in he same general form wih a suiable choice of F. However, since he possynapic membrane poenial can only direcly depend on he spiking oupu of presynapic cells, we propose ha he cell approximaes equaion S3 by applying is non-lineariy o reliable esimaes of he presynapic membrane poenials, û (i. These we sugges are represened by he local possynapic poenials, v (i described above: v (soma = F ( v (1,v (2,..., v (M F ( û (1, û (2,..., û (M This is a key reason for inroducing v (i as an idealizaion. In line wih sandard reduced neuron models 3,5, we assumed here ha he somaic membrane poenial can be wrien o a reasonable approximaion in he form given by equaion S4 as a funcion of v (i, raher han v (i, which means ha he effecs of I (i oher are incorporaed ino F. Crucially, he beer he individual v (i esimae u (i, he beer equaion S4 implemens equaion S3. This is illusraed in Supplemenary Figure S1. (S4 2 Esimaion under he swiching Ornsein Uhlenbeck process 2.1 Generaive process For convenience, recall here he descripion of he generaive model under he swiching Ornsein Uhlenbeck (OU process. In such a process, he resing membrane poenial u res is no fixed bu randomly swiches beween wo levels, u + ans u, corresponding o up and down saes (Supplemenary Fig. S2b P ( u res u res δ = 1 η δ if u res η δ if u res 1 η + δ if u res η + δ if u res = u + and u res δ = u+ = u and u res δ = u+ = u and u res δ = u = u + and u res δ = u where η and η + are he raes of swiching o he down and up saes, respecively. The presynapic membrane poenial evolves as an Ornsein-Uhlenbeck (OU process around he resing poenial u res which is now ime-dependen: P ( [ u u δ,u res = N u ; u δ + 1 ] ( u res u δ δ, σ 2 τ W δ (S6 (S5 2
3 Pfiser e al. Synapses as opimal esimaors Spike generaion is described by he same rule as in he non-swiching case. See Eqs. 5-7 of he main paper. 2.2 Opimal esimaor The opimal esimaor is given by he following filering equaion: P ( u,u res s 0: P(s u u res δ P ( u u δ,u res ( P u res u res ( δ P u δ,u res δ s 0: δ du δ We are primarirly ineresed in he poserior over he membrane poenial. This can be obained by marginalising Equaion S7: where P(u s 0: = u res (S7 P ( u,u res s 0: = (1 ρ p (u +ρ p + (u (S8 ρ =P ( u res = u + s 0: is he esimaed probabiliy of he resing membrane poenial being in is up sae (or he mixure raio, and p (u = P ( u u res = u,s 0: (S10 p + (u = P ( u u res = u +,s 0: (S11 express he poserior disribuion of u assuming ha u res is in is down or up sae, respecively. The mean of he poserior over he presynapic membrane poenial can be wrien as: (S9 û = (1 ρ µ + ρ µ + (S12 where µ = µ + = u p (u du u p + (u du (S13 (S14 are he condiional mean esimaes of u, assuming again ha u res is in is down or up sae, respecively. The change in he poserior mean, corresponding o possynapic poenial dynamics (in coninuous ime is hen û = [1 ρ +ɛ ] µ + ρ +ɛ µ + [ + ρ µ + ɛ µ ] ɛ (S15 Therefore, here are wo facors conribuing o changes in he mean poserior (and hus o he size of an EPSP: changes in he condiional means µ and µ +, and changes in he mixure raio ρ. These wo facors ac addiively. However, for closer correspondence wih he synapic resource and uilisaion variables (Online Mehods, Equaion S15 can be rearranged as: [ ] û = µ 1+ ρ µ (S16 where µ = [1 ρ +ɛ ] µ + ρ +ɛ µ + (S17 ρ [ = ρ µ + ɛ µ ] ɛ (S18 correspond o he wo facors. The associaions of µ and ρ wih shor-erm depression and faciliaion respecively are discussed in he wo nex secions. 3
4 Pfiser e al. Synapses as opimal esimaors 2.3 Changes in he condiional means, µ In order o undersand he condiional means, le us firs revisi he condiionalised poseriors, p (u and p + (u. In he limi when he dynamics of u res are sufficienly slow, and u and u + are no oo far apar, hese are approximaely p (u p + (u P(s u P(s u P ( u u δ = u,u res = u p δ (u du (S19 P ( u u δ = u,u res = u + p + δ (u du (S20 If p δ (u and p + δ (u are Gaussians, each of Equaions S19-S20 describes he poserior updaes for a simple OU process wih non-linear Poisson spike generaion, as derived in he main paper. This implies ha he wo condiional means, µ and µ +, evolve as he poserior mean, û in Eq. 11 of he main paper: heir updaes depend on he (here, condiionalised, or relaive poserior variances when observing a spike a ime : where µ ( σ ɛ 2, µ + ( σ + ɛ 2 (S21 ( σ 2 = u 2 p (u du ( µ 2 (S22 ( σ + 2 = u 2 p + (u du ( µ + 2 (S23 We know from Eqs. 11 and 12 of he main paper ha he proporionaliy in equaion S21 leads o depression. Thus µ, he oal change in û due o changes in he condiional means a he ime of an incoming spike, will also show depression because i is a weighed some of wo erms ha boh depress individually: µ σ2 (S24 where, from Eq. S17 σ 2 = [1 ρ +ɛ ] ( σ ɛ 2 + ρ+ɛ ( σ + ɛ 2 (S Changes in he mixure raio, ρ The dynamical equaion for he