* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download Handout Topic 5, 10 New Charge Carrier Drift teacher
Operational amplifier wikipedia , lookup
Power electronics wikipedia , lookup
Power MOSFET wikipedia , lookup
Integrating ADC wikipedia , lookup
Surge protector wikipedia , lookup
Nanofluidic circuitry wikipedia , lookup
Rectiverter wikipedia , lookup
Resistive opto-isolator wikipedia , lookup
Current mirror wikipedia , lookup
Name:_________________________________ Handout Charge Carrier Drift , Kirchhoff’s laws Ideal and Non Ideal Meters Charge Carrier Drift 1. Define charge density and drift speed: Density - The number of charge carriers per 1 m3 of conductor. Drift speed -How fast the charge carriers “ drift” through a certain length – volume of 1 m3 of conductor in in one sec. Explain the following formula: I = nAvq Current = number of charge carriers x cross sectional area x velocity x charge 2. Example . Show basic work 3. Why is drift speed so slow? Use the comparison of Cu and Germanium to answer the question. It depends on charge carrier density. The higher number of charges per 1 m3 , the higher the density and the faster the drift speed and , subsequently current , will be: I α v . Cu is 109 times faster than the semiconductor Ge because of its higher charge carrier density, as a matter of fact directly proportional at 109 times more dense. 1 4. If drift speed is so slow why does a light turn on so fast? Kirchhoff’s laws Note : this is nothing new. Kirchoff’ s First Law You already know that the current going to a parallel circuit is equal to the current coming out. 2 Kirchoff’ s Second Law You already know that the sum of the individual voltage drops in a circuit is equal to the total voltage of the circuit. 3 New term Potential Difference sink = PD sink = Voltage drop Some Examples - Show Work 4 Ideal and Non Ideal Meters: Summarize the differences: 5