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Chapter 7-Resonant Inverters: = 2π × 7500 = 47124 rad/s

Chapter 7 discusses resonant inverters, providing various problems that involve calculations of voltage, current, and frequency parameters related to resonant circuits. Key equations and their applications are presented to determine values such as peak load current, capacitor voltage, and power loss. The chapter emphasizes the relationships between circuit components and their effects on performance metrics in resonant inverter systems.
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0% found this document useful (0 votes)
170 views13 pages

Chapter 7-Resonant Inverters: = 2π × 7500 = 47124 rad/s

Chapter 7 discusses resonant inverters, providing various problems that involve calculations of voltage, current, and frequency parameters related to resonant circuits. Key equations and their applications are presented to determine values such as peak load current, capacitor voltage, and power loss. The chapter emphasizes the relationships between circuit components and their effects on performance metrics in resonant inverter systems.
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
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Chapter 7-Resonant Inverters

Prob 7-1

Given: Vs = 220 V, R = 4 , L = 40 × 10−6 H, C = 4 × 10−6 F, f0 = 7.5 kHz, toff = 15 µs

ω0 = 2π × 7500 = 47124 rad/s;

ωr = = 61237  /
   

∴ = 9746.17 Hz

∴  102.6 
 

α = R/2L = 4/(2×40×10−6) = 50000

a. From Eq. (7.17),


        15.36 
ω    

b. From Eq. (7.18) 7541 

 
c. From Eq. (7.14), Vc = / .  18.33 
From Eq. (7.16), Vc1 = 220 + 18.33 = 238.33 V. The peak-to-peak capacitor voltage is

Vpp = 18.33 + 238.33 = 256.66 V.

d. From Eq. (7.7), the peak load current, which is the same as the peak supply current,
occurs at

tm = 

Chapter 7-Resonant Inverters


Page # 7-1
Prob 7-2
−6 −6
Vs := 220 C1 := 2⋅ 10 C2 := 2⋅ 10 C := C1 + C2

−6 −6 3 −6
C = 4 × 10 L := 40⋅ 10 R := 1.2 fo := 8.5⋅ 10 tq := 15⋅ 10
4
ω o := 2⋅ π ⋅ fo ω o = 5.341 × 10
Using Eq. (7-4)
2
1 R 4
ω r := − ω r = 7.762 × 10
L⋅ C 4⋅ L2

Chapter 7-Resonant Inverters


Page # 7-2
ωr 1
4 −5
fr := fr = 1.235 × 10 Tr := Tr = 8.095 × 10
2⋅ π fr
Using Eq. (7-6)
R 4
α := α = 1.5 × 10
2⋅ L
α⋅π
z := z = 0.607
ωr

Using Eq. (7-17)


π π
( a) toff := − −5
ωo ωr toff = 1.835 × 10
Using Eq. (7-18)
1
fmax := 3
fmax = 9.013 × 10

2⋅ ⎜ tq +
π ⎞
ωr ⎟
Using Eq. (7-14) ⎝ ⎠

Vs
Vc := Vc = 263.439
z
e −1
Vc1 := Vs + Vc Vc1 = 483.439

Vpp := Vc + Vc1 Vpp = 746.878

Using Eq. (7-7)


1 ⎛ ωr ⎞ −5
tm := ⋅ atan ⎜ ⎟ tm = 1.778 × 10
ωr ⎝α⎠
Using Eq. (7-5)
V s + V c − α ⋅ tm
Ip :=
ω r⋅ L
⋅e ( )
⋅ sin ω r⋅ tm Ip = 117.093

Ip
Ips := Ips = 58.547
2

Chapter 7-Resonant Inverters


Page # 7-3
Tr
⌠2 2
⎮ ⎛⎜ Vs + Vc − α ⋅ t ⎞
Io := 2⋅ fo⋅ ⎮ ⋅e ⋅ sin ( ω r⋅ t) ⎟ dt I = 68.232
⎮ ⎜ ω r⋅ L ⎟ o
⌡0 ⎝ ⎠

2 3
Po := Io ⋅ R Po = 5.587 × 10
Po
Is := Is = 25.394
Vs
⎡ Tr ⎤
⎢⌠ 2 ⎥
⎢⎮ ⎛⎜ Vs + Vc − α ⋅ t ⎞ ⎥
( b) IA := fo⋅ ⎢ ⎮ ⋅e ⋅ sin ( ω r⋅ t) ⎟ dt ⎥ IA = 25.394
⎜ ω r⋅ L ⎟
⎢⎮ ⎝ ⎠ ⎥
⎣ ⌡0 ⎦
( c) Ipk := IA Ipk = 25.394