mixure raio can be derived as (see secion 2.5: ρ η + [ η + + η + γ + γ ] ρ [ γ + γ ] ρ 2 + ρ ɛ S (S26 where γ + δ =P ( s =1 u res = u +,s 0: δ and γ δ =P ( s =1 u res = u,s 0: δ (S27 are he (condiionalised poserior firing raes and are analogous o γ derived in Eq. 10 of he main ex. The mos imporan erm from Equaion S26 for us now is ρ = 1 1+ γ 1 ρ γ + ρ ρ (S28 expressing he size of he insananeous updae in ρ afer observing a spike (Fig. S3 a ime (see Supplemenary Figure S3. This quaniy is non-negaive, and highly non-linear in ρ: in paricular, i has an invered U-shape which means ha in he range of low ρ values (he lef arm of he invered-u, larger ρ values imply larger incremens in ρ hus leading o faciliaion. The greaer he difference in firing raes beween he up and down saes is, γ + /γ, he 4
5 Pfiser e al. Synapses as opimal esimaors larger he magniude bu also he smaller he window of faciliaion becomes (he peak of he ρ curve shifs up and o he lef. Also noe, ha for he range of large ρ values, depression, raher han faciliaion, is prediced. The overall effec, of course, also depends on he condiional means, because ρ = [ µ + ɛ µ ] ɛ ρ (see Eq. S18, and he balance beween µ and ρ (Eq. S Deriving ρ The mixure raio ρ = P(u res u res δ = u + s 0: a ime can be wrien as ρ = P ( u,u res = u + s 0: du (S29 By using he filering equaion of he opimal esimaor (equaion S7, we wrie ρ P ( u res = u + u res ( δ P u res δ s 0: δ u res δ u res δ P ( u res P(s u P ( u u δ,u res = u + u res ( δ P u res δ s 0: δ P ( s u δ,u res P ( u res u res δ = u + P ( u δ u res δ,s 0: δ du δ du = u + P ( u δ u res δ,s 0: δ du δ = u + u res ( ( δ P u res δ s 0: δ P s u res = u +,u res δ,s 0: δ (S30 (S31 If we assume ha he he probabiliy of having a spike a ime, given he resing membrane poenial a ime, u res and he spiking hisory s 0: δ, is independen of he resing membrane poenial a ime δ, we have: ρ P ( u res = u + u res ( ( δ P u res δ s 0: δ P s u res = u +,s 0: δ P ( s u res = u +,s 0: δ [ (1 ρ δ η + δ + ρ δ ( 1 η δ ] (S32 Similarly, he esimaed probabiliy of being in he down sae is appoximaely proporional (wih he same consan of proporionaliy o (1 ρ P ( s u res = u,s 0: δ [ (1 ρ δ ( 1 η + δ + ρ δ η δ ] (S33 Le α denoe he proporionaliy facor assumed in equaions S32 and S33. By firs noing ha ρ can be rivially rearranged as 1 ρ = 1+ α (1 ρ (S34 αρ we can inser equaions S32 and S33 o ge 1 ρ 1+ P(s u res = u,s 0: δ [(1 ρ δ (1 η + δ+ρ δ η δ] P(s u res = u +,s 0: δ [(1 ρ δ η + δ + ρ δ (1 η δ] Formally, i can be shown, ha (S35 lim ρ γ + /γ =1 ρ and lim ρ γ + /γ = ɛρ [1 ρ ] where ɛ = 1 1 γ /γ + 0. I is ineresing o noe ha in his laer limi he updae in ρ happens o be proporional o he uncerainy abou he resing membrane poenial (i.e. he variance of he associaed Bernoulli disribuion, ρ [1 ρ ] 5
6 Pfiser e al. Synapses as opimal esimaors By aking he limi of δ 0 and afer some elemenary algebra, we can express he emporal derivaive of ρ: ρ ρ δ ρ = lim δ 0 δ η + [ η + + η + γ + γ ] ρ [ γ + γ ] ρ 2 + ρ ɛs (S36 where γ + and γ denoe he condiionalised poserior firing raes of he up sae and down sae respecively: γ + δ = P ( s =1 u res = u +,s 0: δ γ δ = P ( s =1 u res = u,s 0: δ and ρ denoes he ampliude of he updae of ρ afer having observed a spike a ime : ρ = 1+ γ γ ρ ρ ρ (S37 6
7 Pfiser e al. Synapses as opimal esimaors { Supplemenary Figures and Legends 100 ms { presynapic neurons J 1 J M -('./012/*'3, #!!#! "!! #!! $!! %&'(*'+, possynapic neuron Firing rae [Hz] Time [ms] Supplemenary Figure S1. Compuaion wih M = 100 inpus. Lef: membrane poenial races u (i of he presynapic neurons. Middle-lef: presynapic spike rains generaed from he membrane poenial races. Middle: esimaed presynapic membrane poenial û (i wih a saic synapse (green a dynamical synapse (blue and he opimal esimaor (red. The black line denoes he presynapic membrane poenial iself. Middle-righ: ideally, he somaic membrane poenial of he possynapic cell compues a (poenially non-linear funcion (here, we ook v (soma = i J iu (i of is M = 100 inpus (black. Pracically, his is approximaed as i J iû (i wih esimaes û (i given by saic synapses (green, dynamical synapses (blue, or he opimal esimaor (red. Righ: firing rae of he possynapic neuron which is compued as a non-linear (here sigmoidal funcion of he somaic poenial of he possynapic neuron, f ( v (soma. Parameers for he simulaion were: βσ=2, τ =20 ms, g(u res =10 Hz, J i =1/ M, f(v=f 0 /(1 + exp( αv, wih f 0 =50 Hz and α=2 mv 1. 7
