I understand your conviction but sorry you will want to revise your outlook on this. Last attempt to explain -
suppose you can charge a cap with a high voltage source, but stop charging when it reaches a lower voltage. The cap itself is never subjected to a high voltage in this situation (this is certain). It will receive current at the voltage it is at, and the power transferred to it will be the current * its voltage. No fast charging magic present.
You cannot charge a battery or capacitor (directly) at voltages higher than their own voltage.
If source voltage is suitable, resistive current limiting is plausible, but power is dissipated by resistance (within the cap and path to it) proportional to the square of the current. This is why efficient voltage transformation is required if source has a significantly higher potential.
ok I see it, but this statement is just fundamentally wrong here:
capacitor can be charged at any voltage as long as you cut off the supply when the voltage across the capacitor reaches a certain threshold
The cap in your circuit is not charging at any voltage, it is charging at Vn001 - its own voltage (the electrical potential created by virtue of its capacitance). In your circuit the only modelled resistance (and the drop in voltage between supply and the cap) is across R1.
This is all to explain the point which you disagreed with but is iron cast - you cant run power into a phone at 50volts to fast charge its 4volt battery without a missing, quite impossibly cool and small voltage transformer inside the phone to make the idea work.
Im not pointing this out to you to win an argument, Im explaining something which I didnt understand either when I began experimenting with ltspice and making charge circuitry. Take the advice or leave it now, but if you keep on with electronics you will find out sooner or later - "power stores charge and discharge > directly < at their own voltages" and if you dont have enough resistance between different electric potentials - take heed 'fun' will ensue of the dwarven kind ;)
To me the fundamentals have always been based on batteries being chemical reactions with their characteristic cell voltages. A cell definitely has its own discharge voltage, and can be used as a reference because the voltage remains relatively unchanged until the available chemicals are becoming effectively exhausted. It is an energy source based on the amount of chemicals available, plus a storage medium based on the reliable reversibility of the reaction.
In the case of rechargeable batteries, the desired reverse reaction can often be best obtained by carefully matching the recharge voltage & current dynamically, against the quantity of chemical you wish to react, including the amount undischarged and remaining to be reacted at any time. The recharge/maintenance voltages will need to be above the discharged/characterisitc voltages any time that cell recharging is expected to occur. The upper limit on charging voltage is based on the cell's characteristic voltage & the ability of the particular chemical system to withstand overvoltage. This is an electrochemical limit. The electrodes are separated by an electrolyte where having a low DC resistance is a desired property. As to the polarity of the DC voltage being provided or stored, this should always be respected, at your peril.
The working voltage of a battery cell can not be adjusted to match a particular circuit, the circuits must instead be closely designed to match the cell's characteristic voltage and chemical behavior. Increased energy storage requires more voluminous chemicals at the same voltage.
A capacitor whose plates can store charge across a dielectric has no characteristic voltage.
A capacitor can be a power store but there's no electrochemistry required.
Semantically, you can not "recharge" a capacitor since there is no original charge to begin with. You must first charge it with an energy source, which a battery by definition contains but a capacitor does not. A capacitor stores energy but it is not an actual energy source.
When charging a simple solid-state capacitor the upper limit on charging voltage is based on the electrical resistance of the particular dielectric & its ability to withstand overvoltage. This is a physical limit. The electrodes are separated by a dielectric where having a high DC resistance is a desired property. A simple solid-state capacitor functions equally well for operation at reversed polarity.
For an electrolytic capacitor, it is polarized because the chemicals it contains provide an effective increase in storage per volume, at the disadvantage of having high DC resistance in only one direction. An additional limit in maximum voltage is imposed by the electrochemical nature of these type capacitors, but they are still rated as against a physical limit. Plus the polarity of the DC voltage being stored in them should always be respected, your peril is once again at stake.
But no capacitor has its own ideal voltage, they are not at all like batteries in this regard.
A battery's maximum charging voltage is usually limited to a range close to its nominal voltage, imposed by the natural scientific ability of the chemicals to withstand overvoltage while retaining composure. There is very little leeway to work with here. To change the working voltage of a battery storage bank requires addressing the granularity of a different number of matched cells in series, plus circuitry carefully re-optimized for the incremented working battery voltage.
A capacitor's maximum charging voltage is only limited to a range within its rated voltage,
which is an engineering value assigned based on the natural scientific ability of the dielectric to withstand overvoltage while retaining composure. The order(s) of magnitude more leeway should be easily recognized. To change the working voltage of a capacitor storage bank requires only addressing the dielectric strength, which would not need to be changed if it was over-specified to begin with.
