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LDO design technique

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LDO Deisgn
Santosh kumar Nov20
Design specifications: LDO with low output capacitor
S.No
Parameter
Value
units
1
LDO output
1.2+/-5%
V
2
Output current
10
mA
3
No load current(pass gate)
33
uA
4
Reference output
0.7
V
5
Output capacitance
Max:200
Min: 80
pF
4
Phase margin
Min:35
Deg
5
Gain margin
Min:-5
dB
6
PSR overshoot
Max:0
dB
Design: Error Amplifier
1. Error amplifier has with 8u A tail
current with supply 1.5v and input
common mode is 0.7v i.e from vref.
Design: overall LDO with out compensation
1.Ldo consist of error amplifier, pass gate and
resistive divider.
2. Both pass gate and resistive divider
connected in feedback fashion
3. Sizes of resistor is determined from non
𝑅
inverting amp Vout=vref(1+𝑅2) configuration
1
4. The resistor ratio will come from above
𝑅
equation i.e 𝑅2
1
5. Vout 1.2v and current at no load 30u A
gives R1+R2, finally we get both R1 and R2
values 21k,15k
6. Size of pass gate is done at full load
condition and with slow process corner at high
temp(150 deg)
Design: LDO with internally compensated
1. Ldo with source follower compensation to improve the
stability of Ldo.
2. By the addition of extra source follower, it
cancels
right half plane zero (gm6/Cgd).
3. New pole locations are
πœ”π‘1 =
πœ”π‘2 =
πœ”π‘§ =
1
π‘”π‘šπ‘π‘Žπ‘ π‘  ∗ π‘…π‘œπ‘’π‘‘,𝐸𝐴 ∗ 𝑅1 + 𝑅2 π‘…π‘™π‘œπ‘Žπ‘‘ π‘Ÿπ‘‘π‘ , π‘π‘Žπ‘ π‘  ∗ 𝐢𝐢
π‘”π‘š,π‘π‘Žπ‘ π‘ 
πΆπ‘™π‘œπ‘Žπ‘‘
−π‘”π‘š,𝑆𝐹
𝐢𝐢
Test bench: LDO with internally compensated DC and Stability analysis
ADE XL setup
ADE XL Setup
Corner setup
DC gain: No Load condition
Phase: No Load condition
Unity Gain Bandwidth: No Load condition
Gain margin: No Load condition
Phase margin: No Load condition
Regulated output: No Load condition
DC gain: Full Load condition
Phase: Full Load condition
Unity Gain Bandwidth: Full Load condition
Gain margin: Full Load condition
Phase margin: Full Load condition
Regulated output: Full Load condition
Test bench: LDO with internally compensated Transient Variations
Regulator output: tr and tf =1us typ corners
Regulator output: tr and tf =1us typ corners
Regulator output: tr and tf =5us typical corners
Regulator output: tr and tf =1us
Regulator output: tr and tf =5us typ corners
Regulator output: tr and tf =5us
Test bench: LDO with internally compensated PSR
LDO : power supply rejection at no load(rload=1M ohms)
LDO : power supply rejection at full load(rload=120 ohms)
Gain error and Settling time: model of LDO
Gain error and Settling time: model of LDO
Gain error and Settling time: model of LDO
Gain error and Settling time: model of LDO
Gain error and Settling time: model of LDO
Gain error and Settling time: model of LDO
Gain error and Settling time: model of LDO
Gain error and Settling time: model of LDO
Effect of finite risetime in single pole system
Ideal
1. Time Constant T= RC=1k*1u=1m Sec
Effect of finite risetime in single pole system
Effect of finite risetime in single pole system
Effect of finite risetime
S.No
Rise time(βˆ†tr)
Input delay(π’•π’Šπ’π’‘π’–π’•,𝟏τ )