8 Pfiser e al. Synapses as opimal esimaors a.u 1... u 1 u c.s 1... s 1 s b u res 1... u res 1 u res.u 1... u 1 u :/;3./3./*26;0<4-4/=0-.3*07>?9 "!!"!#$!#"!$$!$".s 1... s 1 s *+,-./*0123*/ u $" (" '" &" %" Supplemenary Figure S2. Generaive model for presynapic membrane poenial flucuaions and spike generaion. (a Graphical model for he case wih consan resing membrane poenial. The membrane poenial u follows an Ornsein-Uhlenbeck (OU process around a consan resing poenial u res. A spike is elicied a ime (s = 1 wih probabiliy g(u δ. (b Graphical model for he case wih changing resing membrane poenial. The resing poenial u res (see Eq. S5 can randomly swich beween a down and an up sae. (c Insananeous firing rae g(u as a funcion of he membrane poenial u for differen values of he spiking deerminism parameer β (β 1 = 3 mv solid line, 10 mv do-dashed line, 1 mv doed line wih g 0 se such ha g( 60 mv=10 Hz. 8
9 Pfiser e al. Synapses as opimal esimaors 1 ρ ρ Supplemenary Figure S3. ρ, he incremen in ρ afer observing a spike, as a funcion of ρ, for differen values of γ+ γ (1 blue, 2 green, 5 orange, 10 red, - black. Doed black line shows he locaion of he peak of he curves as γ+ γ is varied 1. 9
10 Pfiser e al. Synapses as opimal esimaors References 1. Bors, J.G.G. The low synapic release probabiliy in vivo. Trends Neurosci. 33, ( Diman, J., Kreizer, A. & Regehr, W. Inerplay beween faciliaion, depression, and residual calcium a hree presynapic erminals. J. Neurosci. 20, ( Dayan, P. & Abbo, L.F. Theoreical Neuroscience (MIT Press, Cambridge, Zador, A. The basic uni of compuaion. Na. Neurosci. 3, 1167 ( Aguera y Arcas, B., Fairhall, A.L. & Bialek, W. Compuaion in a single neuron: Hodgkin and Huxley revisied. Neural Compu. 15, (
Nature Neuroscience: doi: /nn Supplementary Figure 1. Spike-count autocorrelations in time.
Supplemenary Figure 1 Spike-coun auocorrelaions in ime. Normalized auocorrelaion marices are shown for each area in a daase. The marix shows he mean correlaion of he spike coun in each ime bin wih he spike
More informationVehicle Arrival Models : Headway
Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where
More information20. Applications of the Genetic-Drift Model
0. Applicaions of he Geneic-Drif Model 1) Deermining he probabiliy of forming any paricular combinaion of genoypes in he nex generaion: Example: If he parenal allele frequencies are p 0 = 0.35 and q 0
More informationEE100 Lab 3 Experiment Guide: RC Circuits
I. Inroducion EE100 Lab 3 Experimen Guide: A. apaciors A capacior is a passive elecronic componen ha sores energy in he form of an elecrosaic field. The uni of capaciance is he farad (coulomb/vol). Pracical
More informationSimulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010
Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid
More informationModule 2 F c i k c s la l w a s o s f dif di fusi s o i n
Module Fick s laws of diffusion Fick s laws of diffusion and hin film soluion Adolf Fick (1855) proposed: d J α d d d J (mole/m s) flu (m /s) diffusion coefficien and (mole/m 3 ) concenraion of ions, aoms
More informationThe field of mathematics has made tremendous impact on the study of
A Populaion Firing Rae Model of Reverberaory Aciviy in Neuronal Neworks Zofia Koscielniak Carnegie Mellon Universiy Menor: Dr. G. Bard Ermenrou Universiy of Pisburgh Inroducion: The field of mahemaics
More informationPhysics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle
Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,
More informationKriging Models Predicting Atrazine Concentrations in Surface Water Draining Agricultural Watersheds
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 Kriging Models Predicing Arazine Concenraions in Surface Waer Draining Agriculural Waersheds Paul L. Mosquin, Jeremy Aldworh, Wenlin Chen Supplemenal Maerial Number
More informationChapter 7 Response of First-order RL and RC Circuits
Chaper 7 Response of Firs-order RL and RC Circuis 7.- The Naural Response of RL and RC Circuis 7.3 The Sep Response of RL and RC Circuis 7.4 A General Soluion for Sep and Naural Responses 7.5 Sequenial
More informationPhysics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution
Physics 7b: Saisical Mechanics Fokker-Planck Equaion The Langevin equaion approach o he evoluion of he velociy disribuion for he Brownian paricle migh leave you uncomforable. A more formal reamen of his
More informationLinear Response Theory: The connection between QFT and experiments
Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and
More informationLinear Time-invariant systems, Convolution, and Cross-correlation
Linear Time-invarian sysems, Convoluion, and Cross-correlaion (1) Linear Time-invarian (LTI) sysem A sysem akes in an inpu funcion and reurns an oupu funcion. x() T y() Inpu Sysem Oupu y() = T[x()] An
More informationDiebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles
Diebold, Chaper 7 Francis X. Diebold, Elemens of Forecasing, 4h Ediion (Mason, Ohio: Cengage Learning, 006). Chaper 7. Characerizing Cycles Afer compleing his reading you should be able o: Define covariance
More informationReading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.
