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1 of 36 © Boardworks Ltd 2010 2 of 36 © Boardworks Ltd 2010 What is electric charge? Electric charge is a feature of certain elementary particles, such as electrons and protons, that causes them to interact with each other. The unit of electric charge is the coulomb, C. One coulomb is equivalent to the charge transported by 1 ampere of current in 1 second. Protons have an electric charge of 1.60 × 10-19 C (e). Electrons have an electric charge of -1.60 × 10-19 C (-e). Like charges repel; unlike charges attract. 3 of 36 © Boardworks Ltd 2010 Charges and electric fields An object is said to be ‘charged’ if it has an imbalance in positive and negative charges. In most cases, this is due to the addition or removal of electrons. Static electricity is a build-up of electric charge on the surface of an object due to the removal or addition of electrons, commonly caused by friction. A Van der Graaff generator uses a rubber belt rubbing against metal points to create a build-up of charge on the surface of a hollow metal sphere. 4 of 36 © Boardworks Ltd 2010 Charges and electric fields All charged objects are surrounded by a region called an electric field. An electric field is a region where a charged particle will experience a force. Electric fields can be represented by electric field lines. ● The direction of the lines represents the direction of the field – it shows the direction a positive charge would move in the field. ● The distance between lines represents the strength of the field – the closer the lines, the stronger the field. 5 of 36 © Boardworks Ltd 2010 Charged particle interactions 6 of 36 © Boardworks Ltd 2010 Inverse-square law 7 of 36 © Boardworks Ltd 2010 Coulomb’s experiments In 1783, the French physicist Charles Augustin de Coulomb measured the electrostatic force between two electric charges. He deduced that the magnitude of the force, F, between charges Q1 and Q2 is: proportional to the product of Q1 and Q2 (i.e. Q1 × Q2) inversely proportional to the square of the distance (r) between them. This forms the basis of Coulomb’s law. 8 of 36 © Boardworks Ltd 2010 Coulomb’s law Coulomb deduced that: Q 1Q 2 F r2 or: kQ1Q2 where k is a constant F = of proportionality: r2 1 k = 4πεo εo is the permittivity of free space: 8.85 × 10-12 C2 N-1 m-2 (or 8.85 × 10-12 F m-1) So Coulomb’s law can be stated as: 1 Q 1Q 2 F = 4πεo r2 9 of 36 or Q 1Q 2 F = 4πεor2 © Boardworks Ltd 2010 Coulomb’s law 10 of 36 © Boardworks Ltd 2010 Effect of distance and charge on force 11 of 36 © Boardworks Ltd 2010 Coulomb’s law: true or false? 12 of 36 © Boardworks Ltd 2010 13 of 36 © Boardworks Ltd 2010 Placing a charge in an electric field 14 of 36 © Boardworks Ltd 2010 Electric field strength Electric field strength is defined as the force experienced per unit charge. The charge in the equation refers to the charge of the particle in the field. electric field strength = force / charge E = F/Q Example: What is the electric field strength around a point charge if a 3.20 × 10-19 C charge experiences a force of 7.30 × 10-15 N? E = F/Q E = (7.30 × 10-15 ) / (3.20 × 10-19 ) E = 2.28 × 104 N C-1 15 of 36 © Boardworks Ltd 2010 Electric field strength: uniform fields The electric field between two parallel plates (e.g. capacitor plates) is uniform: a charge will experience the same force wherever it is placed between the plates. The electric field strength depends on two factors: the voltage between the plates and the distance between them. electric field strength = voltage / distance E = V/d The units of E in this instance are volts per metre (V m-1). 16 of 36 © Boardworks Ltd 2010 Electric field strength: radial fields 17 of 36 © Boardworks Ltd 2010 Electric field strength calculations 18 of 36 © Boardworks Ltd 2010 Zero values of E between two charges (1) In the case of two positive or two negative point charges, there is a point along the line between the two charges where the electric field strength is zero. Can you explain why? E is a vector quantity that acts in the same direction as the force on a positive charge placed in the field. Therefore the strength of each field will be equal and opposite at some point along the line above, and the vector sum will be zero. Where will that point be in the above example if Q1 = 2Q2? 19 of 36 © Boardworks Ltd 2010 Zero values of E between two charges (2) At what point will E be zero if Q1 = 2Q2? When E is 0: E1 = E2 Substitute in equations for E: Q1/4πεor12 = Q2/4πεor22 Cancel constants: Q1/r12 = Q2/r22 Q1 = 2Q2 so: 2Q2/r12 = Q2/r22 Cancel Q2 values from each side: 2 = r12/r22 Square root each side: √2 = r1/r2 Multiply both sides by r2: r1 = r2√2 20 of 36 © Boardworks Ltd 2010 Zero values of E between two charges (3) At what point will E be zero if Q1 = 2Q2? r1 = r2√2 This means that the point lies along the line further from Q1 than from Q2. The exact distance can be calculated if necessary by working out the fraction of the total distance r1 and r2 make up: r1 is √2/(1+√2) of the total distance from Q1 r2 is 1/(1+√2) of the total distance from Q2. 21 of 36 © Boardworks Ltd 2010 Electric field strength: summary 22 of 36 © Boardworks Ltd 2010 23 of 36 © Boardworks Ltd 2010 What is electric potential? If a positive test charge is moved from infinity to a position in an electric field, the electric potential energy (Ep) of that charge will change. In other words work is done on the charge. electric field positive test charge at infinity Zero Ep can be set anywhere, but in electric fields around a point charge it is set at infinity. This is because the strength of the field would also be zero at infinity. 24 of 36 © Boardworks Ltd 2010 What is electric potential? The electric potential at a certain position in an electric field is the work done per unit positive charge when a positive test charge is moved from infinity to that position. electric potential = electric potential energy / charge V = Ep / Q In other words, electric potential is voltage, and is measured in volts (V) or joules per coulomb (J C-1). Rearranging gives: electric potential energy = electric potential × charge Ep = QV 25 of 36 © Boardworks Ltd 2010 Electric potential and radial fields The electric potential, V, near a point charge, Q, at a distance r is given by the formula: Q V = 4πεor Example: What is the electric potential at a distance of 20.0 mm around a point charge of 1.40 × 10-8 C? Q V = 4πεor 1.40 × 10-8 V = 4 × π × (8.85 × 10-12) × 0.02 V = 6294 V 26 of 36 © Boardworks Ltd 2010 Electric potential calculations 27 of 36 © Boardworks Ltd 2010 Equipotentials 28 of 36 © Boardworks Ltd 2010 Potential gradients 29 of 36 © Boardworks Ltd 2010 Electric potential: summary 30 of 36 © Boardworks Ltd 2010 Gravitational fields vs. electric fields 31 of 36 © Boardworks Ltd 2010 32 of 36 © Boardworks Ltd 2010 Glossary 33 of 36 © Boardworks Ltd 2010 What’s the keyword? 34 of 36 © Boardworks Ltd 2010 Electric fields: equations summary 35 of 36 © Boardworks Ltd 2010 Multiple-choice quiz 36 of 36 © Boardworks Ltd 2010