:= IR = 48.247

Chapter 7-Resonant Inverters


Page # 7-4
Where
1 10 6
ωr = = = 81650 𝑟𝑟𝑟𝑟𝑟𝑟/𝑠𝑠
√𝐿𝐿𝐿𝐿 �(5×30)

𝜔𝜔 𝑟𝑟 81650
∴ 𝑓𝑓𝑟𝑟 = = = 12995 𝐻𝐻𝐻𝐻 = 12.99 𝑘𝑘𝐻𝐻𝐻𝐻
2𝜋𝜋 2𝜋𝜋

1 𝑡𝑡 𝑟𝑟
∴ 𝑡𝑡𝑟𝑟 = = 76.95 𝜇𝜇𝑠𝑠 ; 𝑡𝑡1 = = 38.47 𝜇𝜇𝑠𝑠
𝑓𝑓𝑟𝑟 2

5
a. Ip = Vs√(C/L) = 220� = 89.81 A.
30

𝜋𝜋
b. IA = fo∫0 𝐼𝐼𝑝𝑝 sin 𝜃𝜃 𝑟𝑟𝜃𝜃 = Ip fo/(𝜋𝜋𝑓𝑓𝑟𝑟 ) = 44.01 A

c. IR = Ip√(fot1/2) = 89.81×√ (20000×38.47× 10−6 )= 55.703 A.

d. The peak-to-peak capacitor voltage Vpp = Vc1 − Vc = 440 V.

e. From Eq. (7.25), f max = 106/(2 × 15) = 33.33 kHz.

f. Because there is no power loss in the circuit, Is = 0.

Prob 7-4
−6 −6
Vs := 220 C1 := 2⋅ 10 C2 := 2⋅ 10 C := C1 + C2

Chapter 7-Resonant Inverters


Page # 7-5
−6 −6 3
C = 4 × 10 L := 20⋅ 10 R := 1.5 fo := 3.5⋅ 10

4
ω o := 2⋅ π ⋅ fo ω o = 2.199 × 10
Using Eq. (7-4)

2
1 R 5
ω r := − ω r = 1.053 × 10
L⋅ C 4⋅ L2
ωr 1
4 −5
fr := fr = 1.676 × 10 Tr := Tr = 5.965 × 10
2⋅ π fr
Tr 1 −4
−5 To := To = 2.857 × 10
t1 := t1 = 2.983 × 10 fo
2
−4
td := To − Tr td = 2.261 × 10
Using Eq. (7-6)
R 4
α := α = 3.75 × 10
2⋅ L
α⋅π
z := z = 1.119
ωr

Using Eq. (7-14)


Vs
Vc := Vc = 106.78
z
e −1
Vc1 := Vs + Vc Vc1 = 326.78
Using Eq. (7-7)

1 ⎛ ωr ⎞ −5
( a) tm := ⋅ atan ⎜ ⎟ tm = 1.167 × 10
ωr ⎝α⎠
Using Eq. (7-5)
V s + V c − α ⋅ tm
Ip :=
ω r⋅ L
⋅e ( )
⋅ sin ω r⋅ tm Ip = 94.357

Chapter 7-Resonant Inverters


Page # 7-6
⎡ Tr ⎤
⎢⌠ 2 ⎥
⎢⎮ ⎛⎜ Vs + Vc − α ⋅ t ⎞ ⎥
( b) IA := fo⋅ ⎢ ⎮ ⋅e ⋅ sin ( ω r⋅ t) ⎟ dt ⎥ IA = 6.07
⎜ ω r⋅ L ⎟
⎢⎮ ⎝ ⎠ ⎥
⎣ ⌡0 ⎦

t
⌠1 2
⎮ ⎛⎜ Vs + Vc − α ⋅ t ⎞
⋅ sin ( ω r⋅ t) ⎟ dt
( c) IR := fo⋅ ⎮ ⋅e IR = 21.098
⎮ ⎜ ω r⋅ L ⎟
⌡0 ⎝ ⎠