Output delay(𝒕𝒐𝒖𝒕𝒑𝒖𝒕,𝟏τ )
Delay=𝒕𝒐𝒖𝒕𝒑𝒖𝒕,𝟏τ-π’•π’Šπ’π’‘π’–π’•,𝟏τ
units
1
1u
632.1n
1.001m
1m
Sec
2
2u
1.264u
1.001m
1m
Sec
3
4u
2.528u
1.002m
999.44u
Sec
4
10u
6.321u
1.005m
998.8u
Sec
5
50u
31.6u
1.026m
994.4u
Sec
6
100u
63.21u
1.051m
987.8u
Sec
βˆ†tr
π’•π’Šπ’π’‘π’–π’•,𝟏τ=0.632*βˆ†tr
𝒕𝒐𝒖𝒕𝒑𝒖𝒕,𝟏τ=τπ’Šπ’…π’†π’‚π’ +
𝟎. πŸ“βˆ†tr
Delay=~ τπ’Šπ’…π’†π’‚π’ - 0.132βˆ†tr
Effect of finite risetime
S.No
Rise
time(βˆ†tr)
Theoretical calculation
simulation
unit
s
Input
delay(π’•π’Šπ’π’‘π’–π’•,𝟏τ )
Output
delay(𝒕𝒐𝒖𝒕𝒑𝒖𝒕,𝟏τ )
Delay=𝒕𝒐𝒖𝒕𝒑𝒖𝒕,𝟏τ -π’•π’Šπ’π’‘π’–π’•,𝟏τ
Input
delay(π’•π’Šπ’π’‘π’–π’•,𝟏τ
Output
delay(𝒕𝒐𝒖𝒕𝒑𝒖𝒕,𝟏τ )
Delay=𝒕𝒐𝒖𝒕𝒑𝒖𝒕,𝟏τ π’•π’Šπ’π’‘π’–π’•,𝟏τ
1
1m
632.1u
1.5m
868u
632.1u
1.519m
886.9u
Sec
2
2m
1264u
2m
736u
1264u
2.158m
914u
Sec
3
3m
1896u
2.5m
604u
1896u
2.837m
941.5u
Note: Above equation is valid only when rise time< 1τ(for smaller time constants)
It verified with other time constant circuits also
Capacitor charging with current step
βˆ†π‘‰π‘œπ‘’π‘‘ =
𝐼𝑠𝑑𝑒𝑝 ∗ βˆ†π‘‘
πΆπ‘œπ‘’π‘‘
Calculation:
Iavg= 0.5m A
βˆ†π‘‘=1u Sec
Cout=200p F
βˆ†π‘‰π‘œπ‘’π‘‘ =2.5 V
Capacitor charging with current step
Load transient analysis of LDO
• Sudden rise current step of iLoad which creates voltage undershoot and
overshoot at output voltage, it will be regulated after loop response time
• The change in undershoot or overshoot approximately defined
βˆ†π‘‰π‘œπ‘’π‘‘ =
πΌπ‘™π‘œπ‘Žπ‘‘π‘Žπ‘£π‘”
π‘π‘œπ‘’π‘‘
1
(
2πœ‹π‘ˆπΊπΉ
+
𝐢𝑔 𝑉𝑔
𝐼𝑠𝑙𝑒𝑀
)
πΌπ‘™π‘œπ‘Žπ‘‘π‘Žπ‘£π‘” =0.5m A
cout=200p
UGF at no load=906K Hz
Cgg=620f F
Vg=145m V
Islew=5.3m A
=484.5m V
Load transient analysis of LDO
Load transient analysis of LDO
• Change in output voltage βˆ†π‘‰π‘œπ‘’π‘‘ due sudden current step(βˆ†πΌπ‘™π‘œπ‘Žπ‘‘)
The voltage scaled at the feedback network
• βˆ†Vf= 𝛽 βˆ†π‘‰π‘œπ‘’π‘‘ ……………..(1)
This change in voltage generated the current called as Ix
• βˆ†πΌπ‘₯ = π‘”π‘š1,2 βˆ†π‘‰π‘“ ……………(2)
• The output voltage at error amplifier for that we need to find output impedance π‘π‘œπ‘’π‘‘
• Let unity gain frequency and dc gain is available so that we will get first pole location i.e
• πœ”π‘1 =
π΄π‘œ πœ”π‘œ
π΄π‘œ
=>
1
π‘…π‘œπ‘’π‘‘,𝐸𝐴 πΆπ‘œπ‘’π‘‘,𝐸𝐴
• πΆπ‘œπ‘’π‘‘,𝐸𝐴 = 𝐢𝐢 𝐴𝑣2
• π‘…π‘œπ‘’π‘‘,𝐸𝐴 =
(𝐴𝑣2 =π‘”π‘š,π‘π‘Žπ‘ π‘  π‘…π‘œπ‘’π‘‘,π‘π‘Žπ‘ π‘  )
1
πœ”π‘1 ∗πΆπ‘œπ‘’π‘‘,𝐸𝐴
1
Finally π‘π‘œπ‘’π‘‘ = π‘…π‘œπ‘’π‘‘,𝐸𝐴 || π‘†πΆπ‘œπ‘’π‘‘
𝐸𝐴
at 3 dB frequency
Load transient analysis of LDO
• Change in current at error amplifier provides the voltage at pass gate
• 𝑉𝑔,π‘π‘Žπ‘ π‘  = βˆ†πΌπ‘₯ ∗ π‘π‘œπ‘’π‘‘,𝐸𝐴
Voltage change at gate of pass gate circuit creates current change in βˆ†πΌπ‘π‘Žπ‘ π‘ 
βˆ†πΌπ‘π‘Žπ‘ π‘  = π‘”π‘š,π‘π‘Žπ‘ π‘  ∗ 𝑉𝑔,π‘π‘Žπ‘ π‘ 
The discharge current pass through the capacitor is βˆ†πΌπΏπ‘œπ‘Žπ‘‘ − βˆ†πΌπ‘π‘Žπ‘ π‘ 
βˆ†πΌπ‘π‘Žπ‘ π‘  −βˆ†πΌπΏπ‘œπ‘Žπ‘‘ ∗ βˆ†t
βˆ†π‘‰π‘œπ‘’π‘‘ =
𝐢
π‘œπ‘’π‘‘
Verifications:
Current step βˆ†πΌπ‘™π‘œπ‘Žπ‘‘ = 1π‘š 𝐴 π‘Žπ‘›π‘‘ π‘€π‘–π‘‘β„Ž βˆ†π‘‘ = 1𝑒 𝑑𝑒𝑒 π‘‘π‘œ π‘‘β„Žπ‘’π‘ π‘’ π‘β„Žπ‘Žπ‘›π‘”π‘’ 𝑖𝑛 βˆ†π‘‰π‘œπ‘’π‘‘
Load transient analysis of LDO
Load transient analysis of LDO
Load transient analysis of LDO
Load transient analysis of LDO
Low dropout regulator : Noise analysis
