EE42/100 Lecture 9 Topics: More on First-Order Circuits Water model and potential plot for RC...

transcript

EE42/100 Lecture 9

Topics: More on First-Order Circuits Water model and potential plot for RC circuits A bit on Second-Order Circuits

First-Order Circuits• A circuit which contains only sources, resistors

and an inductor is called an RL circuit.• A circuit which contains only sources, resistors

and a capacitor is called an RC circuit.• RL and RC circuits are called first-order circuits

because their voltages and currents are described by first-order differential equations.

The natural response of an RL or RC circuit is its behavior (i.e. current and voltage) when stored energy in the inductor or capacitor is released to the resistive part of the network (containing no independent sources).

The step response of an RL or RC circuit is its behavior when a voltage or current source step is applied to the circuit, or immediately after a switch state is changed.

Natural Response of an RL Circuit

• Consider the following circuit, for which the switch is closed for t < 0, and then opened at t = 0:

Notation:0– is used to denote the time just prior to switching

0+ is used to denote the time immediately after switching

• The current flowing in the inductor at t = 0– is Io

Ro RIo

Recall: The current flowing in an inductor cannot change instantly, and the voltage across a capacitor, which is proportional to the charge stored in the capacitor, cannot change instantly. For a first-order circuit these are called initial values of current and voltage. A long time after the circuit configuration changes, the currents and voltages achieve their final, or steady-state values.

Later when we talk about second-order circuits – ones that consist of resistors and the equivalent of two energy storage elements, like an L and a C or two Cs – we’ll take a look at the initial and final values of thesequantities and their time derivatives.

Solving for the Current (t 0)• For t > 0, the circuit reduces to

• Applying KVL to the LR circuit:

• Solution:

LRo RIo

tLReiti )/()0()(

What Does e-t/ Look Like?

with = 10-4

• is the amount of time necessary for an exponential to decay to 36.7% of its initial value.

• -1/ is the initial slope of an exponential with an initial value of 1.

Solving for the Voltage (t > 0)

• Note that the voltage changes abruptly:

tLRoeIti )/()(

LRo RIo

ReIiRtvt

)( 0,for

0)0()/(

Time Constant

• In the example, we found that

• Define the time constant

– At t = , the current has reduced to 1/e (~0.37) of its initial value.

– At t = 5, the current has reduced to less than 1% of its initial value.

tLRo ReItveIti )/()/( )( )( and

Transient vs. Steady-State Response• The momentary behavior of a circuit (in response

to a change in stimulation) is referred to as its transient response.

• The behavior of a circuit a long time (many time constants) after the change in voltage or current is called the steady-state response.

Review (Conceptual)• Any first-order circuit can be reduced to a

Thévenin (or Norton) equivalent connected to either a single equivalent inductor or capacitor.

– In steady state, an inductor behaves like a short circuit

– In steady state, a capacitor behaves like an open circuit

LRThITh

• Consider the following circuit, for which the switch is closed for t < 0, and then opened at t = 0:

Notation:0– is used to denote the time just prior to switching

0+ is used to denote the time immediately after switching

• The voltage on the capacitor at t = 0– is Vo

Natural Response of an RC Circuit

t = 0+

Solving for the Voltage (t 0)• For t > 0, the circuit reduces to

• Applying KCL to the RC circuit:

• Solution:

RCtevtv /)0()(

Solving for the Current (t > 0)

• Note that the current changes abruptly:

RCtoeVtv /)(

)( 0,for

Time Constant

• In the example, we found that

• Define the time constant

– At t = , the voltage has reduced to 1/e (~0.37) of its initial value.

– At t = 5, the voltage has reduced to less than 1% of its initial value.

RCtoRCto e

VtieVtv // )( )( and

(with R in ohms and C infarads, is in seconds)

Natural Response SummaryRL Circuit

• Inductor current cannot change instantaneously

• time constant

RC Circuit

• Capacitor voltage cannot change instantaneously

• time constantR

/)0()(

)0()0(teiti

/)0()(

)0()0(tevtv

Transient Response of 1st-Order Circuits• We saw that the currents and voltages in RL and RC

circuits decay exponentially with time, with a characteristic time constant , when an applied current or voltage is suddenly removed.

