Click here to go to the applet. 
This java applet is an electronic circuit simulator.  When the applet starts up you will see
a simple LRC circuit.  The green
color indicates positive voltage. 
The gray color indicates ground. 
A red color indicates negative voltage.  The moving yellow dots indicate current.
To turn a switch on or off, just click on it.  If you move the mouse over any component of the circuit, you
will see a short description of that component and its current state in the
lower right corner of the window. 
To modify a component (say, to change the resistance of one of the
resistors), move the mouse over it, click the right mouse button (or
control-click, if you have a Mac) and select “Edit”.
There are three graphs at the bottom of the window; these act like
oscilloscopes, each one showing the voltage and current across a particular
component.  Voltage is shown in
green, and current is shown in yellow. 
The current may not be visible if the voltage graph is on top of
it.  The peak value of the voltage
in the scope window is also shown. 
Move the mouse over one of the scope views, and the component it is
graphing will be highlighted.  To
modify or remove a scope, click the right mouse button over it.  To view a component in the scope, click
the right mouse button over the component and select “View in Scope”.
If the simulation is moving too slowly or too quickly, you can adjust the
speed with the “Simulation Speed” slider.
The Circuits menu can be used to
view some interesting pre-defined circuits. Once a circuit is selected, you may
modify it all you want. The choices are: 
 - Basics
  - Resistors: this shows some resistors of various sizes
      in series and parallel.
- Capacitor: this shows a capacitor that you can charge
      and discharge by clicking on the switch.
- Inductor: this shows an inductor that you can charge
      and discharge by clicking on the switch.
- LRC
      Circuit: this shows an
      oscillating circuit with an inductor, resistor, and capacitor.  You can close the switch to get
      current moving in the inductor, and then open the switch to see the
      oscillation.
- Voltage
      Divider: this shows a voltage
      divider, which generates a reference voltage of 7.5V, 5V, and 2.5V from
      the 10V power supply.
- Thevenin’s
      Theorem states that the circuit
      on top is equivalent to the circuit on the bottom.
- Norton’s
      Theorem states that the circuit
      on top is equivalent to the circuit on the bottom.
- A/C Circuits
  - Capacitor: this shows a capacitor connected to an
      alternating voltage source.
- Inductor
- Caps of Various
      Capacitances: shows the response of
      three different capacitors to the same frequency.
- Caps w/ Various
      Frequencies: shows the response of
      three equal capacitors to three different frequencies; the higher the
      frequency, the larger the current.
- Inductors of
      Various Inductances: shows the
      response of three different inductors to the same frequency.
- Inductors w/
      Various Frequencies: shows the
      response of three equal inductors to three different frequencies: the
      lower the frequency, the larger the current.
- Impedances of Same
      Magnitude: shows a capacitor, an
      inductor, and a resistor that have impedances of equal magnitude (but
      different phase).  The peak
      current is the same in all three cases.
- Series
      Resonance: shows three identical
      LRC circuits being driven by three different frequencies.  The middle one is being driven at
      the resonance frequency (shown in the lower right corner of the screen as
      “res.f”).  The top one is
      being driven at a slightly lower frequency, and the bottom one has a
      slightly higher frequency. 
      The peak voltage in the middle circuit is very high because it is
      resonating with the source.
- Parallel
      Resonance: these three circuits
      have the inductor, resistor, and capacitor in parallel instead of
      series.  In this case, the
      middle circuit is being driven at resonance, which causes the current
      there to be lower than in the other two cases (because the impedance of
      the circuit is highest at resonance).
- Passive Filters
  - High-Pass
      Filter (RC).  The original signal is shown at the lower left, and the filtered
      signal (with the low-frequency part removed) is shown to the right.  The breakpoint (-3 dB point) is
      shown at the lower right, as “f.3db”.
- Low-Pass
      Filter (RC).
- High-Pass Filter (RL). 
      This high-pass filter uses an inductor rather than a capacitor.
- Low-Pass Filter
      (RL). 
- Band-Pass Filter: this filter passes a range of frequencies
      close to the resonance frequency (shown at the lower right, as “res.f”).