PHY1 Elecriciy Topic 7 (Lecures 1 & 11) Elecric Circuis n his opic, we will cover: 1) Elecromoive Force (EMF) ) Series and parallel resisor combinaions 3) Kirchhoff s rules for circuis 4) Time dependence
More informationNotes on Kalman Filtering
Noes on Kalman Filering Brian Borchers and Rick Aser November 7, Inroducion Daa Assimilaion is he problem of merging model predicions wih acual measuremens of a sysem o produce an opimal esimae of he curren
More informationINDEX. Transient analysis 1 Initial Conditions 1
INDEX Secion Page Transien analysis 1 Iniial Condiions 1 Please inform me of your opinion of he relaive emphasis of he review maerial by simply making commens on his page and sending i o me a: Frank Mera
More informationd 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3
and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or
More informationSome Basic Information about M-S-D Systems
Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,
More informationPENALIZED LEAST SQUARES AND PENALIZED LIKELIHOOD
PENALIZED LEAST SQUARES AND PENALIZED LIKELIHOOD HAN XIAO 1. Penalized Leas Squares Lasso solves he following opimizaion problem, ˆβ lasso = arg max β R p+1 1 N y i β 0 N x ij β j β j (1.1) for some 0.
More informationMath 333 Problem Set #2 Solution 14 February 2003
Mah 333 Problem Se #2 Soluion 14 February 2003 A1. Solve he iniial value problem dy dx = x2 + e 3x ; 2y 4 y(0) = 1. Soluion: This is separable; we wrie 2y 4 dy = x 2 + e x dx and inegrae o ge The iniial
More informationTwo Coupled Oscillators / Normal Modes
Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own
More informationMath 10B: Mock Mid II. April 13, 2016
Name: Soluions Mah 10B: Mock Mid II April 13, 016 1. ( poins) Sae, wih jusificaion, wheher he following saemens are rue or false. (a) If a 3 3 marix A saisfies A 3 A = 0, hen i canno be inverible. True.
More informationRC, RL and RLC circuits
Name Dae Time o Complee h m Parner Course/ Secion / Grade RC, RL and RLC circuis Inroducion In his experimen we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors.
More informationChapter 2. First Order Scalar Equations
Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.
More informationDesigning Information Devices and Systems I Spring 2019 Lecture Notes Note 17
EES 16A Designing Informaion Devices and Sysems I Spring 019 Lecure Noes Noe 17 17.1 apaciive ouchscreen In he las noe, we saw ha a capacior consiss of wo pieces on conducive maerial separaed by a nonconducive
More informationProblem Set #1. i z. the complex propagation constant. For the characteristic impedance:
Problem Se # Problem : a) Using phasor noaion, calculae he volage and curren waves on a ransmission line by solving he wave equaion Assume ha R, L,, G are all non-zero and independen of frequency From
More informationBasic Circuit Elements Professor J R Lucas November 2001
Basic Circui Elemens - J ucas An elecrical circui is an inerconnecion of circui elemens. These circui elemens can be caegorised ino wo ypes, namely acive and passive elemens. Some Definiions/explanaions
More informationKEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow
1 KEY Mah 4 Miderm I Fall 8 secions 1 and Insrucor: Sco Glasgow Please do NOT wrie on his eam. No credi will be given for such work. Raher wrie in a blue book, or on our own paper, preferabl engineering
More informationSOLUTIONS TO ECE 3084
SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no
More informationOn Measuring Pro-Poor Growth. 1. On Various Ways of Measuring Pro-Poor Growth: A Short Review of the Literature
On Measuring Pro-Poor Growh 1. On Various Ways of Measuring Pro-Poor Growh: A Shor eview of he Lieraure During he pas en years or so here have been various suggesions concerning he way one should check
More informationThe Arcsine Distribution
The Arcsine Disribuion Chris H. Rycrof Ocober 6, 006 A common heme of he class has been ha he saisics of single walker are ofen very differen from hose of an ensemble of walkers. On he firs homework, we
More informationFinal Spring 2007
.615 Final Spring 7 Overview The purpose of he final exam is o calculae he MHD β limi in a high-bea oroidal okamak agains he dangerous n = 1 exernal ballooning-kink mode. Effecively, his corresponds o
More informationGuest Lectures for Dr. MacFarlane s EE3350 Part Deux
Gues Lecures for Dr. MacFarlane s EE3350 Par Deux Michael Plane Mon., 08-30-2010 Wrie name in corner. Poin ou his is a review, so I will go faser. Remind hem o go lisen o online lecure abou geing an A
More information3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon
3..3 INRODUCION O DYNAMIC OPIMIZAION: DISCREE IME PROBLEMS A. he Hamilonian and Firs-Order Condiions in a Finie ime Horizon Define a new funcion, he Hamilonian funcion, H. H he change in he oal value of
More informationClass Meeting # 10: Introduction to the Wave Equation
MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion
More informationACE 562 Fall Lecture 5: The Simple Linear Regression Model: Sampling Properties of the Least Squares Estimators. by Professor Scott H.