( d) Io := 2⋅ IR Io = 42.196

2 3
( e) Po := Io ⋅ R Po = 2.671 × 10
Po
Is := Is = 12.14
Vs

Prob 7-6
−6 −6 3
Vs := 220 C := 2⋅ 10 L := 20⋅ 10 R := 1.2 fo := 3.5⋅ 10
4
ω o := 2⋅ π ⋅ fo ω o = 2.199 × 10
Using Eq. (7-4)
2
1 R 5
ω r := − ω r = 1.552 × 10
L⋅ C 4⋅ L2
ωr 1
4 −5
fr := fr = 2.471 × 10 Tr := Tr = 4.047 × 10
2⋅ π fr
Tr 1 −4
−5 T o := To = 2.857 × 10
t1 := t1 = 2.024 × 10 fo
2
−4
td := To − Tr td = 2.452 × 10
Using Eq. (7-6)
R 4
α := α = 3 × 10
2⋅ L

Chapter 7-Resonant Inverters


Page # 7-7
α⋅π
z := z = 0.607
ωr

Using Eq. (7-15)


(z )
Vs⋅ e + 1
Vc := Vc = 746.878
z
e −1

Vc1 := Vc Vc1 = 746.878


Using Eq. (7-7)
1 ⎛ ωr ⎞ −6
( a) tm := ⋅ atan ⎜ ⎟ tm = 8.889 × 10
ωr ⎝α⎠
Using Eq. (7-5)
V s + V c − α ⋅ tm
Ip :=
ω r⋅ L
⋅e ( )
⋅ sin ω r⋅ tm Ip = 234.186

⎡ ⌠ t1 ⎤
⎢ ⎮ ⎛⎜ Vs + Vc − α ⋅ t ⎞⎟ ⎥
( b) IA := fo⋅ ⎢ ⎮ ⋅e ⋅ sin ( ω r⋅ t) dt ⎥ IA = 10.456
⎜ ω r⋅ L ⎟
⎢⎮⌡0 ⎝ ⎠ ⎥
⎣ ⎦
t
⌠1 2
⎮ ⎛⎜ Vs + Vc − α ⋅ t ⎞
⋅ sin ( ω r⋅ t) ⎟ dt
( c) IR := fo⋅ ⎮ ⋅e IR = 43.783
⎮ ⎜ ω r⋅ L ⎟
⌡0 ⎝ ⎠

( d) Io := 2⋅ IR Io = 87.567

2 3
( e) Po := Io ⋅ R Po = 9.202 × 10
Po
Is := Is = 41.825
Vs

Chapter 7-Resonant Inverters


Page # 7-8
Prob 7-7
a. Because at resonance u = 1 and | ω  |max = 1, the peak fundamental load voltage
is Vp = Vi(pk) = 4Vs/π.

PL =Vp 2/2R = 42Vs2/2Rπ2 or 3000 = 42Vs2/2π2 × 7

which gives Vs = 160.9 V.

b. To reduce the load power by (3000/1500 = ) 2, the voltage gain must be reduced by 1.414 at u
= 0.8.

That is, from Eq. (7.35), we get 1 + Qs2(u − 1/u)2 = 2, which gives Qs = 2.22.

c. Qs is defined by

Qs = ω0L/R or 2.22 = 2π × 30 kHz × L/7

which gives L = 82.44 µH.

d. f0 = 1/2π√ LC) or 30 kHz = 1/[2π(√ 82.44 µH × C)], which gives C = 0.341 µF.

Prob 7-8
3 3
PL := 2⋅ 10 Vp := 330 R := 6.5 fo := 25⋅ 10 PRQ := 500

⎛ P ⋅ 2⋅ π 2⋅ R⎞
Vs := ⎝ L ⎠ Vs = 126.642
( a) 4

4⋅ Vs
Vi :=
π Vi = 161.245
Vp
( b) Q :=
Vi Q = 2.047
PL
x := x=4
PRQ

Guess
u := 1.
Given
2
(1 − u )
2
2
+ ⎛⎜ ⎞⎟ = x
u
⎝Q⎠

Chapter 7-Resonant Inverters


Page # 7-9
Uval := Find ( u)
u := Uval u = 1.68

R
( c) L := −5
2⋅ π ⋅ fo⋅ Q L = 2.022 × 10

1
( d) C := −6
C = 2.004 × 10
( 2⋅ π ⋅ fo) ⋅ L
2

Prob 7-9

a. Because at resonance u = 1 and |Z ω  |max = 1, the peak fundamental load current


is Ip = Ii(pk) = 4Is/π.
PL =Ip 2R/2 = 42Is2R/(2π2) or 3000 =42Is2×7.5/(2π2)
which gives Is = 22.21 A.