- Notch Filter: Also known as a band-stop filter, this
      circuit filters out a range of frequencies close to the resonance
      frequency.
- Twin-T Filter: This filter does a very good job of
      filtering out 60 Hz signals.
- Crossover:  A
      set of three filters; the top one passes low frequencies, the middle one
      passes midrange, and the bottom one passes high frequencies.
- Other Passive Circuits
  - Series/Parallel
   - Inductors in
       Series.  The circuit at left is equivalent to the circuit at
       right.
- Inductors in
       Parallel.
- Caps in Series.
- Caps in Parallel.
- Transformers
   - Transformer:
       A basic transformer circuit with an
       equal number of windings in each coil.
- Transformer w/ DC:
       Here we try to pass a DC current
       through a transformer.
- Step-Up
       Transformer: Here we step 10 V up
       to 100 V.
- Step-Down
       Transformer: Here we step 120 V
       down to 12 V.
- 3-Way Light
      Switches: shows how a light bulb can
      be turned on and off from two locations.
- 3- and 4-Way Light
      Switches: shows how a light bulb can
      be turned on and off from three locations.
- Differentiator: shows how a capacitor can act as a
      differentiator, reflecting changes in voltage.
- Wheatstone Bridge: shows a balanced Wheatstone bridge.  If the bridge were not balanced,
      current would be flowing across from one leg to the other.
- Critically Damped LRC.
- Current Source: shows a source that keeps the current
      through the circuit constant regardless of the switch positions.
- Inductive Kickback: In this circuit, we have a switch that
      controls the supply of current to an inductor.  An inductor resists any changes in current.  If you open the switch, the
      inductor tries to maintain the same current; it does this by charging the
      capacitance between the contacts of the switch.  (Any two wires in close proximity have some parasitic
      capacitance between them.) 
      There is a small capacitor (much larger than the actual value)
      across the switch terminals to simulate this.  When you open the switch, the voltage goes very high;
      in real life, this would cause arcing.
- Blocking Inductive
      Kickback: shows how inductive
      kickback can be blocked with a “snubber” circuit.
 
 
- Power
      Factor: This circuit shows an
      inductor being driven by an AC voltage.  The colors indicate power consumption; red means that
      a component is consuming power, and green means that the component is
      contributing power.  The left
      side of the circuit represents the power company’s side, and the right side
      represents a factory (with a large induction motor).
 
 The highly inductive load is causing the power company to work a lot
      harder than normal for a given amount of power delivered.  The graph on the left indicates the power lost in the power
      company’s equipment (the resistor at top left).  The graph in the middle is the power delivered to the
      factory.  The graph on the
      right is the power delivered to the inductor (and then returned, causing
      the time average of power delivered to be zero).
 
 Even though a peak power of 40 mW is being delivered to the factory, 200
      mW is being dissipated in the power company’s wires.  This is why power companies
      charge extra for inductive loads.
 
 
- Power
      Factor Correction: Here a
      capacitor has been added to the circuit, causing far less energy to be
      wasted in the power company’s wires (aside from an initial spike to
      charge the capacitor).
- Resistor Grid: shows current flowing in a two-dimensional
      grid of resistors.
- Resistor Grid 2.
- Coupled LC's
o     
LC Modes(2):
Shows both modes of two coupled LC circuits.
o     
Weak Coupling. 
o     
LC Modes(3):
Shows all 3 modes of 3 coupled LC circuits.
o     
LC Ladder: This
circuit is a simple model of a transmission line.  A pulse propagates down the length of the ladder like a
wave.  The resistor at the end has
a value equal to the characteristic impedance of the ladder (determined by the
ratio of L to C), which causes the wave to be absorbed.  A larger resistance or an open circuit
will cause the wave to be reflected; a smaller resistance or a short will cause
the wave to be reflected negatively.  See the Feynman
Lectures 22-6, 7.
 
  - Phase-Sequence
      Network: This circuit generates a
      series of sine waves with a phase difference of 90°.
- Lissajous Figures:
      Just for fun.
- Diodes
  - Half-Wave Rectifier: This circuit removes the negative part of an
      input waveform.