ACE 56 Fall 005 Lecure 5: he Simple Linear Regression Model: Sampling Properies of he Leas Squares Esimaors by Professor Sco H. Irwin Required Reading: Griffihs, Hill and Judge. "Inference in he Simple
More information0.1 MAXIMUM LIKELIHOOD ESTIMATION EXPLAINED
0.1 MAXIMUM LIKELIHOOD ESTIMATIO EXPLAIED Maximum likelihood esimaion is a bes-fi saisical mehod for he esimaion of he values of he parameers of a sysem, based on a se of observaions of a random variable
More information( ) = Q 0. ( ) R = R dq. ( t) = I t
ircuis onceps The addiion of a simple capacior o a circui of resisors allows wo relaed phenomena o occur The observaion ha he ime-dependence of a complex waveform is alered by he circui is referred o as
More informationTwo Popular Bayesian Estimators: Particle and Kalman Filters. McGill COMP 765 Sept 14 th, 2017
Two Popular Bayesian Esimaors: Paricle and Kalman Filers McGill COMP 765 Sep 14 h, 2017 1 1 1, dx x Bel x u x P x z P Recall: Bayes Filers,,,,,,, 1 1 1 1 u z u x P u z u x z P Bayes z = observaion u =
More informationExplaining Total Factor Productivity. Ulrich Kohli University of Geneva December 2015
Explaining Toal Facor Produciviy Ulrich Kohli Universiy of Geneva December 2015 Needed: A Theory of Toal Facor Produciviy Edward C. Presco (1998) 2 1. Inroducion Toal Facor Produciviy (TFP) has become
More informationKINEMATICS IN ONE DIMENSION
KINEMATICS IN ONE DIMENSION PREVIEW Kinemaics is he sudy of how hings move how far (disance and displacemen), how fas (speed and velociy), and how fas ha how fas changes (acceleraion). We say ha an objec
More informationR t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t
Exercise 7 C P = α + β R P + u C = αp + βr + v (a) (b) C R = α P R + β + w (c) Assumpions abou he disurbances u, v, w : Classical assumions on he disurbance of one of he equaions, eg. on (b): E(v v s P,
More informationSTATE-SPACE MODELLING. A mass balance across the tank gives:
B. Lennox and N.F. Thornhill, 9, Sae Space Modelling, IChemE Process Managemen and Conrol Subjec Group Newsleer STE-SPACE MODELLING Inroducion: Over he pas decade or so here has been an ever increasing
More information8. Basic RL and RC Circuits
8. Basic L and C Circuis This chaper deals wih he soluions of he responses of L and C circuis The analysis of C and L circuis leads o a linear differenial equaion This chaper covers he following opics
More informationLab 10: RC, RL, and RLC Circuits
Lab 10: RC, RL, and RLC Circuis In his experimen, we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors. We will sudy he way volages and currens change in
More informationCHAPTER 12 DIRECT CURRENT CIRCUITS
CHAPTER 12 DIRECT CURRENT CIUITS DIRECT CURRENT CIUITS 257 12.1 RESISTORS IN SERIES AND IN PARALLEL When wo resisors are conneced ogeher as shown in Figure 12.1 we said ha hey are conneced in series. As
More informationR.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder#
.#W.#Erickson# Deparmen#of#Elecrical,#Compuer,#and#Energy#Engineering# Universiy#of#Colorado,#Boulder# Chaper 2 Principles of Seady-Sae Converer Analysis 2.1. Inroducion 2.2. Inducor vol-second balance,
More information2.4 Cuk converter example
2.4 Cuk converer example C 1 Cuk converer, wih ideal swich i 1 i v 1 2 1 2 C 2 v 2 Cuk converer: pracical realizaion using MOSFET and diode C 1 i 1 i v 1 2 Q 1 D 1 C 2 v 2 28 Analysis sraegy This converer
More information14 Autoregressive Moving Average Models
14 Auoregressive Moving Average Models In his chaper an imporan parameric family of saionary ime series is inroduced, he family of he auoregressive moving average, or ARMA, processes. For a large class
More informationChallenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k
Challenge Problems DIS 03 and 0 March 6, 05 Choose one of he following problems, and work on i in your group. Your goal is o convince me ha your answer is correc. Even if your answer isn compleely correc,
More informationNavneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi
Creep in Viscoelasic Subsances Numerical mehods o calculae he coefficiens of he Prony equaion using creep es daa and Herediary Inegrals Mehod Navnee Saini, Mayank Goyal, Vishal Bansal (23); Term Projec
More informationChapter 2. Models, Censoring, and Likelihood for Failure-Time Data
Chaper 2 Models, Censoring, and Likelihood for Failure-Time Daa William Q. Meeker and Luis A. Escobar Iowa Sae Universiy and Louisiana Sae Universiy Copyrigh 1998-2008 W. Q. Meeker and L. A. Escobar. Based
More informationCHAPTER 2 Signals And Spectra
CHAPER Signals And Specra Properies of Signals and Noise In communicaion sysems he received waveform is usually caegorized ino he desired par conaining he informaion, and he undesired par. he desired par
More informationA Bayesian Approach to Spectral Analysis
Chirped Signals A Bayesian Approach o Specral Analysis Chirped signals are oscillaing signals wih ime variable frequencies, usually wih a linear variaion of frequency wih ime. E.g. f() = A cos(ω + α 2
More information) were both constant and we brought them from under the integral.
YIELD-PER-RECRUIT (coninued The yield-per-recrui model applies o a cohor, bu we saw in he Age Disribuions lecure ha he properies of a cohor do no apply in general o a collecion of cohors, which is wha
More informationEcon107 Applied Econometrics Topic 7: Multicollinearity (Studenmund, Chapter 8)
I. Definiions and Problems A. Perfec Mulicollineariy Econ7 Applied Economerics Topic 7: Mulicollineariy (Sudenmund, Chaper 8) Definiion: Perfec mulicollineariy exiss in a following K-variable regression
More informationEcological Archives E A1. Meghan A. Duffy, Spencer R. Hall, Carla E. Cáceres, and Anthony R. Ives.
Ecological Archives E9-95-A1 Meghan A. Duffy, pencer R. Hall, Carla E. Cáceres, and Anhony R. ves. 29. Rapid evoluion, seasonaliy, and he erminaion of parasie epidemics. Ecology 9:1441 1448. Appendix A.
More informationElectrical and current self-induction
Elecrical and curren self-inducion F. F. Mende hp://fmnauka.narod.ru/works.hml mende_fedor@mail.ru Absrac The aricle considers he self-inducance of reacive elemens. Elecrical self-inducion To he laws of
More informationCHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK
175 CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK 10.1 INTRODUCTION Amongs he research work performed, he bes resuls of experimenal work are validaed wih Arificial Neural Nework. From he
More informationSUPPLEMENTARY INFORMATION
SUPPLEMENTARY INFORMATION DOI: 0.038/NCLIMATE893 Temporal resoluion and DICE * Supplemenal Informaion Alex L. Maren and Sephen C. Newbold Naional Cener for Environmenal Economics, US Environmenal Proecion
More informationCHAPTER 6: FIRST-ORDER CIRCUITS
EEE5: CI CUI T THEOY CHAPTE 6: FIST-ODE CICUITS 6. Inroducion This chaper considers L and C circuis. Applying he Kirshoff s law o C and L circuis produces differenial equaions. The differenial equaions
More informationDimitri Solomatine. D.P. Solomatine. Data-driven modelling (part 2). 2
Daa-driven modelling. Par. Daa-driven Arificial di Neural modelling. Newors Par Dimiri Solomaine Arificial neural newors D.P. Solomaine. Daa-driven modelling par. 1 Arificial neural newors ANN: main pes
More informationSequential Importance Resampling (SIR) Particle Filter
Paricle Filers++ Pieer Abbeel UC Berkeley EECS Many slides adaped from Thrun, Burgard and Fox, Probabilisic Roboics 1. Algorihm paricle_filer( S -1, u, z ): 2. Sequenial Imporance Resampling (SIR) Paricle
More information6.2 Transforms of Derivatives and Integrals.
SEC. 6.2 Transforms of Derivaives and Inegrals. ODEs 2 3 33 39 23. Change of scale. If l( f ()) F(s) and c is any 33 45 APPLICATION OF s-shifting posiive consan, show ha l( f (c)) F(s>c)>c (Hin: In Probs.