• In general, when an applied current or voltage suddenly changes, the voltages and currents in an RL or RC circuit will change exponentially with time, from their initial values to their final values, with the characteristic time constant as follows:

where x(t) is the circuit variable (voltage or current)xf is the final value of the circuit variablet0 is the time at which the change occurs

This is a very useful equation!

0 )()( tt

ff extxxtx

Procedure for Finding Transient Response

1. Identify the variable of interest• For RL circuits, it is usually the inductor current iL(t)

• For RC circuits, it is usually the capacitor voltage vc(t)

2. Determine the initial value (at t = t0+) of the

variable

• Recall that iL(t) and vc(t) are continuous variables:

iL(t0+) = iL(t0

) and vc(t0+) = vc(t0

• Assuming that the circuit reached steady state before t0 , use the fact that an inductor behaves like a short circuit in steady state or that a capacitor behaves like an open circuit in steady state

Procedure (cont’d)

3. Calculate the final value of the variable (its value as t ∞)

• Again, make use of the fact that an inductor behaves like a short circuit in steady state (t ∞) or that a capacitor behaves like an open circuit in steady state (t ∞)

4. Calculate the time constant for the circuit = L/R for an RL circuit, where R is the Thévenin

equivalent resistance “seen” by the inductor

= RC for an RC circuit where R is the Thévenin equivalent resistance “seen” by the capacitor

Example: RL Transient AnalysisFind the current i(t) and the voltage v(t):

R = 50

Vs = 100 V + L = 0.1 H

1. First consider the inductor current i

2. Before switch is closed, i = 0

--> immediately after switch is closed, i = 0

3. A long time after the switch is closed, i = Vs / R = 2 A

4. Time constant L/R = (0.1 H)/(50 ) = 0.002 seconds

Amperes 22 202)( 500002.0/)0( tt eeti

R = 50

Vs = 100 V + L = 0.1 H

Now solve for v(t), for t > 0:

From KVL, 5022100100)( 500teiRtv

Example: RC Transient AnalysisFind the current i(t) and the voltage v(t):

R2 = 10 kVs = 5 V + C = 1 F

1. First consider the capacitor voltage v

2. Before switch is moved, v = 0

--> immediately after switch is moved, v = 0

3. A long time after the switch is moved, v = Vs = 5 V

4. Time constant R1C = (104 )(10-6 F) = 0.01 seconds

Volts 55 505)( 10001.0/)0( tt eetv

R1 = 10 k

R2 = 10 kVs = 5 V + C = 1 F

555)()(

R1 = 10 k

Now solve for i(t), for t > 0:

From Ohm’s Law,

When we perform a sequence of computations using a digital circuit, we switch the input voltages between logic 0 (e.g. 0 Volts) and logic 1 (e.g. 5 Volts).

The output of the digital circuit changes between logic 0 and logic 1 as computations are performed.

Application to Digital Integrated Circuits (ICs)

• Every node in a real circuit has capacitance; it’s the charging of these capacitances that limits circuit performance (speed)

We compute with pulses.

We send beautiful pulses in:

But we receive lousy-looking pulses at the output:

Capacitor charging effects are responsible!

Digital Signals

Circuit Model for a Logic Gate• Electronic building blocks referred to as “logic gates”

are used to implement logical functions (NAND, NOR, NOT) in digital ICs– Any logical function can be implemented using these gates.

• A logic gate can be modeled as a simple RC circuit:

Vin(t) + C

switches between “low” (logic 0) and “high” (logic 1) voltage states

Transition from “0” to “1”

(capacitor charging)

0.63Vhigh

timeRC

0.37Vhigh

Transition from “1” to “0”

(capacitor discharging)

(Vhigh is the logic 1 voltage level)

Logic Level Transitions

RCthighout eVtV /1)( RCt

highout eVtV /)(

What if we step up the input,

wait for the output to respond,

then bring the input back down?