- Full-Wave Rectifier: This circuit replaces a waveform with its
      absolute value.
- Full-Wave Rectifier
      w/ Filter: This circuit smoothes out
      the rectified waveform, doing a pretty good job of converting AC to DC.
- Diode I/V Curve: This demonstrates the response of a diode to
      an applied voltage.  The
      voltage source generates a sawtooth wave, which starts out at –800 mV and
      slowly rises to 800 mV, and then immediately drops back down again.
- Diode Limiter.
- DC Restoration. 
      This takes an AC signal and adds a DC offset, making it a positive
      signal.
- Blocking Inductive
      Kickback: shows how inductive
      kickback can be blocked with a diode.
- Spike Generator.
- Voltage Multipliers
   - Voltage Doubler: Doubles the voltage in the AC input signal
       (minus two diode drops), and turns it into DC.
- Voltage Doubler 2
- Voltage Tripler
- Voltage Quadrupler
- AM
      Detector: This is a “crystal
      radio”, an AM radio receiver with no amplifier.  The raw antenna feed is shown in the first scope slot
      in the lower left.  The
      inductor and the capacitor C1 are tuned to 3 kHz, the frequency shown in
      the lower right as “res.f”. 
      This picks up the carrier wave shown in the middle scope
      slot.  A diode is used to
      rectify this, and the C2 capacitor smoothes it out to generate the audio
      signal in the last scope slot (which is simply a 12 Hz sine wave in this
      example).  By experimenting
      with the value of C1’s capacitance, you can pick up two other “stations”
      at 2.71 kHz and 2.43 kHz.
- Triangle-to-Sine
      Converter
- Transistors
  - Switch.
- Emitter
      Follower.
- Astable
      Multivibrator: A simple
      oscillator.  The applet has
      trouble simulating this circuit, so there might be a slight delay every
      time one of the transistors switches on.
- Bistable
      Multivibrator (Flip Flop): This
      circuit has two states; use the set/reset switches to toggle between
      them.
- Monostable
      Multivibrator (One-Shot): When
      you hit the switch, the output will go to 1.7 V for a short time, and
      then drop back down.
- Common-Emitter
      Amplifier: This circuit amplifies
      the voltage of the input signal by about 10 times.
- Unity-Gain Phase
      Splitter: Outputs two signals 180°
      out of phase from each other.
- Schmitt
      Trigger.
- Current Source: The current is the same regardless of the
      switch position.
- Current Source
      Ramp: Uses a current source to
      generate a ramp waveform every time you hit the switch.
- Current Mirror: The current on the right is the same as the
      current on the left, regardless of the position of the right switch.
- Differential
      Amplifiers
   - Differential Input:
       This circuit subtracts the first
       signal from the second and amplifies it.
- Common-Mode Input: This shows a differential amplifier with two
       equal inputs.  The output
       should be a constant value, but instead the input waveforms make it
       through to the output (attenuated rather than amplified).  (When both inputs change
       together, that is called “common-mode input”; the “common-mode rejection
       ratio” is the ability of a differential amplifier to ignore common-mode
       signals and amplify only the difference between the inputs.)
- Common-Mode
       w/Current Source: This is an
       improved differential amplifier that uses a current source as a
       load.  The common-mode
       rejection ratio is very good; the circuit amplifies the small
       differences between the two inputs, and ignores the common-mode signal.
- Push-Pull Follower:
      This is another type of emitter
      follower.
- Oscillators
   - Colpitts
       Oscillator
- Hartley Oscillator
- Emitter-Coupled LC
       Oscillator
- JFETs
  - JFET Current Source
- JFET Follower: This is like an emitter follower, except that
      the output is 3V more positive than the input.
- JFET Follower
      w/zero offset
- Common-Source
      Amplifier
- Volume Control: Here the JFET is used like a variable
      resistor.
- MOSFETs
  - CMOS
      Inverter: The white “H” is a
      logic input.  Click on it to
      toggle its state.  “H” means
      “high” (5 V) and “L” means “low” (0 V).  The output of the inverter is shown at right, and is
      the opposite of the input. 
