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Bipolar Junction and Field Effect Transistors (BJTs and FETs) is a short introductory video tutorial by Robert Keim, published June 7, 2020. It explains the terminals and basic operation of both transistor families, then connects them to switching and amplification. It is a useful starting point, not a complete design course: the guide below adds operating regions, practical switching and amplifier advice, and ways to simulate and measure a circuit.

What a transistor does

A transistor is a three-terminal semiconductor device that controls current in a circuit. Depending on its circuit and bias, it can act as an on/off switch, amplify a signal, buffer one stage from another, or regulate current. “A small input controls a larger output” is a helpful first picture, but it does not guarantee a particular voltage gain, current gain, or power gain. Those depend on the device, its bias point, circuit topology, load, frequency, and temperature.

The tutorial assumes familiarity with basic voltage, current, resistance, and diode behavior. If PN junctions are new, the related PN-junction and diode tutorial is a useful primer.

How a BJT works

A bipolar junction transistor has three semiconductor regions: emitter, base, and collector. The two junctions meet at the thin base. In an NPN device the regions are N-type, P-type, and N-type; in a PNP device their polarities are reversed. The emitter injects carriers, the base controls how many pass through, and the collector gathers them. In normal forward-active operation, the base is thin and lightly doped relative to the emitter, so most injected carriers cross it rather than recombining there.

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Conventional current direction is opposite to electron motion. In an NPN transistor operating as an amplifier, conventional collector current flows into the collector and out of the emitter; electrons move in the opposite direction. The base-emitter junction behaves approximately like a forward-biased diode, while the base-collector junction is reverse-biased in forward-active operation.

Useful first-order BJT relationships

In forward-active operation, a simple model is IC ≈ βIB, and emitter current is IE = IC + IB. Here β, also called hFE, is the current gain at a particular operating point. It varies with device, collector current, temperature, and voltage, so do not rely on a typical β as a fixed value when designing a switch.

A more physical first-order model is IC ≈ ISeVBE/VT. This exponential relationship explains why collector current is strongly affected by base-emitter voltage. For a silicon BJT at moderate current, VBE is often around 0.6–0.7 V, but it is not a constant: it changes with current and temperature. Calling a BJT “current-controlled” is useful circuit shorthand because base current is a convenient way to set collector current in many designs; it is not the whole device physics.

BJT operating regions

Region What it means Common use or caution
Cutoff The transistor is intended to be off; collector current is mainly leakage. Off state of a switch.
Forward-active Base-emitter is forward-biased and base-collector is reverse-biased. Linear amplification, if the signal remains within the region.
Saturation Both junctions are forward-biased. On state of a switch. It is not the normal linear-amplifier region.
Reverse-active Collector and emitter effectively exchange roles. Rarely useful; performance is generally poor compared with forward-active operation.
Breakdown A junction voltage exceeds its rated limit. May damage the device unless the device and circuit are designed for the relevant avalanche condition.

How a FET works

A field-effect transistor has a gate, source, and drain. The gate’s electric field changes the conductivity of a channel between source and drain. For insulated-gate MOSFETs, the gate is separated from the channel by an insulating layer, so steady-state gate current is very small in normal operation. That does not mean the gate never draws current: charging and discharging its capacitance requires transient current, leakage exists, and excessive gate-source voltage or electrostatic discharge can damage the oxide.

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JFETs and MOSFETs

“FET” is the family name, not a synonym for MOSFET. A JFET uses a PN-junction gate, normally reverse-biased in operation, to control its channel; JFETs are commonly depletion-mode devices. A MOSFET has an insulated gate and may be enhancement-mode or depletion-mode. Enhancement-mode MOSFETs are off at zero gate-to-source voltage and need the appropriate gate polarity to turn on; depletion-mode devices conduct at zero bias and can be driven toward cutoff.

MOSFETs are the most common FETs in modern switching applications, as the introductory tutorial notes. Small-signal and power MOSFETs are not interchangeable just because both have three terminals: power-device selection also requires attention to voltage, current, resistance, gate charge, thermal path, package, and body-diode behavior.

