Electrostatic principles. Field pattern in a capacitor Field strength = V/d Volts per metre (voltage gradient)

Slides:



Advertisements
Similar presentations
APPLIED PHYSICS AND CHEMISTRY ELECTRICITY LECTURE 4 Work and Electric Potential.
Advertisements

5.1 Electric potential difference, current and resistance
Electric forces and electric fields
Uniform Electric Fields
Electric Potential Energy and the Electric Potential
Coulomb law.
Electricity & Magnetism
Chapters 25--Examples.
IB 5.2 Electric Field & Potential
Two protons, each of charge 1. 6 x C are 2 x 10-5m apart
Physics 102: Lecture 4, Slide 1
PHYSICS UNIT 7: ELECTRICITY
Electrostatics and Electricity. ELECTRIC CHARGE Static Electricity: electric charge at rest due to electron transfer (usually by friction) + – + – + –
Fields 3: Electric Potential Energy. How does electric potential energy compare to gravitational potential energy? A gravitational field acts between.
Electrical Energy and Capacitance
Electric Potential Energy
Chapter 16 Electric Energy and Capacitance
Maxwell’s Equations Electromagnetic
Chapter 18 Electric Energy and Capacitance demonstrations.
ELE1110C – Tutorial Luk Chun Pong Outline -Basic concepts of Capacitors -RC circuits (DC) -Examples.
General Physics 2Electric Potential1 As with mechanics, energy is a useful quantity in studying electric forces electric potential or potential electric.
Electric Charge and Electric Field
Electric Potential Energy or Potential Difference (Voltage) Recall the idea of Gravitational Potential Energy: lifting an object against gravity requires.
Electrons Thermionic Emission
A device that can hold or store a reasonable amount of electric charge It is made of two parallel plates separated by insulator( dielectric) or air It.
Electricity and Magnetism Electric Charge Coulomb’s Law Capacitors Electric Charges and Forces.
Gioko, A. (2007). Eds AHL Topic 9.3 Electric Field, potential and Energy.
1 CAPACITORS 2 BASIC CONSTRUCTION INSULATOR CONDUCTOR + - TWO OPPOSITELY CHARGED CONDUCTORS SEPARATED BY AN INSULATOR - WHICH MAY BE AIR The Parallel.
Topic 25: Charged Particles 25.1 Electrons 25.2 Beams of charged particles.
Chapter 2.3 Capacitor Charging & Discharging Page 1 of 23 Last Updated: 1/9/2005 Electrical Theory I (ENG3322) Engineering Course Board Charging of a capacitor.
Book Reference : Pages & To look at the work of Charles Coulomb 2.To understand electric potential.
Unlike charges ATTRACT Like charges REPEL + FORCE We define the direction of the electric field at a particular place as being the direction of.
Electrostatic Forces Homework: Complete handout. Magnitude of Force According to Coulomb’s Law  The magnitude of force exerted on a charge by another.
Chapter 16 Electrical Energy and Capacitance. Objectives Electrical potential Electric Potential from a Point Charge Electron Volt Capacitance Parallel.
CAPACITORS NCEA Level 3 Physics CAPACITORS Electric field strength Capacitors Capacitance & Charge Energy in capacitors Capacitors in series and.
CAPACITORS. A capacitor is a device used to “store” electric charge. It can store energy and release it very quickly!!
Physics II, Pg 1 AP Physics Today’s Agenda AP Physics Today’s Agenda l CHAPTER 16 - ELECTRIC POTENTIAL AND ELECTRIC ENERGY; CAPACITANCE l Chp 16 problems.
Electric Fields and Forces
Electric Potential and Energy. Objectives Define work and relate it to energy Define electric potential difference, and relate it to the work done on.
Electrostatics #5 Capacitance. Capacitance I. Define capacitance and a capacitor: Capacitance is defined as the ability of an object to store charge.
Chapter 6 Motion of Charged Particles in Electric Fields.
Electric Fields Year 13. Electrostatic force Like charges repel, unlike charges attract How does this force act if charges are not in contact? –An electric.
© John Parkinson 1 2 Electric Field "An electric field is a region in which charged particles experience a force" ELECTRIC FIELD +Q FORCE -Q FORCE Lines.
Charged Particles Discovery of Electron Electron beams in Fields Electron Tubes Measurement of the Charge of the Electron.
Parallel Plates.
Capacitance Contents: Capacitance Parallel plate capacitors and dielectrics Energy RC discharge.
Electromagnetism Topic 11.1 Electrostatic Potential.
An electric force of 4.5 x N is measured between two particles. One particle has a charge of 2.0 x C & the other has a charge of 3.0 x
Static Electricity, Electric Forces, Electric Fields.
Electrons Thermionic Emission
1 Motion in Electric Fields SACE Stage 2 Physics.
Copyright © 2009 Pearson Education, Inc. E Determined from V.
Motion of Charges in Electric Fields. Electric Potential Difference.
Capacitors & Exponential Decay. Unit Structure 1.Electric and magnetic fields 2.Capacitors and exponential decay 3.Nuclear physics 4.Medical imaging 5.Modelling.
ELECTRIC Potential © John Parkinson.
What charge exists on a 30 μF capacitor (fully charged) with a 120 V potential difference between its plates and what is the energy stored? Ans: 3.6.
Storing Electrical Energy Electrical Potential (Voltage)
Charged Particles in Uniform Electric Fields
Electrons Thermionic Emission
Chapter 23 Electric Potential.
ELE 1001: Basic Electrical Technology Lecture 6 Capacitors
Electronic Physics Dr. Ghusoon Mohsin Ali
Electrical Potential Voltage.
F  eE F  ma ma  eE Electron Ballistics
Unit 2 Particles and Waves Electric Fields and Movements of Charge
Equation relating speed, frequency, and wavelength of a wave
Key Areas covered The relationship between potential difference, work and charge gives the definition of the volt. Calculation of the speed of a charged.
Electric Potential.
Lab: AC Circuits Integrated Science II.
Unit 2 Particles and Waves Electric Fields and Movements of Charge
Presentation transcript:

