2022-10-01 11:02 Status: # MOSFET Current Equations Drain current flows into the drain terminal. ID can be derived from the operating range of the transistor. Cutoff: $I_D = 0$ Triode: $I_D=\mu C_{OX} \frac{W}{L}((V_{GS}-V_{TH})V_{DS}-\frac{1}{2} V_{DS}^2)$ Where $\mu C_{OX}$ is the current factor (can be called K, K' but these are ambiguous - use $\mu C_{OX}$ for clarity) $V_{TH}$ is the threshold voltage. Given $V_{GS}>V_{TH}$, $V_{DS}<V_{GS}-V_{TH}$ Saturation: (Current independent of drain-source voltage) $I_D=\frac{1}{2}\mu C_{OX} \frac{W}{L}(V_{GS}-V_{TH})^2$ for $V_{GS}>V_{TH}$, $V_{DS}>V_{GS}-V_{TH}$ Graph: ![](attachments/Pasted%20image%2020221001123623.png#invert) Saturation for MOSFET vs. active for BJT ![](attachments/Pasted%20image%2020221001123705.png#invert) ## Further Detail Best idea is to use the simplest equation that explains the phenomena you're looking for else it's too difficult to do analysis. ### Issues with simple model for current Output impedance in saturation becomes infinite (1/slope) This implies an amplifier with infinite gain can be created. Need to include [channel length modulation](channel%20length%20modulation.md). This becomes a factor: ![](attachments/Pasted%20image%2020221001124105.png#invert) Introduces a slope: also include in the triode (not really necessary) ![](attachments/Pasted%20image%2020221001124129.png#invert) $\lambda = \frac{k_\lambda}{L}$ ## Process Constant Summary Can be found in the design kit. - $\mu C_{OX}$ is the current factor - $V_{TH}$ is the threshold voltage - $k_\lambda$ is the [[channel length modulation](channel%20length%20modulation.md)](channel%20length%20modulation.md) constant ## Bulk Source Voltage $V_{TH} = V_{THO} + \gamma(\sqrt{|2\Phi_F-V_{BS}|}-\sqrt{|2\Phi_F|})$ Process constants: ![](attachments/Pasted%20image%2020221001172830.png#invert) ![](attachments/Pasted%20image%2020221001172901.png#invert) Ignore whenever you can if possible. If you increase the bulk source voltage, the threshold voltage decreases and the current increases. The bulk is called the 'back-gate'' because it has a similar effect to the gate (increase bulk V, increase the current!) ## PMOS ![](attachments/Pasted%20image%2020221002121029.png#invert) We can also define these voltages as reversed so the equations to make it the same! ### PMOS Equations ON: $V_{GS} < 0$ $V_{DS}<0$ $V_{BS}\geq0$ (else forward bias the diode) $I_D<0$ $\mu C_{OX}<0$ $V_{TH}<0$ and so on... ### NMOS Equations Flip the PMOS signs: $V_{GS} > 0$ $V_{DS}>0$ $V_{BS}\leq0$ $I_D>0$ $\mu C_{OX}>0$ $V_{TH}>0$ ... [^1] --- # References [^1]: [vr-4602-wk03-sc03-currentequations](../../Spaces/University/ELEC4602%20–%20Microelectronics%20Design%20and%20Technology/Lectures/W2/vr-4602-wk03-sc03-currentequations.mp4)