'Current equation' presentation slideshows

Solid State Electronics

2.36k views • 141 slides

Lecture 3: linearizing the HH equations

Lecture 3: linearizing the HH equations. HH system is 4-d, nonlinear. For some insight, linearize around a (subthreshold) resting state. (Can vary resting voltage V 0 by varying constant injected current I 0 .). Ref: C Koch, Biophysics of Computation , Ch 10. Full Hodgkin-Huxley model.

491 views • 37 slides

Next Generation Electronics from Silicon Carbide to Carbon Nanotubes and Smart Sensors: Paradigms for UMD-ARO/ARL Colla

Next Generation Electronics from Silicon Carbide to Carbon Nanotubes and Smart Sensors: Paradigms for UMD-ARO/ARL Collaboration. Neil Goldsman Dept. of Electrical and Computer Engineering. SiC, Nanotubes and Smart Sensors. Outline Existing Program: Silicon Carbide Electronics

631 views • 33 slides

Announcements

Announcements. Office hours 11am-12:30pm canceled However, I'll be back at 1pm (instead of 2pm), and I'll stay until 4:30pm (instead of 4pm). CS225: JAVA classes opened. Computer Science Minor?

239 views • 18 slides

139 views • 12 slides

LECTURE 12

LECTURE 12. FIELDS AND MATERIALS. INTRODUCTION. In our discussion of electric field thus far, we considered the medium to be free space and source to be static charges. We shall now introduce materials. Contain charged particles that respond to applied field. Conductor. Depending on their

112 views • 11 slides

LECTURE # 14

LECTURE # 14. CONDUCTOR PROPERTIES UNDER STATIC CONDITIONS. OBJECTIVES. To understand what happens to excess free charge in a conductor when exposed to external electric field. To list down various conductor properties that under static conditions. MODEL.

187 views • 9 slides

LECTURE # 14

LECTURE # 14. CONDUCTOR PROPERTIES UNDER STATIC CONDITIONS. OBJECTIVES. To understand what happens to excess free charge in a conductor when exposed to external electric field. To list down various conductor properties that under static conditions. MODEL.

94 views • 9 slides