      In this (idealized) simulation, the CMOS inverter draws no current
      at all.
- CMOS Inverter
      (w/capacitance): In reality, there
      are two reasons that CMOS gates draw current.  This circuit demonstrates the first reason:
      capacitance between the MOSFET gate and its source and drain.  It requires current to charge
      this capacitance, which consumes power.  It also causes a short delay when changing state.
- CMOS Inverter (slow
      transition): The other reason that
      CMOS gates draw current is that both transistors will conduct at the same
      time when the input is halfway between high and low.  This causes a current spike when
      the input is in transition. 
      In this circuit, there is a low-pass filter on the input which
      causes it to transition slowly, so you can see the spike.
- CMOS Transmission
      Gate: This circuit will pass any
      signal, even an analog signal (as long as it stays between 0 and 5 V)
      when the gate input is “H”. 
      When it’s “L”, then the gate acts as an open circuit.
- CMOS Multiplexer: This circuit uses two transmission gates to
      select one of two inputs.  If
      the logic input is “H”, then the output is a 40Hz triangle wave.  If it’s “L”, then the output is a
      80Hz sine wave.
- Sample-and-Hold: Click and hold the “sample” button to sample
      the input.  When you release
      the button, the output level will be held constant.
- Delayed Buffer: This circuit delays any changes in its input
      for 15 microseconds.
- Leading-Edge
      Detector
- Switchable Filter: Click the “L” to select from two different
      low-pass filters.
- Voltage Inverter
- Inverter Amplifier:
      This shows how a CMOS inverter can
      be used as an amplifier.
- Inverter Oscillator
- Op-Amps
  - Amplifiers
   - Inverting
       Amplifier: This one has a gain
       of –3.
- Non-Inverting
       Amplifier
- Follower
- Differential
       Amplifier
- Summing
       Amplifier
- Log Amplifier: output is the (inverted) log of the input
- Class D
       Amplifier
- Oscillators
   - Relaxation
       Oscillator
- Phase-Shift
       Oscillator
- Triangle
       Wave Generator
- Sine
       Wave Generator
- Sawtooth Wave
       Generator
- Voltage-Controlled
       Oscillator: Here the frequency of
       oscillation depends on the input (shown in the scope on the left).  The oscillator outputs a square
       wave and a triangle wave.
- Rossler Circuit
- Half-Wave Rectifier: An active rectifier that works on voltages
      smaller than a diode drop.
- Full-Wave Rectifier
- Peak Detector: This circuit outputs the peak voltage of the
      input.  Whenever the input
      voltage is higher than the output, the output will be adjusted upward to
      match.  Press the switch
      marked “reset” to reset the peak voltage back to 0.
- Integrator
- Differentiator
- Schmitt
      Trigger
- Negative Impedance
      Converter: Converts the resistor to
      a “negative” resistor.  In
      the first graph, note that the current is 180° out of phase with the
      voltage.
- Gyrator: The top circuit simulates the bottom circuit
      without using an inductor.
- Capacitance
      Multiplier: This circuit allows you
      to simulate a large capacitor with a smaller one.  The effective capacitance of the
      top circuit is C1 x (R1/R2), and the effective resistance is R2.
- Howland Current
      Source
- I-to-V Converter: The output voltage depends on the input
      current, which you can adjust with the switches.
- 741
      Internals: The implementation of
      a 741 op-amp.
- 555 Timer Chip
  - Square Wave
      Generator
- Internals: The implementation of a 555 chip, acting as a
      square wave oscillator
- Sawtooth Oscillator
- Low-duty-cycle
      Oscillator: produces short pulses.
- Monostable
      Multivibrator: This is a one-shot
      circuit that will produce a timed pulse when you click the “H”.
- Pulse Position
      Modulator: Produces pulses whose
      width is proportional to the input voltage.
- Schmitt Trigger
- Missing Pulse
      Detector: Setting the logic input
      low will turn off the square wave input.  The missing pulse detector will detect the missing
      input and bring the output high.
- Active Filters
  - VCVS Low-Pass Filter: An active Butterworth low-pass filter.