More information5. Stochastic processes (1)
Lec05.pp S-38.45 - Inroducion o Teleraffic Theory Spring 2005 Conens Basic conceps Poisson process 2 Sochasic processes () Consider some quaniy in a eleraffic (or any) sysem I ypically evolves in ime randomly
More informationMacroeconomic Theory Ph.D. Qualifying Examination Fall 2005 ANSWER EACH PART IN A SEPARATE BLUE BOOK. PART ONE: ANSWER IN BOOK 1 WEIGHT 1/3
Macroeconomic Theory Ph.D. Qualifying Examinaion Fall 2005 Comprehensive Examinaion UCLA Dep. of Economics You have 4 hours o complee he exam. There are hree pars o he exam. Answer all pars. Each par has
More informationTesting the Random Walk Model. i.i.d. ( ) r
he random walk heory saes: esing he Random Walk Model µ ε () np = + np + Momen Condiions where where ε ~ i.i.d he idea here is o es direcly he resricions imposed by momen condiions. lnp lnp µ ( lnp lnp
More informationTesting for a Single Factor Model in the Multivariate State Space Framework
esing for a Single Facor Model in he Mulivariae Sae Space Framework Chen C.-Y. M. Chiba and M. Kobayashi Inernaional Graduae School of Social Sciences Yokohama Naional Universiy Japan Faculy of Economics
More informationComparing Means: t-tests for One Sample & Two Related Samples
Comparing Means: -Tess for One Sample & Two Relaed Samples Using he z-tes: Assumpions -Tess for One Sample & Two Relaed Samples The z-es (of a sample mean agains a populaion mean) is based on he assumpion
More informationIntroduction D P. r = constant discount rate, g = Gordon Model (1962): constant dividend growth rate.
Inroducion Gordon Model (1962): D P = r g r = consan discoun rae, g = consan dividend growh rae. If raional expecaions of fuure discoun raes and dividend growh vary over ime, so should he D/P raio. Since
More information13.3 Term structure models
13.3 Term srucure models 13.3.1 Expecaions hypohesis model - Simples "model" a) shor rae b) expecaions o ge oher prices Resul: y () = 1 h +1 δ = φ( δ)+ε +1 f () = E (y +1) (1) =δ + φ( δ) f (3) = E (y +)
More informationEstimation of Poses with Particle Filters
Esimaion of Poses wih Paricle Filers Dr.-Ing. Bernd Ludwig Chair for Arificial Inelligence Deparmen of Compuer Science Friedrich-Alexander-Universiä Erlangen-Nürnberg 12/05/2008 Dr.-Ing. Bernd Ludwig (FAU
More informationEE 435. Lecture 31. Absolute and Relative Accuracy DAC Design. The String DAC
EE 435 Lecure 3 Absolue and Relaive Accuracy DAC Design The Sring DAC . Review from las lecure. DFT Simulaion from Malab Quanizaion Noise DACs and ADCs generally quanize boh ampliude and ime If convering
More informationSolutions to Odd Number Exercises in Chapter 6
1 Soluions o Odd Number Exercises in 6.1 R y eˆ 1.7151 y 6.3 From eˆ ( T K) ˆ R 1 1 SST SST SST (1 R ) 55.36(1.7911) we have, ˆ 6.414 T K ( ) 6.5 y ye ye y e 1 1 Consider he erms e and xe b b x e y e b
More informationChapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws
Chaper 5: Phenomena Phenomena: The reacion (aq) + B(aq) C(aq) was sudied a wo differen emperaures (98 K and 35 K). For each emperaure he reacion was sared by puing differen concenraions of he 3 species
More information( ) ( ) ( ) + W aa. ( t) n t ( ) ( )
Supplemenary maerial o: Princeon Universiy Press, all righs reserved From: Chaper 3: Deriving Classic Models in Ecology and Evoluionary Biology A Biologis s Guide o Mahemaical Modeling in Ecology and Evoluion
More informationEECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits
EEE25 ircui Analysis I Se 4: apaciors, Inducors, and Firs-Order inear ircuis Shahriar Mirabbasi Deparmen of Elecrical and ompuer Engineering Universiy of Briish olumbia shahriar@ece.ubc.ca Overview Passive
More information15. Vector Valued Functions
1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,
More informationEECE 301 Signals & Systems Prof. Mark Fowler
EECE 3 Signals & Sysems Prof. Mark Fowler Noe Se # Wha are Coninuous-Time Signals??? /6 Coninuous-Time Signal Coninuous Time (C-T) Signal: A C-T signal is defined on he coninuum of ime values. Tha is:
More informationMechanical Fatigue and Load-Induced Aging of Loudspeaker Suspension. Wolfgang Klippel,
Mechanical Faigue and Load-Induced Aging of Loudspeaker Suspension Wolfgang Klippel, Insiue of Acousics and Speech Communicaion Dresden Universiy of Technology presened a he ALMA Symposium 2012, Las Vegas
More informationWhat Ties Return Volatilities to Price Valuations and Fundamentals? On-Line Appendix
Wha Ties Reurn Volailiies o Price Valuaions and Fundamenals? On-Line Appendix Alexander David Haskayne School of Business, Universiy of Calgary Piero Veronesi Universiy of Chicago Booh School of Business,
More informationLecture 2 October ε-approximation of 2-player zero-sum games