The working voltage of capacitor storage can be any arbitrary voltage selected for various engineering reasons, the working voltage only needs to be selected below the electrical rating of the components. Increased energy storage requires more voluminous dielectric, whether more capacitors having the same voltage rating, or bigger packages handling higher chosen voltages.
One of the differences between electronics and electrochemistry, capacitors are nominally marked with a usually conservative rating, but some parts may often be capable of truly handling twice the rated voltage reliably. Batteries not so much.
As a natural scientist designing circuits primarily using natural intelligence through experimentation & discovery, key efforts in computer science seem to be 100% helpful when invested in calculations which are too heavy or numerous otherwise.
As a computer scientist designing circuits primarily using software simulation, when key efforts in physical prototype building fail, this might reveal the investment in computer science itself to be less than 100% helpful.
Don't get me started on electrochemistry . . . the potential for reaction could be unlimited ;-)
Thanks, from reading your comment, I can see that I was a bit loose with the term 'charging voltage' - I was focusing on the internal electrical potential of the cap or battery(stabilised), but 'charging voltage' should pinpoint the external potential which is applied to the component.
In programdudes circuit, the internal and external voltage of the cap are the same, because the cap has no internal resistance modelled. But really the resistive and inductive functions of current stores like caps and batts are what moderates current flow , into or out of from them, and therefore they are what determines suitable charging voltages.
The resistive function of a cap is much simpler than a battery, but the capacity of each to store and release current makes their voltage (the ~pressure of their current) persistent in the respect that internal voltage will only change by releasing or storing current. Well there are caveats of course that chemical and other reactions may alter the stores potential over time, but current exchange is the fundamental cause of potential, and purpose of electrical storage.
Id like to edit this line but to late now:
> its own voltage (the electrical potential created by virtue of its capacitance)
It would be better to write "electric potential sustained by virtue of its capacity".
For caps vs batteries, the only modelling difference I see between them is their resistance functions - that function in batteries tends to be very complex, approximated very roughly by charging curves. Caps tend to be much simpler, but can still involve significant internal resistance and inductance especially to maximum performance applications.
In summary what ive struggled to explain for the record is - the charging(external) voltage of a battery or cap, is only separated by its internal voltage by its internal resistance. A store which will charge moderately at +0.5v above its internal potential, is liable to blow very quickly if 10 or 100 times that voltage is applied.
Comments
I understand your conviction but sorry you will want to revise your outlook on this. Last attempt to explain - suppose you can charge a cap with a high voltage source, but stop charging when it reaches a lower voltage. The cap itself is never subjected to a high voltage in this situation (this is certain). It will receive current at the voltage it is at, and the power transferred to it will be the current * its voltage. No fast charging magic present.
You cannot charge a battery or capacitor (directly) at voltages higher than their own voltage.
If source voltage is suitable, resistive current limiting is plausible, but power is dissipated by resistance (within the cap and path to it) proportional to the square of the current. This is why efficient voltage transformation is required if source has a significantly higher potential.
Please see my comment here: https://news.ycombinator.com/item?id=13032719 to understand what I am trying to say.
ok I see it, but this statement is just fundamentally wrong here:
The cap in your circuit is not charging at any voltage, it is charging at Vn001 - its own voltage (the electrical potential created by virtue of its capacitance). In your circuit the only modelled resistance (and the drop in voltage between supply and the cap) is across R1.
This is all to explain the point which you disagreed with but is iron cast - you cant run power into a phone at 50volts to fast charge its 4volt battery without a missing, quite impossibly cool and small voltage transformer inside the phone to make the idea work.
Im not pointing this out to you to win an argument, Im explaining something which I didnt understand either when I began experimenting with ltspice and making charge circuitry. Take the advice or leave it now, but if you keep on with electronics you will find out sooner or later - "power stores charge and discharge > directly < at their own voltages" and if you dont have enough resistance between different electric potentials - take heed 'fun' will ensue of the dwarven kind ;)
To me the fundamentals have always been based on batteries being chemical reactions with their characteristic cell voltages. A cell definitely has its own discharge voltage, and can be used as a reference because the voltage remains relatively unchanged until the available chemicals are becoming effectively exhausted. It is an energy source based on the amount of chemicals available, plus a storage medium based on the reliable reversibility of the reaction.
In the case of rechargeable batteries, the desired reverse reaction can often be best obtained by carefully matching the recharge voltage & current dynamically, against the quantity of chemical you wish to react, including the amount undischarged and remaining to be reacted at any time. The recharge/maintenance voltages will need to be above the discharged/characterisitc voltages any time that cell recharging is expected to occur. The upper limit on charging voltage is based on the cell's characteristic voltage & the ability of the particular chemical system to withstand overvoltage. This is an electrochemical limit. The electrodes are separated by an electrolyte where having a low DC resistance is a desired property. As to the polarity of the DC voltage being provided or stored, this should always be respected, at your peril.