- VCVS High-Pass
      Filter
- Switched-Capacitor
      Filter: A digital filter,
      implemented using capacitors and analog switches.
- Logic Families
  - RTL Logic Family
   - RTL
       Inverter: The white “H” is a
       logic input.  Click on it to
       toggle its state.  “H” means
       “high” (3.6 V) and “L” means “low” (0 V).  The output of the inverter is shown at right, and is
       the opposite of the input.
- RTL
       NOR: The three inputs are at
       the bottom, and the output is to the right.  The output is “L” if any of the inputs are “H”.  Otherwise it’s “H”.
- RTL NAND: The output is “H” unless all three inputs
       are “H”, and then it’s “L”.
- DTL Logic Family
   - DTL
       Inverter
- DTL
       NAND
- DTL
       NOR
- TTL Logic Family
   - TTL
       Inverter
- TTL NAND
- TTL
       NOR
- NMOS Logic Family
   - NMOS Inverter
- NMOS Inverter 2: This uses a second MOSFET instead of a
       resistor, to save space on a chip.
- NMOS NAND
- CMOS
      Logic Family
   - CMOS Inverter
- CMOS NAND
- CMOS NOR
- CMOS XOR
- CMOS
       Flip-Flop (or latch): This
       circuit consists of two CMOS NAND gates.
- CMOS
       Master-Slave Flip-Flop
- ECL
      Logic Family
   - ECL NOR/OR
- Ternary: This demonstrates three-valued logic, where
      the inputs can be 0, 1, or 2 instead of H and L.  This logic is implemented using
      MOSFETs; the threshold
      voltage of each one is shown.
   - CGAND: the output is 2-X where X is the minimum of
       the two inputs.
- CGOR: the output is 2-X where X is the maximum of
       the two inputs.
- Complement.
- F211: 0 becomes 2, 1 becomes 1, 2 becomes 1.
- F220
- F221
- Combinational Logic
  - Exclusive OR
      (XOR) 
- Half Adder
- Full Adder
- 1-of-4 Decoder
- 2-to-1
      Mux: This multiplexer uses two
      tri-state buffers connected to the output.
- Majority Logic: The output is high if a majority of the inputs
      are high.
- 2-Bit Comparator: Tells you if the two-bit input A is greater
      than, less than, or equal to the two-bit input B.
- 7-Segment LED
      Decoder
- Sequential Logic
- Analog/Digital
  - Flash
      ADC: This is a
      direct-conversion, or “flash” analog-to-digital converter.
- Delta-Sigma
      ADC
- Half-Flash
      (Subranging) ADC: Also known as
      a pipeline ADC.  The first
      stage converts the input voltage to a four-bit digital value.  Then, a DAC converts these four
      bits to analog, and then a comparator calculates the difference between
      this and the input voltage. 
      Another ADC converts this to digital, giving a total of eight
      bits. 
- Binary-Weighted
      DAC:  Converts a four-bit binary number to a negative
      voltage.
- R-2R
      Ladder DAC
- Switch Tree DAC
- Digital Sine Wave
- Phase-Locked Loops
  - XOR Phase Detector: Shows an XOR gate being used as a type I
      phase detector.  The output
      is high whenever the two input signals are not in phase.
- Type I PLL: This phase-locked loop circuit consists of an
      XOR gate (the phase detector), a low-pass filter (the resistor and
      capacitor), a follower (the op-amp), and a voltage-controlled oscillator
      chip.  The voltage-controlled
      oscillator outputs a frequency proportional to the input voltage.  After the PLL circuit locks onto
      the input frequency, the output frequency will be the same as the input
      frequency (with a small phase delay).
- Phase Comparator
      (Type II): Shows a more
      sophisticated phase detector, which has no output when the inputs are in
      phase, but outputs high (5V) when input 1 is leading input 2, and low
      (0V) when input 2 is leading input 1.  The phase comparator and VCO in this applet are based
      on the 4046
      chip.
- Phase Comparator
      Internals.
- Type II PLL: Shows a phase-locked loop with a type II phase
      detector.  If you adjust the
      input frequency, the output should lock onto it in a short time.
