Cockroft Walton Voltage Multipliers. The classic multistage diode/capacitor voltage multipler, popularized by Cockroft and Walton, is probably the most popular. Abstract—This paper primarily describes a Cockcroft Walton voltage multiplier circuit. The objective of the project is to design a voltage multiplier which should. For now I’ll thoroughly explain principle part and its assumptions. First assume that voltage doubler and cw multlipier is not loaded. Voltage doubler circuit: Let at .

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The biggest advantage coltage such circuits is that the voltage across each stage of the cascade is equal to only twice the peak input voltage in a half-wave rectifier. In a full-wave rectifier it is three times the input voltage. As the number of stages is increased, the voltages of the higher stages begin to “sag”, primarily due to the electrical impedance of the capacitors in the lower stages. Please help improve this article by adding citations to reliable sources.

CW multipliers are also found, with a higher number of stages, in laser systems, high-voltage power supplies, X-ray systems, LCD backlightingtraveling-wave tube amplifiers, ion pumpselectrostatic systems, air ionisersparticle acceleratorscopy machinesscientific waltoj, oscilloscopestelevision sets and cathode ray tubes vkltage, electroshock weaponsbug zappers and many other applications that use high-voltage DC.

All the capacitors are charged to a voltage of 2 V pexcept for C1which is charged to V p. For substantial loads, the charge on the capacitors is partially depleted, and the output voltage drops according to the output current divided by the capacitance. It has the advantage of requiring relatively low-cost components and being easy to insulate. In this case, the ripple is: For these reasons, CW multipliers with large number of stages are used only where relatively low output current is required.

CW multipliers are typically used to develop higher voltages for relatively low-current applications, such as bias voltages ranging from tens or hundreds of volts to millions of volts for high-energy physics experiments or lightning safety testing. This is particularly useful when the charging stack capacitors are significantly smaller than the output filter capacitors.

It has the advantage of requiring relatively low cost components and multip,ier easy to insulate. By driving the CW from a high-frequency source, such as an inverteror a combination of an inverter and HV transformer, the overall physical size and weight of the CW power supply can be substantially reduced.


Taken from the High Power Microwave Transmitters report by North, here is a three phase multiplier circuit. Unlike the Cockcroft-Walton multiplier generatorthe Marx generator need air for the spark gaps and can not multiplie immersed in oil as an insulator.

Cockroft Walton Voltage Multipliers

Iload is the load current C is the stage capacitance f is the AC frequency n is the number of stages. From Wikipedia, the free encyclopedia. It is used in virtually every television set made to generate the kV second anode accelerating voltage from a transformer putting out kV pulses. By using this site, you agree to the Terms of Use and Privacy Policy.

Cockcroft–Walton generator – Wikipedia

It also inherently produces a series of stepped voltages which is useful in some forms of particle accelerators, and for biasing photomultipler tube voltwge. The CW multiplier has the disadvantage of having very poor voltage regulation, that is, the voltage drops rapidly as a function the output current. This article needs additional citations for verification. One way to look at the circuit is that it functions as a charge “pump”, pumping electric charge in one direction, up the stack of capacitors.

Articles needing additional references from March All articles needing additional references Commons category voltagw is on Wikidata.

The key to the voltage multiplication is that while the capacitors are charged in parallel, they are connected to the load in series. Furthermore, the ripple on the output, particularly at high loads, is quite high. They also are used in everyday electronic devices that require high voltages, such as X-ray machinestelevision setsmicrowave ovens and photocopiers. The high ripple means that there is a signficant energy spread in the ion beam, though, and for applications where low ripple is important at megavolt potentials, electrostatic systems like Van de Graaf and Pelletron machines are preferred.

This page was last edited on 18 Decemberat Note the three human figures at top center for scale. The circuit was discovered inby Heinrich Greinachera Swiss physicist. To understand the fockroft operation, see the diagram of the two-stage version at right. March Learn how and when to remove this template message.


The sag can be reduced by increasing the capacitance in the lower stages, and the ripple can by reduced by increasing the frequency of the input and by using a square waveform.

It is made up of a voltage multiplier ladder network of capacitors and diodes to generate high voltages. And, when supplying an output current, the voltage ripple rapidly increases as the number of stages is increased this can be corrected with an output filter, but it requires a stack of capacitors in order to withstand the high voltages involved.

A modification to the classic CW multiplier, popularized by XXX, uses two charging stacks driven by out of phase input voltages.

The number of stages is equal to the number of capacitors in series between the output and ground. Increasing the frequency can dramatically reduce the ripple, and the voltage drop under load, which accounts for the popularity driving a multipler stack with a switching power supply.

Cockcroft–Walton generator

The CW circuit, along with other similar capacitor circuits, is often called charge pump. In some applications, an addtional capacitor stack is connected to the output capacitor stack in the above design. This circuit can be extended to any number of stages.

It is quite popular for relatively low powered particle accelerators for injecting into another accelerator, particularly for heavy ions. One can also tap the output from any stage, like in a multitapped transformer.

The no-load output voltage is twice the peak input voltage multiplied by the number of stages N or equivalently the peak-to-peak input voltage swing V pp times the number of stages. It was named after the British and Irish physicists John Douglas Cockcroft and Ernest Thomas Sinton Waltonwho in used this circuit design to power their particle acceleratorperforming the first artificial nuclear disintegration in history.

Retrieved from ” https: An Introduction to Mechanics 2nd ed.