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Fundamentals of Power Electronics. 1. Chapter 19: Resonant Conversion. Announcements ... Inverter is capable of producing a peak open circuit output voltage of 400 V ... – PowerPoint PPT presentation

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Title: Announcements


1
Announcements
  • Homework 2 due today for on-campus students.
    Off-campus students submit according to your own
    schedule.
  • Homework 3 is posted and is due NEXT Friday for
    on-campus students (Friday Feb. 8)

2
19.4 Load-dependent propertiesof resonant
converters
  • Resonant inverter design objectives
  • 1. Operate with a specified load characteristic
    and range of operating points
  • With a nonlinear load, must properly match
    inverter output characteristic to load
    characteristic
  • 2. Obtain zero-voltage switching or zero-current
    switching
  • Preferably, obtain these properties at all loads
  • Could allow ZVS property to be lost at light
    load, if necessary
  • 3. Minimize transistor currents and conduction
    losses
  • To obtain good efficiency at light load, the
    transistor current should scale proportionally to
    load current (in resonant converters, it often
    doesnt!)

3
Inverter output characteristics
  • General resonant inverter output characteristics
    are elliptical, of the form

This result is valid provided that (i) the
resonant network is purely reactive, and (ii) the
load is purely resistive.
4
A Theorem relating transistor current variations
to load resistance R
  • Theorem 1 If the tank network is purely
    reactive, then its input impedance Zi is a
    monotonic function of the load resistance R.
  • So as the load resistance R varies from 0 to ?,
    the resonant network input impedance Zi
    varies monotonically from the short-circuit
    value Zi0 to the open-circuit value Zi?
    .
  • The impedances Zi? and Zi0 are easy
    to construct.
  • If you want to minimize the circulating tank
    currents at light load, maximize Zi? .
  • Note for many inverters, Zi? lt Zi0 !
    The no-load transistor current is therefore
    greater than the short-circuit transistor current.

5
Example Zi of LCC
  • for f lt f m, Zi increases with increasing R
    .
  • for f gt f m, Zi decreases with increasing R
    .
  • for f fm, Zi constant for all R .
  • at a given frequency f,  Zi is a monotonic
    function of R.
  • Its not necessary to draw the entire plot just
    construct Zi0 and  Zi? .

6
A Theorem relating the ZVS/ZCS boundary to load
resistance R
  • Theorem 2 If the tank network is purely
    reactive, then the boundary between zero-current
    switching and zero-voltage switching occurs when
    the load resistance R is equal to the critical
    value Rcrit, given by

It is assumed that zero-current switching (ZCS)
occurs when the tank input impedance is
capacitive in nature, while zero-voltage
switching (ZVS) occurs when the tank is inductive
in nature. This assumption gives a necessary but
not sufficient condition for ZVS when significant
semiconductor output capacitance is present.
7
LCC example
  • f gt f? ZVS occurs for all R
  • f lt f0 ZCS occurs for all R
  • f0 lt f lt f?, ZVS occurs for Rlt Rcrit, and ZCS
    occurs for Rgt Rcrit.
  • Note that R Zo0 corresponds to operation
    at matched load with maximum output power. The
    boundary is expressed in terms of this matched
    load impedance, and the ratio Zi? / Zi0.

8
LCC example, continued
Typical dependence of Rcrit and matched-load
impedance Zo0 on frequency f, LCC example.
Typical dependence of tank input impedance phase
vs. load R and frequency, LCC example.
9
19.4.4 Design Example
  • Select resonant tank elements to design a
    resonant inverter that meets the following
    requirements
  • Switching frequency fs 100 kHz
  • Input voltage Vg 160 V
  • Inverter is capable of producing a peak open
    circuit output voltage of 400 V
  • Inverter can produce a nominal output of 150 Vrms
    at 25 W

10
Solve for the ellipse which meets requirements
11
Calculations
The required short-circuit current can be found
by solving the elliptical output characteristic
for Isc
hence
Use the requirements to evaluate the above
12
Solve for the open circuit transfer function
  • The requirements imply that the inverter tank
    circuit have an open-circuit transfer function of

Note that Voc need not have been given as a
requirement, we can solve the elliptical
relationship, and therefore find Voc given any
two required operating points of ellipse. E.g.
Isc could have been a requirement instead of Voc
13
Solve for matched load (magnitude of output
impedance )
  • Matched load therefore occurs at the operating
    point