- Type II PLL (fast): Just a faster simulation of the type II PLL.
- Frequency Doubler
- Transmission Lines
  - Simple TL: A properly terminated transmission line,
      showing the delay as the signal travels down the line.
- Standing Wave: A standing wave on a shorted transmission
      line.
- Termination: The top line is terminated properly, but the
      others are not, and so the incoming wave is reflected.
- Mismatched lines: Shows reflections caused by the middle line
      having a different impedance than the other two lines.
- Mismatched lines 2:
      Shows a standing wave on the first
      line, caused by the second line having a different impedance.
To
add a new component to the circuit, click the right mouse button on an unused
area of the window.  This will
bring up a menu that allows you to select what component you want.  Then click where you want the first
terminal of the component, and drag to where you want the other terminal.  The menu items allow you to create:
·     
wires
·     
resistors; you can adjust the resistance after creating
the resistor by clicking the right mouse button and selecting “Edit”
·     
capacitors; you can adjust the capacitance using “Edit”
·     
inductors, switches, transistors, etc.
·     
voltage sources, in either 1-terminal or 2-terminal
varieties.  The 1-terminal versions
use ground as the other terminal. 
By clicking the right mouse button and selecting “Edit”, you can modify
the voltage and the waveform of the voltage source, changing it to DC, AC (sine
wave), square wave, triangle, sawtooth, or pulse.  If it’s not a DC source, you can also change the frequency
and the DC offset.
·     
op-amps, with power supply limits of –15V and 15V
assumed (not shown).  The limits
can be adjusted using “Edit”.
·     
text labels, which you can modify with the “Edit”
dialog
·     
scope probes; these have no effect on the circuit, but
if you select them and use the right mouse menu item “View in Scope”, you can
view the voltage difference between the terminals.
Also
in the “Other” submenu, there are some items that allow you to click and drag
sections of the circuit around. 
Save your work before trying these.
The
File menu allows you to import or
export circuit description files. 
Java security restrictions usually prevent an applet from writing files
to a user’s computer.  So instead,
when you select the File->Export
menu item, the applet brings up a window containing the description file for
the circuit, which you can copy and paste into another application.  You can paste the file back into the
window later and click Import to
load it.
The
Reset button resets the circuit to a
reasonable state.  The Stopped
checkbox allows you to stop the
simulation.  The Simulation
Speed slider allows you to adjust the
speed of the simulation.  If the
simulation isn’t time-dependent (that is, if there are no capacitors,
inductors, or time-dependent voltage sources), then this won’t have any effect.  The Current Speed slider lets you adjust the speed of the dots, in
case the currents are so weak (or strong) that the dots are moving too slowly
(or too quickly).
To
edit one of the scope views, click the right mouse button on it to view a
menu.  The menu items allow you to
remove a scope view, speed up or slow down the display, adjust the scale,
select what value(s) you want to view, etc.
Here
are some errors you might encounter when using the simulator:
·     
Voltage source loop with no resistance! – this means one of the voltage sources in your
circuit is shorted.  Make sure
there is some resistance across every voltage source.
·     
Capacitor loop with no resistance! – it’s not allowed to have any current loops
containing capacitors but no resistance. 
For example, capacitors connected in parallel are not allowed; you must
put a resistor in series with them. 
Shorted capacitors are allowed.
·     
Singular matrix!
– this means that your circuit is inconsistent (two different voltage sources
connected to each other), or that the voltage at some point is undefined.  It might mean that some component’s
terminals are unconnected; for example, if you create an op-amp but haven’t
connected anything to it yet, you will get this error.  
·     
Convergence failed! – this means the simulator can’t figure out what the state of the
circuit should be.  Just click Reset and hopefully that should fix it.  Your circuit might be too complicated,
but this happens sometimes even with the examples.
·     
Transmission line delay too large! – the transmission line delay is too large compared
to the timestep of the simulator, so too much memory would be required.  Make the delay smaller.
·     
Need to ground transmission line! – the bottom two wires of a transmission line must
always be grounded in this simulator.
Click here to go to the applet. 
 
 java@falstad.com
java@falstad.com