NPN, PNP, NMOS, and PMOS at a glance

Type Control convention Typical beginner application
NPN BJT Base current supports collector current; conventional current is typically directed into the collector and out of the emitter. Low-side switch or common-emitter amplifier.
PNP BJT Complementary polarity to an NPN; it is commonly controlled by pulling its base below its emitter. High-side switch or complementary amplifier stage.
Enhancement NMOS A sufficiently positive VGS increases channel conduction. Efficient low-side switch when the gate drive is adequate.
Enhancement PMOS A sufficiently negative VGS increases channel conduction. Convenient high-side switch at modest switching speeds and currents.

These are common conventions, not universal rankings. Whether NMOS or PMOS is better depends on circuit position, supply voltage, drive circuitry, current, losses, and switching speed.

BJT and FET differences that matter in practice

Consideration BJT FET, especially MOSFET
Control Base-emitter behavior and base current are central to circuit design. Gate-source voltage establishes an electric field; gate charge matters during transitions.
Input loading Base current loads the preceding stage. Very small steady-state gate current for an insulated gate, but not zero leakage or zero switching current.
Input impedance Generally lower. Generally higher.
Switching considerations Saturation can store charge and slow turn-off. Gate charge and capacitances set drive demands; device and circuit determine switching speed.
Analog and noise behavior Can offer high transconductance for a given bias current and can suit some low-source-impedance, low-noise circuits. Can suit high-source-impedance circuits; noise depends on device and source conditions.
Power design Requires a reliable base-current plan; thermal behavior and safe operating area matter. Conduction loss, gate drive, body diode, temperature, and safe operating area matter.

Neither family is categorically faster, lower-power, or higher-gain. “Gain” could mean current, voltage, transconductance, or power gain, and the comparison changes with the circuit and operating point.

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Using a transistor as a switch

NPN low-side switch

Place the load between the positive supply and the NPN collector, connect the emitter to the circuit’s common ground, and drive the base through a resistor. For an inductive load such as a relay, motor, or solenoid, place a flyback diode across the load, oriented so it is reverse-biased during normal operation. When the transistor turns off, the diode provides a path for the coil current and limits the voltage spike.

For a conservative saturated-switch design, choose a forced beta rather than relying on a typical datasheet hFE: IB ≥ IC/βforced. Then estimate the base resistor with RB ≈ (Vdrive − VBE)/IB. Check that the resulting base current is safe for both the transistor and the control output. The value of VBE is an estimate at the intended current, not an exact fixed drop.

NMOS low-side switch

Connect the source to common ground, the load between the positive supply and drain, and drive the gate relative to the source. Choose a MOSFET whose RDS(on) is specified at the actual gate voltage available from the controller. A part with a headline current rating may still be a poor choice if its low resistance is specified only at a higher gate drive than a 3.3 V GPIO can provide.

As a first estimate of conduction loss, use P ≈ ID2RDS(on). The actual resistance rises with temperature, and package, board, ambient temperature, switching losses, and safe operating area all affect the result. Check maximum VGS, drain voltage and current ratings, gate charge, thermal conditions, and inductive-load suppression. Never leave a MOSFET gate floating; use a suitable gate-source pull-down where needed and a gate resistor when appropriate.

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Using a transistor as an amplifier

An amplifier needs a stable DC bias point, or Q-point, in the intended operating region. The small AC signal then varies around that point. Too much signal swing pushes the device toward cutoff or saturation and clips or distorts the output. A load line helps visualize the voltage-current combinations allowed by the supply and load. Device variation and temperature can shift the Q-point, which is why bias networks need suitable stability rather than assumptions based on one typical gain value.

Common amplifier configurations

Device and configuration Typical role
BJT common emitter Voltage gain with phase inversion.
BJT common collector, or emitter follower Buffering and current gain, usually without voltage gain greater than one.
BJT common base Low input impedance and useful high-frequency behavior in suitable designs.
FET common source Voltage gain with phase inversion.
FET common drain, or source follower Buffering with high input impedance.
FET common gate Low input impedance and useful high-frequency behavior in suitable designs.

Voltage-divider bias is generally more robust for a BJT amplifier than setting its base from a single resistor and assuming a particular β. For a MOSFET amplifier, do not confuse threshold voltage with the gate voltage needed to establish the desired drain current or low on-resistance.

Choose a device from its datasheet

Confirm the exact part number and package before wiring anything: pin order is not universal, even among devices that look alike. Then check the ratings relevant to the circuit rather than choosing by a single headline number.

