To provide output at constant current and voltage there are two main answers
The energy in capacitor = 0.5 x C x V^2
If voltage falls from V1 to V2 then the energy extracted =
0.5 x C x V1^2 - 0,.5 x C x V2^2
= 0.5 x C x (V1^2 - V2^2)
[= for interest : 0.5 x (V1-V2) x (V1+V2)
If Vcap falls by a factor of 4 from Vstart to Vstart/4
E total = 0.5 x C x Vs^2
Energy fro Vs to Vs/4 extraction = 0.5 x C x Vs^2(1-1/16)
= 15/16ths of available energy = most of it.
ie for voltage falling to 1/nth of initial the energy left is Eoriginal x 1/N^2.
This means that say V falling from 12v to 4V (N=3) means only 1/9th is left.
Even for V falling from say 10V to 5V, N=2. Energy left = 25%. Energy used = 75%!
With a Buck converter:
This assumes that Vcap falls to Vout+Vdropout.
The equations below also work for a buck-boost converted with Vcap < Vout.
For a buck-boost converter Vcao can fall to below Vout.
Efficiency in boost mode is usually lower than buck efficiency and usually falls further as Vcal gets very low. As for Vcap = Vinial/4 remaining energy is only 1/16th of initial , there is not usually great advantage in using very low cap voltages.
even for eg 5V6 to 3v3 Out + 0.2 V dropout, remaining energy at the start of boost mode is only 40% of initial. For say 10V to 3.3 + 0.3 remaining efficiency is only 12% of initial.
Energy available = total capacitor loss x efficiency.
0 < efficiency < 1 -> usually in the 0.7 - 0.9 range.
In the following calculations efficieny is assumed as 100%.
Scale answers down linearly by actual efficiency - say start with 0.8 as typical.
Real world efficiencies of some converters can be in the 0.90 - 0.95 range (or even better) BUT this is usually across a restricted load and Vin/Vout range. Starting at 80% and increasing if a "sweet spot" can be managed for a given application is less liable to lead to disappointment.
Assume regulator has NO dropout voltage.
Assume regulator proper is 100% efficient .
Energy will be lost as heat when voltage drops across regulator.
Energy available = 0.5 x C x (Vstart^2 - Vreg_out^2)
For a low dropout regulator with Vin_min is say Vout+0.2V then the above is about right.
If dropout voltage is significant then
Energy available = 0.5 x C x (Vstart^2 - (Vreg_out+Vdropout)^2)
eg using:
10,000 uF = 10 mF = 0.01F capacitor
Vstart = 5.4.
Vout = 3V3.
Vdropout = 0.2V
Energy available = 0.5 x C x (5.4^2 - (3.3+0.2)^2)
= 0.5 x 0.01 x (29.16-12.25) = 0.08455 Joule
= 84.55 mJ
1J = 1A x 1V x 1S = 1 A.V.s
or 1 mA.V.S
So 84.55 mJ = 25.6s x 1 mA x 3.3V
Or 2.56s x 10 mA x 3.3 V or ...
Increase the capacitor to say 1F and you get about 8.5J or 8500 mJ and it starts to "get useful"
eg 8500 / 3.3V / 3600s = 0.715 mA for 1 hour.
Linear.
For a given Vout and Out, current is drained at constant I.
Energy lost is (Vin-Vout-Vdropout) x Iout.
As cap voltage approaches Vout efficincy approaches 100%.
Initially Efficiency is Vout/Vin_initial.
Total cap energy remaining is 0.5 x C x (Vout+Vdropout)^2
As a fraction of total initial energy = (Vout+Vdropout)^2/Vinitial^2
For small Vinitial/Vout drops much energy remains when Vcap = Vout.
Delta_V_cap = dV = T x I / C
dV = V = drop in capacitor voltage - Volts
T - Time - seconds
I - current - Amps
C - Capacitance - Farad
Or
V = TI / C
T = VC / I
C = TI / V
I = VC / T
Allowed drop = Vinitial - Vout - dropout_voltage
Eg 10 F cap, 20 mA, allowed drop = 5V6 to 3V3, dropout = 0.2V.
T = V/IC = (5.4-3.3-0.2) /(0.02 x 10) = 1.9 /0.2 = 9.5 seconds.
or, using above buck converter example:
10,000 uF = 10 mF = 0.01F capacitor
Vstart = 5.4.
Vout = 3V3.
Vdropout = 0.2V
I = 1 mA
T = VC/I = 1.9 x 0.01 /0.001 = 19 seconds
Compared with the 25.6s with the buck regulator AT 100% efficiency
To "break even" the buck regulator would need an efficiency of > 19/25.6 ~= 74%
This would usually be achievable BUT the difference is closer than may be expected.
As Vinitial to Vout ratios rise the buck converter becomes a clear winner.
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