Sequential Switching

The input voltage pulse width must be long enough; otherwise the output pulse is distorted.

(We need to wait for the output to reach a recognizable logic level, before changing the input again.)

0 1 2 3 4 5Time

Pulse width = 0.1RC

0 1 2 3 4 5Time

0 5 10 15 20 25Time

Pulse Distortion

Vin(t) C+

Pulse width = 10RCPulse width = RC

Suppose a voltage pulse of width5 s and height 4 V is applied to theinput of this circuit beginning at t = 0:

R = 2.5 kΩC = 1 nF

• First, Vout will increase exponentially toward 4 V.

• When Vin goes back down, Vout will decrease exponentially back down to 0 V.

What is the peak value of Vout?

The output increases for 5 s, or 2 time constants.

It reaches 1-e-2 or 86% of the final value.

0.86 x 4 V = 3.44 V is the peak value

Example

= RC = 2.5 s

0 2 4 6 8 10

Vout(t) =4-4e-t/2.5s for 0 ≤ t ≤ 5 s

3.44e-(t-5s)/2.5s for t > 5 s{

A Bit on Second-Order Circuits

A second-order circuit consists of resistors and the equivalent of twoenergy storage elements (Ls, Cs). A second-order circuit is characterizedby a second-order differential equation (contains second-derivatives of time)

Example: A circuit containing R, L and C in series with a voltage source; a circuit with R, L and C in parallel.

Initial and final values of v, i, dv/dt, and di/dt

Example: The switch in this circuit has been closed for a long time. It opens at t = 0. Find: i(0+), v(0+), di(0+)/dt, dv(0+)/dt, i(infinite time), v(infinite time)

a. Values for t < 0

b. Values for t = 0+

c. Values for t = infinity

a. Values for t < 0

b. Values for t = 0+

c. Values for t = infinity

A 2nd Order RLC Circuit

-Cvs(t)

• Application: Filters– A bandpass filter such as IF amplifier for the AM

radio.– A lowpass filter with a sharper cutoff than can

be obtained with an RC circuit.

The Differential Equation

KVL around the loop:

vr(t) + vc(t) + vl(t) = vs(t)

-Cvs(t)

+ -vr(t)

+- vl(t)

1 ( )( ) ( ) ( )

di tRi t i x dx L v t

( )( ) 1 ( ) 1( ) sdv tR di t d i t

i tL dt LC dt L dt

The Differential EquationThe voltage and current in a second order circuit is the solution to a differential equation of the following form:

xp(t) is the particular solution (forced response) and xc(t) is the complementary solution (natural response).

( ) ( )2 ( ) ( )

d x t dx tx t f t

( ) ( ) ( )p cx t x t x t

(the forcing function –

the driving voltage or

current source)

The Particular Solution

• The particular solution xp(t) is usually a weighted sum of f(t) and its first and second derivatives.

• If f(t) is constant, then xp(t) is constant.

• If f(t) is sinusoidal, then xp(t) is sinusoidal

(with the same frequency as the source, for a circuit of only linear elements)

The Complementary Solution

The complementary solution has the following form:

K is a constant determined by initial conditions.s is a constant determined by the coefficients of the differential equation.

( ) stcx t Ke

2 0st st

std Ke dKeKe

2 202 0st st sts Ke sKe Ke

2 202 0s s

Characteristic Equation

• To find the complementary solution, we need to solve the characteristic equation:

• The characteristic equation has two roots-call them s1 and s2.

2 20 0

2 0s s

1 21 2( ) s t s t

cx t K e K e

21 0 0 1s

22 0 0 1s

Overdamped, critically damped and underdamped response ofsource-free transiently excited 2nd-order RLC circuit

Assume circuit is excited by energy stored in C or Lof series RLC circuit.

Assume i(t) = K1es1t + K2es2t where (with slightly different notation)

= R/2L is called the damping factor and is the undamped natural frequency

If > 0 overdamped case aIf = critically damped case bIf < underdamped case c

wheres

EE42/100 Lecture 9 Topics: More on First-Order Circuits Water model and potential plot for RC...

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