b. To reduce the load power by (3000/1500 = ) 2, the current gain must be reduced by 1.414 at u
= 1.25. That is, from Eq. (7.35), we get 1 + Qp2(u − 1/u)2 = 2, which gives Qp = 2.22.

c. Qs is defined by
Qs = ω0L/R or 2.22 =2π × 30 kHz × L/7.5
which gives L = 88.33 µH.

d. f0 = 1/2π√ LC) or 30 kHz = 1/[2π(√ 88.33µH × C)], which gives C = 0.3 µF.

Prob 7-10
3
Vs := 18 R := 5 fs := 50⋅ 10 k := 0.304 Q := 7
5
ω s := 2⋅ π ⋅ fs ω s = 3.142 × 10

0.4001⋅ R −6
Le := Le = 6.368 × 10
ωs
2.165 −6
Ce := Ce = 1.378 × 10
R⋅ ω s

Chapter 7-Resonant Inverters


Page # 7-10
Q⋅ R −4
L := L = 1.114 × 10
ωs
1 −8
C := C = 9.578 × 10
(
ω s⋅ ω s⋅ L − 0.3533⋅ R )
R C
δ := ⋅ δ = 0.073
2 L

1 4
fo := fo = 4.872 × 10
2⋅ π ⋅ L⋅ C

Prob 7-11
−3 3
Vm := 12 ΔVm := 20⋅ 10 fo := 350⋅ 10
PL := 1.5 Vo := 5

−9 −8
( a) Let C := 10⋅ 10 C = 1 × 10

1
L := −5
L = 2.068 × 10
(
C⋅ 2⋅ π ⋅ fo ) 2

2
Vo
R := R = 16.67
PL
Vo
Io := Io = 0.3
R
Io
Cf := −5
2⋅ fo⋅ ΔVm Cf = 2.14 × 10
Vm
( b) Im := Im⋅ 1000 = 720 mA
R

2
Im
2
IL_rms := Io + IL_rms⋅ 1000 = 590.931 mA
2

IL_dc := Io IL_dc⋅ 1000 = 300 mA

Chapter 7-Resonant Inverters


Page # 7-11
Im
IC_rms :=
2 IC_rms⋅ 1000 = 509.117 mA

IC_dc := 0 IC_dc = 0

Prob 7-12

x = 1.5, Vs = 15 V, f = fmax = 50 kHz, and T = 1/50 kHz = 20 µs. PL = VoIo or 2.5 W = 9Io, which
gives Io = 0.277 A.

The maximum frequency occurs when t5 = 0. Because t1 = t3 = t5 = 0, t2 + t4 = T. Substituting


t4 = 2VsC/Im and using x = (Vs/Io)√(C/L) gives:
2 2
√           

which gives C = 0.0902 µF.

Thus, L = (Vs/xIo)2C = 117.56 µH.

Prob 7-13

Vo := 5 Vs := 15 3
PL := 1 f := 40⋅ 10
−6 −6 1
L := 150⋅ 10 C := 0.02⋅ 10 ω o :=
L⋅ C 5
ω o = 5.774 × 10
PL
Io := Io = 0.2
Vo

Using Eq. (7-56)

( a) L
Vp := Io⋅ + Vs Vp = 32.321
C

Chapter 7-Resonant Inverters


Page # 7-12
Ip := Io
Ip = 0.2
C
( b) t1 := Vs⋅ −6
Io t1 = 1.5 × 10

−6
t2 := π ⋅ L⋅ C t2 = 5.441 × 10

Vs C
x := ⋅ x = 0.866
Io L

t3 := L⋅ C⋅ asin ( x) −6
t3 = 1.814 × 10

(
IL3 := −Io⋅ cos ω o⋅ t3 ) IL3 = −0.1

L
(
t4 := Io − IL3 ⋅
Vs
) t4 = 3 × 10
−6

(
t5 := T − t1 + t2 + t3 + t4 ) t5 = 1.324 × 10
−5

Chapter 7-Resonant Inverters


Page # 7-13

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