Low dropout regulator : Detail Noise Contributions
Noise contribution of Ldo elements
Noise Contributed by Pass Gate
1.Major contribution of noise is differential pair (M1 and M2 )
2. Pass gate noise was diminished by larger size
3. Input noise of second stage was attenuated by first stage differential pair
Summary of LDO design
S.No
Parameter
Value
1
Supply
1.5V
2
Technology
0.18u UMC CMOS
3
Output
1.2V
4
Gain@ No load
Gain@ Full load
62dB
49.5dB
5
UGB@ No load
UGB@ Full load
1.06M Hz
1.105M Hz
6
PM@ No load
PM@ Full load
62 deg
102 deg
7
GM @ No load
GM @ Full load
59dB
57dB
8
Quiescent
current(iq)
93u A
9
1.
2.
3.
4.
Error amplifier 10u A
Bleeder current 35u A
Voltage buffer compensation 5u A
Pull down circuit 40u A
PSR@ No load
-57.4dB at DC(min)
-69mdb at UGB(max)
PSR@ Full load
-45.36dB at DC(min)
-60m dB max
10
Settling time(ts)|
98%
1.04u Sec
11
Load Transient
(1m A/1u Sec)
βˆ†π‘‰1 =41m V (< 5% vout i.e 60m), βˆ†π‘‘1 = 282.56𝑛 𝑆𝑒𝑐
12
Input referred
noise
61u V/ 𝐻𝑧
compensation with simple miller compensation
• Simple miller compensation:
Frequency response : simulation
Frequency response : simulation No Load
PSR Simulation
1. A higher ROEA undoubtedly provides a better PSRR at low frequency. However,
the PSRR in the moderate frequency range is degraded seriously.
2. AEA and RESR take a significant role on improving the PSRR. A larger AEA could
gain a better PSRR at low to moderate frequency, while a smaller RESR could
achieve PSRR enhancement at moderate to high frequency.
3. Finally, the worst PSRR happens at maximum IO.
PSR: simulation No Load
PSR: simulation No Load variation with Error amplifier gain
PSR: simulation No Load variation with R ESR
LDO with miller compensation : load transient
Ldo with Ahuja compensation
Improvement of frequency response:
1. Complex non-dominant poles with small damping factors are
undesirable because those can cause loss in phase and/or gain margins,
poor transient behavior and, in extreme cases
2. for large values of gm3 needs to be high and/or CC small.
3. The zero in the circuit is usually located just before the complex poles
and the resulting magnitude curve shows pronounced peaking after the
unity-gain crossover
Frequency response of LDO: no load
PM=90deg
GM=28.13dB
PSR response of LDO: no load
Transient performance of LDO ahuja
14 bit accuracy:
𝑑1
1
πœπ‘ˆπΊπ΅ = 𝑁∗ln(2)
here πœπ‘ˆπΊπ΅ = 2∗πœ‹∗𝑓
π‘ˆπΊπ΅
Settling time= 1.96u sec (calculated)
form simulation π‘“π‘ˆπΊπ΅ = 790π‘˜ 𝐻𝑧
Ldo Ahuja compensation with gm boosting
Loop1
Outer loop
Loop2
Inner loop
Frequency response of LDO: outer loop no load
PM=90deg
GM=28.13dB
Frequency response of LDO: inner loop no load
PM=90deg
GM=28.13dB
PSR response of LDO: no load
Transient performance of LDO ahuja
14 bit accuracy:
𝑑1
1
πœπ‘ˆπΊπ΅ = 𝑁∗ln(2)
here πœπ‘ˆπΊπ΅ = 2∗πœ‹∗𝑓
π‘ˆπΊπ΅
Settling time= 1.23u sec (calculated)
form simulation π‘“π‘ˆπΊπ΅ = 1.25𝑀 𝐻𝑧
Comparison of LDO: Miller , Ahuja and Ahuja with gm boosting
Parameter
Miller
Ahuja
Ahuja with gm boosting
Second
pole
1.37 M Hz
7.1M Hz
41M Hz
PSR @DC
55dB
-46dB
-32dB
PSR@UGB
-390m dB
-18dB
-18dB
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