Presentation is loading. Please wait.

Presentation is loading. Please wait.

EEE340Lecture 191 Example 5-1: Vacuum-tube diode Electron cloud where  (y) is negative. The velocity is Newton’s law Hence where (5.9) (5.11) (5.8) y.

Similar presentations


Presentation on theme: "EEE340Lecture 191 Example 5-1: Vacuum-tube diode Electron cloud where  (y) is negative. The velocity is Newton’s law Hence where (5.9) (5.11) (5.8) y."— Presentation transcript:

1 EEE340Lecture 191 Example 5-1: Vacuum-tube diode Electron cloud where  (y) is negative. The velocity is Newton’s law Hence where (5.9) (5.11) (5.8) y Cathode Anode J E 0 (5.10)

2 EEE340Lecture 192 Therefore On the other hand, from Poisson’s Equation, where Therefore (5.14) (5.12) (5.13)

3 EEE340Lecture 193 Solving (5.14), one obtains Or Child-Langmuir law. The I-V curve can be plotted (non-linear) (5.17)

4 EEE340Lecture 194 5-3: Kirchhoff’s Voltage Law D.C. (per unit length) Skin-effect: ( 5.27) (8.57) Surface-resistance Skin depth (5.27)

5 EEE340Lecture 195 5-4: Kirchhoff’s current law versus the continuity equation. Kirchhoff’s current law: In a steady state The algebraic sum of the currents flowing out of a junction in an electric circuit is zero. Continuity (5.47) ( 5.42)

6 EEE340Lecture 196 Applying the divergence theorem The RHS of (5.42) is Equating the two sides, we have Continuity Equation (5.44)

7 EEE340Lecture 197 In combination with Ohm’s law and Gauss’s law We rewrite (5.44) into Which has a solution (5.50) (5.49)

8 EEE340Lecture 198 We define the relaxation time For copper (5.51)

9 EEE340Lecture 199 5-5: Power Dissipation and Joule’s Law Circuits Power Fields Power density (5.53)


Download ppt "EEE340Lecture 191 Example 5-1: Vacuum-tube diode Electron cloud where  (y) is negative. The velocity is Newton’s law Hence where (5.9) (5.11) (5.8) y."

Similar presentations


Ads by Google