  • BJT: VCEO, collector current, power dissipation, hFE at the relevant current, VCE(sat), transition frequency for signal speed, safe operating area, and thermal resistance.
  • MOSFET: VDS, continuous and pulsed ID, RDS(on) at the intended VGS, total gate charge, capacitances, body-diode ratings, maximum junction temperature, avalanche rating, and safe operating area.
  • Any power device: Check how the current and power ratings depend on case temperature, pulse duration, mounting, and heat sinking. Staying below a current rating alone does not ensure safe operation.

VGS(th) is measured under specified test conditions and marks the onset of a small drain current; it is not a recommended drive voltage and does not guarantee low RDS(on). Also verify gate-source absolute maximum voltage, which can be far lower than the drain-source rating.

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Simulate, then measure

Start with LTspice

Analog Devices’ LTspice getting-started tutorial introduces the free simulator. Its LTspice basics video series covers installation, schematic creation, transient and AC simulation, waveform viewing, and model management. A useful sequence is to check a DC operating point first, run a transient simulation for switching or signal response, then sweep a parameter such as base current, VBE, VGS, or load.

  1. Plot a BJT common-emitter amplifier and observe its output as the input amplitude increases.
  2. Sweep BJT VBE and observe how collector current changes.
  3. Plot MOSFET drain current against VDS for several VGS values.
  4. Compare a generic model with a manufacturer model when one is available.
  5. Add an inductive load, compare behavior with and without a flyback diode, and inspect the switching transient.

Simulation depends on the model and does not capture every parasitic, temperature effect, layout issue, or measurement limitation. Treat it as a way to test and understand a circuit, not proof that a physical build will behave identically.

Build safely and take useful measurements

  • Begin with a current-limited supply and keep voltage, current, and power within the device ratings.
  • Check the exact datasheet pinout before placing a part on a breadboard.
  • Use a base resistor for a BJT and ensure the control output can supply the planned base current.
  • Do not leave a MOSFET gate floating; use an appropriate pull-down and avoid exceeding VGS limits.
  • Fit flyback protection across relay, motor, and solenoid coils.
  • Keep oscilloscope ground connections within a safe circuit reference arrangement; do not assume a grounded instrument input is isolated.

A multimeter is enough to check DC node voltages and continuity in a simple switch. For observing waveform shape, clipping, and switching transients, an oscilloscope and signal source are useful. Digilent describes the Analog Discovery 3 as a USB instrument with oscilloscope, waveform-generation, logic-analyzer, and programmable-supply functions; its official product page lists up to 125 MS/s and 30+ MHz oscilloscope bandwidth with the BNC adapter. Its programmable supplies are low-voltage educational supplies, not a universal bench source. An optional Student Bundle adds a parts kit, while the Analog Discovery Studio is positioned as a larger portable circuits lab. Product prices and availability vary by region and can change, so check the vendor pages directly.

Troubleshoot common transistor problems

The load is always on or never turns on

  • Confirm pinout, transistor type, supply polarity, common ground, and load wiring.
  • For an NPN low-side switch, check that base voltage is sufficiently above emitter voltage and that base current is limited but adequate.
  • For a MOSFET, measure VGS at the device rather than only at the controller output; verify the part is specified for that drive voltage.
  • Check that a gate is not floating and that a PNP or PMOS device is being driven with the correct polarity relative to its emitter or source.

The transistor gets hot

  • Measure voltage across the conducting device and current through it to estimate dissipation.
  • For a BJT switch, insufficient base drive can leave it outside saturation and increase VCE.
  • For a MOSFET, inadequate gate drive can leave RDS(on) high; switching slowly can also add loss.
  • Recheck thermal resistance, package limits, pulse conditions, and safe operating area rather than relying on the maximum current line alone.

The amplifier clips or differs from simulation

  • Check the DC Q-point before applying a signal; it may already be near cutoff or saturation.
  • Reduce input amplitude and check whether the output remains within the supply and load-line limits.
  • Verify component values, transistor orientation, model choice, supply voltage, and probe grounding.
  • Allow for device variation, temperature, breadboard parasitics, and simulator-model limits.

If a device fails immediately, disconnect power and verify wiring, polarity, pinout, current limiting, and maximum terminal voltages before replacing it. Repeating a test without finding the fault can destroy another part.

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Quick Recap

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