Opimizaion II Winer 009/10 Lecurer: Khaled Elbassioni Lecure Ocober 19 1 ε-approximaion of -player zero-sum games In his lecure we give a randomized ficiious play algorihm for obaining an approximae soluion
More informationLecture 3: Exponential Smoothing
NATCOR: Forecasing & Predicive Analyics Lecure 3: Exponenial Smoohing John Boylan Lancaser Cenre for Forecasing Deparmen of Managemen Science Mehods and Models Forecasing Mehod A (numerical) procedure
More informationProblem Set 5. Graduate Macro II, Spring 2017 The University of Notre Dame Professor Sims
Problem Se 5 Graduae Macro II, Spring 2017 The Universiy of Nore Dame Professor Sims Insrucions: You may consul wih oher members of he class, bu please make sure o urn in your own work. Where applicable,
More informationGeorey E. Hinton. University oftoronto. Technical Report CRG-TR February 22, Abstract
Parameer Esimaion for Linear Dynamical Sysems Zoubin Ghahramani Georey E. Hinon Deparmen of Compuer Science Universiy oftorono 6 King's College Road Torono, Canada M5S A4 Email: zoubin@cs.orono.edu Technical
More informationT L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB
Elecronic Companion EC.1. Proofs of Technical Lemmas and Theorems LEMMA 1. Le C(RB) be he oal cos incurred by he RB policy. Then we have, T L E[C(RB)] 3 E[Z RB ]. (EC.1) Proof of Lemma 1. Using he marginal
More informationCode-specific policy gradient rules for spiking neurons
Code-specific policy gradien rules for spiking neurons Henning Sprekeler Guillaume Hennequin Wulfram Gersner Laboraory for Compuaional Neuroscience École Polyechnique Fédérale de Lausanne 115 Lausanne
More informationMath 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:
Mah 4 Eam Review Problems Problem. Calculae he 3rd Taylor polynomial for arcsin a =. Soluion. Le f() = arcsin. For his problem, we use he formula f() + f () + f ()! + f () 3! for he 3rd Taylor polynomial
More informationLecture 33: November 29
36-705: Inermediae Saisics Fall 2017 Lecurer: Siva Balakrishnan Lecure 33: November 29 Today we will coninue discussing he boosrap, and hen ry o undersand why i works in a simple case. In he las lecure
More informationA Dynamic Model of Economic Fluctuations
CHAPTER 15 A Dynamic Model of Economic Flucuaions Modified for ECON 2204 by Bob Murphy 2016 Worh Publishers, all righs reserved IN THIS CHAPTER, OU WILL LEARN: how o incorporae dynamics ino he AD-AS model
More informationChapter 2: Principles of steady-state converter analysis
Chaper 2 Principles of Seady-Sae Converer Analysis 2.1. Inroducion 2.2. Inducor vol-second balance, capacior charge balance, and he small ripple approximaion 2.3. Boos converer example 2.4. Cuk converer
More informationBias in Conditional and Unconditional Fixed Effects Logit Estimation: a Correction * Tom Coupé
Bias in Condiional and Uncondiional Fixed Effecs Logi Esimaion: a Correcion * Tom Coupé Economics Educaion and Research Consorium, Naional Universiy of Kyiv Mohyla Academy Address: Vul Voloska 10, 04070
More informationRandom Walk with Anti-Correlated Steps
Random Walk wih Ani-Correlaed Seps John Noga Dirk Wagner 2 Absrac We conjecure he expeced value of random walks wih ani-correlaed seps o be exacly. We suppor his conjecure wih 2 plausibiliy argumens and
More informationZürich. ETH Master Course: L Autonomous Mobile Robots Localization II
Roland Siegwar Margaria Chli Paul Furgale Marco Huer Marin Rufli Davide Scaramuzza ETH Maser Course: 151-0854-00L Auonomous Mobile Robos Localizaion II ACT and SEE For all do, (predicion updae / ACT),
More informationThe Simple Linear Regression Model: Reporting the Results and Choosing the Functional Form
Chaper 6 The Simple Linear Regression Model: Reporing he Resuls and Choosing he Funcional Form To complee he analysis of he simple linear regression model, in his chaper we will consider how o measure
More informationt is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...
Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger
More informationSummary of shear rate kinematics (part 1)
InroToMaFuncions.pdf 4 CM465 To proceed o beer-designed consiuive equaions, we need o know more abou maerial behavior, i.e. we need more maerial funcions o predic, and we need measuremens of hese maerial
More informationSub Module 2.6. Measurement of transient temperature
Mechanical Measuremens Prof. S.P.Venkaeshan Sub Module 2.6 Measuremen of ransien emperaure Many processes of engineering relevance involve variaions wih respec o ime. The sysem properies like emperaure,
More information( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively:
XIII. DIFFERENCE AND DIFFERENTIAL EQUATIONS Ofen funcions, or a sysem of funcion, are paramerized in erms of some variable, usually denoed as and inerpreed as ime. The variable is wrien as a funcion of
More information