Electrostatic principles

Field pattern in a capacitor Field strength = V/d Volts per metre (voltage gradient)

Charging a capacitor CR 2CR 3CR 4CR Charge Current Time Q = Q o (1-e -t/RC ) = CV b (1-e -t/RC ) I = I 0 e –t/RC = (V b /R) e –t/RC

Discharging a capacitor CR 2CR 3CR 4CR Charge Time Q = Q o e -t/CR

Charging a capacitor An RC network comprises an 6 μ F capacitor and a 0.4 MΩ resistor. When a 150 V d.c. supply is applied to the network, calculate: i) initial charging current ii) time constant iii) time taken for the p.d. across the capacitor to reach 100 V iv) current, and p.d. across the capacitor, 2 seconds after connecting the supply.

Charging a capacitor i) V/R = 150/(0.4 x 10 6) = 375 μA ii) time constant = RC = (0.4 x 10 6) x (6 x 10 –6) = 2.4 Seconds

Charging a capacitor iii) v = V (1-e -t/RC ). 100 = 150 (1 - e -t/2.4 ). (100/150) - 1 = -e -t/2.4 = e -t/2.4 = 0.33 Log n 0.33 = -t/ = -t/2.4 t = 1.1x2.4 = 2.64 secs

Charging a capacitor iv) voltage after 2 seconds. v = 150 (1 - e - 2/2.4 ). 150 ( ) =150 x volts

Charging a capacitor current after 2seconds i = Ie - t/2.4. Therefore I= (375 x 10 –6) x 0.43) = 155 x A

Instantaneous current Instantaneous current, I = C x dv/dt If the voltage across a 4μF is changing at the rate 800 v/s the current flow is 4 x x 800 = 3.2 x10 -3 Amps 3.2mA

Deflection of an electron beam ve Centre line of beam Cathode (-) Anodes (+) deflecting plates Electrons are accelerated from the cathode through the anodes

Deflection of an electron beam ve Centre line of beam Cathode (-) Anodes (+) deflecting plates Electrons are accelerated from the cathode through the anodes

Deflection of an electron beam ve Centre line of beam Cathode (-) Anodes (+) deflecting plates An electron accelerated through a potential difference of 1 volt gains an electron-volt (eV) of energy

Deflection of an electron beam ve Centre line of beam Cathode (-) Anodes (+) deflecting plates One eV = 1.6 x Joules (Charge on an electron = 1.6 x coulombs)

Deflection of an electron beam ve Centre line of beam

Deflection of an electron beam ve Centre line of beam Charge on an electron q = 1.6 x coulombs Force acting on the electron = q x potential gradient F = q x v/d

Deflection of an electron beam ve Centre line of beam Vertical deflection of electron From s = ut + 0.5at 2 (suvat equation) Length of plate (l)

Deflection of an electron beam ut =0 (initial velocity indirection of deflection = 0) a = F/m =(qV/d) ÷ m q V/dm t = l/v (l = length of plate, v = electron velocity)

Deflection of an electron beam d = 0.5 x a x t 2 = 0.5 x (q V/dm) x l 2 /v 2

Deflection of an electron beam Example If the axial length of the plates is 24 mm and spacing 12 mm apart, and the axial velocity of the beam entering the plates is 15 x 10 6 m/s. Calculate, for a 60 V deflecting voltage, the transverse distance travelled by the electron beam at the point of exit from the deflecting plates.

Deflection of an electron beam Example The field strength = V/d 60/0.12 = 5000 volts/m Calculate the force exerted on the electron beam as it passes through the plates = q x Potential gradient = 1.6 x x 5000 = 8 x Newtons

Deflection of an electron beam Example The acceleration of the diverted beam resulting from the force applied = force /mass 8 x /9.1 x x10 15

Deflection of an electron beam Example From s = ut + 0.5at 2 (suvat equation) d = 0.5 x a x t 2 = 0.5 x (q V/dm) x l 2 /v (1.6x x 60)/(12 x10 -3 x 9.1 x ) X (24x10 -3 ) 2 /(15 X10 6 ) mm

Electric field from a point charge : E = k Q / r 2 (k =9.0 × 10 9 N m 2 /C 2 ) E r E is the field strength Q is the charge and r is the distance from the centre of the circle

Other equations k = 1/4πε 0 (ε 0 = permittivity of free space) F = qE (F = q x v/d) (force = charge x field strength) Electric flux density D = Q/A [coulombs/metre 2 ] Force between 2 charges (+ if unlike charges) (- if like charges)