Let's begin with a query: How well do you grasp the movement of current and electrons within a circuit?
Figure 1: Insight
The electric field, as demonstrated in Figure 1, travels from the battery's positive to negative electrode. Conversely, electrons journey opposite to the field, starting at the negative electrode and moving toward the positive.
MOSFETs originate from semiconductor materials like silicon, which bridges the gap between conductive and insulative properties. Crafting a proficient conductor involves introducing impurities into pure crystals. Pentavalent impurities transform semiconductors into n-type, dominated by electron carriers. Conversely, trivalent impurities yield a p-type semiconductor, where holes reign as majority charge carriers.
Figure 2: Explained
In Figure 2, connecting n-type and p-type semiconductors results in electrons filling p-type holes at the junction, forming a depletion zone. Connecting the p-type to the battery’s positive terminal and the n-type to the negative minimizes this zone in a forward bias. Reversing polarity intensifies the depletion zone, thus creating reverse bias.
MOSFETs are categorized into two principal types: enhancement and depletion, further split into N-channel and P-channel.
An N-channel MOSFET, particularly the enhancement-mode, is our focus. Its operating principle begins here.
Figure 3: MOSFET Structure
In Figure 3, observe the MOSFET's composition: a yellow-hued n-type, a blue p-type semiconductor, and their connections. The starting point is the blue substrate terminal. From the yellow side, terminals diverge into source and drain. These components are interspersed by a thin insulative layer, topped by the gate terminal, as shown further in Figure 4.
Figure 4: MOSFET Structure
Notably, due to symmetrical nature, MOSFETs allow source-drain interchangeability. With the source tied internally to the substrate, our observation reduces to three terminals at a uniform potential, blocking substrate-source current.
For optimal current flow from drain to source in a MOSFET, a battery connects these terminals, defining Vds.
Figure 5: Dynamic Relationship Between Drain Current and Vds
The battery’s positive end elevates drain terminal voltage, widening the depletion between drain and substrate, inhibiting current flow — the off state or Cutoff region.
Constructing a channel, crucial for drain-source current flow, involves a small voltage source between gate and substrate, forthcoming in Figure 6.
Figure 6: Establishing a Channel
By securing the gate to the battery’s positive end, termed Vgs, a field forms. P-type substrate holes predominate, with sparse free electrons present. This electric field prompts electrons toward the gate grid, restrained by insulator presence, accumulating nearby.
Comparatively to capacitors' electrical charge storage capability, a MOSFET's insulator enhances charge presence, drawing more electrons.
Figure 7: Analysis
Figure 7 reveals a hole-void red box area filled with electrons, converting the region into an n-type semiconductor. Connecting source and drain forms a channel, allowing electron transit. Adjustments in gate voltage modify channel width, influencing threshold voltage and channel thickness.
Figure 8: Contribution
Post-channel creation, Figure 8 portrays current proceeding from drain to source, driven by source-fed electrons collected by the drain. This directional flow underpins naming conventions: source and drain.
In the ohmic region, MOSFETs comply with Ohm's law, aligning current growth with voltage increase. Yet, heightened voltage extends the depletion zone, especially where channel electrons drain towards positive potential. This current reduction culminates in the pinch-off effect, but in practice, electron volume stabilizes flow, maintaining a saturation current without cease – hence introducing the saturation zone.
MOSFETs are dubbed voltage-controlled devices given gate voltage’s role in managing current flow. The gate remains current-free.
Figure 9: Characteristics
In Figure 9, the left side outlines drain characteristics against the transfer characteristic at constant Vds on the right.
Depletion-mode MOSFETs, while akin to enhancement, inherently possess a channel post-doping. Their operation echoes enhancement types, albeit different in higher default consumption. Unlike the closed enhancement type, they are open by default and close under negative gate voltage.
Figure 10: Circuit Symbol
Figure 10 showcases traditional MOSFET symbols: four terminals comprising source, gate, drain, and substrate, with internal source-substrate linkage. For N channels, arrows target the substrate; for P channels, they diverge from the gate.
JFETs cater to minor signal processing, contrasting MOSFETs’ role in linear and switch-mode power supplies. JFETs bifurcate into N-channel and P-channel, while MOSFETs diversify into four distinct categories: N-channel and P-channel, both in enhancement and depletion varieties. MOSFETs further segment by conductivity into vertical and lateral channels, with subsets like VMOSFET, DMOSFET, and UMOSFET.
Switching MOSFETs shine in high-frequency applications, boasting low resistance when active and small gate capacitance. Unlike typical FETs, they excel in switching operations absent linearity constraints. Predominantly featured in power supply circuits.
For N-channel MOSFETs with arrows gating inward, connect the drain to a high level (G), gate positive, and source negative. If Vgs surpasses the pinch-off threshold (sometimes around 1V), D and S activate, directing current from D to S. Adherence to G's safe voltage range (under 30V, generally around 10V) and consideration of DS voltage and transconductance are paramount (e.g., 2N60B’s IDS=2A, VDS=600V).
December 28th, 2023
July 29th, 2024
April 22th, 2024
January 25th, 2024
December 28th, 2023
December 28th, 2023
April 16th, 2024
July 4th, 2024
December 26th, 2023
August 28th, 2024