Hence the tank should be designed such that its
output impedance is
14
Solving for the tank elementsto give required
Zo0 and Hinf
  • Lets design an LCC tank network for this example

The impedances of the series and shunt branches
can be represented by the reactances
15
Analysis in terms of Xs and Xp
  • The transfer function is given by the voltage
    divider equation

The output impedance is given by the parallel
combination
Solve for Xs and Xp
16
Analysis in terms of Xs and Xp
17
Hinf
18
Zo0
19
Zo0
20
Analysis in terms of Xs and Xp
21
Analysis in terms of Xs and Xp
  • The transfer function is given by the voltage
    divider equation

The output impedance is given by the parallel
combination
Solve for Xs and Xp
22
Evaluate tank element values
23
DiscussionChoice of series branch elements
  • The series branch is comprised of two elements L
    and Cs, but there is only one design parameter
    Xs 733 ?. Hence, there is an additional degree
    of freedom, and one of the elements can be
    arbitrarily chosen.
  • This occurs because the requirements are
    specified at only one operating frequency. Any
    choice of L and Cs, that satisfies Xs 733 ?
    will meet the requirements, but the behavior at
    switching frequencies other than 100 kHz will
    differ.
  • Given a choice for Cs, L must be chosen according
    to

For example, Cs 3Cp 3.2 nF leads to L 1.96
mH
24
Requirements met at one frequency
25
What if Cs infinity?
26
DiscussionChoice of series branch elements
  • The series branch is comprised of two elements L
    and Cs, but there is only one design parameter
    Xs 733 ?. Hence, there is an additional degree
    of freedom, and one of the elements can be
    arbitrarily chosen.
  • This occurs because the requirements are
    specified at only one operating frequency. Any
    choice of L and Cs, that satisfies Xs 733 ?
    will meet the requirements, but the behavior at
    switching frequencies other than 100 kHz will
    differ.
  • Given a choice for Cs, L must be chosen according
    to

For example, Cs 3Cp 3.2 nF leads to L 1.96
mH
27
Rcrit
  • For the LCC tank network chosen, Rcrit is
    determined by the parameters of the output
    ellipse, i.e., by the specification of Vg, Voc,
    and Isc. Note that Zo? is equal to jXp. One can
    find the following expression for Rcrit

Since Zo0 and H ? are determined uniquely by the
operating point requirements, then Rcrit is also.
Other, more complex tank circuits may have more
degrees of freedom that allow Rcrit to be
independently chosen. Evaluation of the above
equation leads to Rcrit 1466 ?. Hence ZVS for
R lt 1466 ?, and the nominal operating point with
R 900 ? has ZVS.
28
Rcrit
29
Ellipse again with Rcrit, Rmatched, and
RnomShowing ZVS and ZCS
30
Converter performance
  • For this design, the salient tank frequencies are
  • (note that fs is nearly equal to fm, so the
    transistor current should be nearly independent
    of load)

The open-circuit tank input impedance is
So when the load is open-circuited, the
transistor current is
Similar calculations for a short-circuited load
lead to
31
Extending ZVS range
32
Extending ZVS range
33
Extending ZVS range
34
Discussion wrt ZVS and transistor current
scalingSeries and parallel tanks
  • fs above resonance
  • No-load transistor current 0
  • ZVS
  • fs below resonance
  • No-load transistor current 0
  • ZCS
  • fs above resonance
  • No-load transistor current greater than short
    circuit current
  • ZVS
  • fs below resonance but gt fm
  • No-load transistor current greater than short
    circuit current
  • ZCS for no-load ZVS for short-circuit
  • fs lt fm
  • No-load transistor current less than short
    circuit current
  • ZCS for no-load ZVS for short-circuit

35
Discussion wrt ZVS and transistor current
scalingLCC tank
  • fs gt finf
  • No-load transistor current greater than short
    circuit current
  • ZVS
  • fm lt fs lt finf
  • No-load transistor current greater than short
    circuit current
  • ZCS for no-load ZVS for short-circuit
  • f0 lt fs lt fm
  • No-load transistor current less than short
    circuit current
  • ZCS for no-load ZVS for short-circuit
  • fs lt f0
  • No-load transistor current less than short
    circuit current
  • ZCS
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