The working voltage of a battery cell can not be adjusted to match a particular circuit, the circuits must instead be closely designed to match the cell's characteristic voltage and chemical behavior. Increased energy storage requires more voluminous chemicals at the same voltage.
A capacitor whose plates can store charge across a dielectric has no characteristic voltage.
A capacitor can be a power store but there's no electrochemistry required.
Semantically, you can not "recharge" a capacitor since there is no original charge to begin with. You must first charge it with an energy source, which a battery by definition contains but a capacitor does not. A capacitor stores energy but it is not an actual energy source.
When charging a simple solid-state capacitor the upper limit on charging voltage is based on the electrical resistance of the particular dielectric & its ability to withstand overvoltage. This is a physical limit. The electrodes are separated by a dielectric where having a high DC resistance is a desired property. A simple solid-state capacitor functions equally well for operation at reversed polarity.
For an electrolytic capacitor, it is polarized because the chemicals it contains provide an effective increase in storage per volume, at the disadvantage of having high DC resistance in only one direction. An additional limit in maximum voltage is imposed by the electrochemical nature of these type capacitors, but they are still rated as against a physical limit. Plus the polarity of the DC voltage being stored in them should always be respected, your peril is once again at stake.
But no capacitor has its own ideal voltage, they are not at all like batteries in this regard.
A battery's maximum charging voltage is usually limited to a range close to its nominal voltage, imposed by the natural scientific ability of the chemicals to withstand overvoltage while retaining composure. There is very little leeway to work with here. To change the working voltage of a battery storage bank requires addressing the granularity of a different number of matched cells in series, plus circuitry carefully re-optimized for the incremented working battery voltage.
A capacitor's maximum charging voltage is only limited to a range within its rated voltage, which is an engineering value assigned based on the natural scientific ability of the dielectric to withstand overvoltage while retaining composure. The order(s) of magnitude more leeway should be easily recognized. To change the working voltage of a capacitor storage bank requires only addressing the dielectric strength, which would not need to be changed if it was over-specified to begin with.
The working voltage of capacitor storage can be any arbitrary voltage selected for various engineering reasons, the working voltage only needs to be selected below the electrical rating of the components. Increased energy storage requires more voluminous dielectric, whether more capacitors having the same voltage rating, or bigger packages handling higher chosen voltages.
One of the differences between electronics and electrochemistry, capacitors are nominally marked with a usually conservative rating, but some parts may often be capable of truly handling twice the rated voltage reliably. Batteries not so much.
As a natural scientist designing circuits primarily using natural intelligence through experimentation & discovery, key efforts in computer science seem to be 100% helpful when invested in calculations which are too heavy or numerous otherwise.
As a computer scientist designing circuits primarily using software simulation, when key efforts in physical prototype building fail, this might reveal the investment in computer science itself to be less than 100% helpful.
Don't get me started on electrochemistry . . . the potential for reaction could be unlimited ;-)
Thanks, from reading your comment, I can see that I was a bit loose with the term 'charging voltage' - I was focusing on the internal electrical potential of the cap or battery(stabilised), but 'charging voltage' should pinpoint the external potential which is applied to the component.
In programdudes circuit, the internal and external voltage of the cap are the same, because the cap has no internal resistance modelled. But really the resistive and inductive functions of current stores like caps and batts are what moderates current flow , into or out of from them, and therefore they are what determines suitable charging voltages.
The resistive function of a cap is much simpler than a battery, but the capacity of each to store and release current makes their voltage (the ~pressure of their current) persistent in the respect that internal voltage will only change by releasing or storing current. Well there are caveats of course that chemical and other reactions may alter the stores potential over time, but current exchange is the fundamental cause of potential, and purpose of electrical storage.
Id like to edit this line but to late now: > its own voltage (the electrical potential created by virtue of its capacitance)
It would be better to write "electric potential sustained by virtue of its capacity".
For caps vs batteries, the only modelling difference I see between them is their resistance functions - that function in batteries tends to be very complex, approximated very roughly by charging curves. Caps tend to be much simpler, but can still involve significant internal resistance and inductance especially to maximum performance applications.
In summary what ive struggled to explain for the record is - the charging(external) voltage of a battery or cap, is only separated by its internal voltage by its internal resistance. A store which will charge moderately at +0.5v above its internal potential, is liable to blow very quickly if 10 or 100 times that voltage is applied.