#7.108
understand that an electric field (force field) is defined as a region where a charged particle experiences a force
#7.109
understand that electric field strength is defined as \(E = \dfrac{F}{Q}\) and be able to use this equation
#7.110
be able to use the equation \(F = \dfrac{Q_1Q_2}{4πε_0r^2}\) for the force between two charges
#7.111
be able to use the equation \(E = \dfrac{Q}{4πε_0r^2}\) for the electric field due to a point charge
#7.112
know and understand the relation between electric field and electric potential
#7.113
be able to use the equation \(E = \dfrac{V}{d}\) for an electric field between parallel plates
#7.114
be able to use \(V = \dfrac{Q}{4πε_0r}\) for a radial field
#7.115
be able to draw and interpret diagrams using field lines and equipotentials to describe radial and uniform electric fields
#7.116
understand that capacitance is defined as \(C = \dfrac{Q}{V}\) and be able to use this equation
#7.117
be able to use the equation \(W = \dfrac{1}{2}QV\) for the energy stored by a capacitor, be able to derive the equation from the area under a graph of potential difference against charge stored and be able to derive and use the equations
\(W = \dfrac{1}{2}CV^2 \) and \(W = \dfrac{\frac{1}{2}Q^2}{C} \)
#7.118
be able to draw and interpret charge and discharge curves for resistor capacitor circuits and understand the significance of the time constant RC
#7.119
CORE PRACTICAL 11: Use an oscilloscope or data logger to display and analyse the potential difference (p.d.) across a capacitor as it charges and discharges through a resistor.
#7.120
be able to use the equation \(Q = Q_0e^{-t/RC}\) and derive and use related equations for exponential discharge in a resistor-capacitor circuit,
\(I = I_0e^{-t/RC}\), and \(V = V_0e^{-t/RC}\) and the corresponding log equations
\(\ln{Q} = \ln{Q_0} - \dfrac{t}{RC}\), \(\ln{I} = \ln{I_0} - \dfrac{t}{RC}\) and \(\ln{V} = \ln{V_0} - \dfrac{t}{RC}\)
#7.121
understand and use the terms magnetic flux density B, flux φ and flux linkage Nφ
#7.122
be able to use the equation \(F = Bqv\sin{θ}\) and apply Fleming’s left-hand rule to charged particles moving in a magnetic field
#7.123
be able to use the equation \(F = BIl\sin{θ}\) and apply Fleming’s left-hand rule to current carrying conductors in a magnetic field
#7.124
understand the factors affecting the e.m.f. induced in a coil when there is relative motion between the coil and a permanent magnet
#7.125
understand the factors affecting the e.m.f. induced in a coil when there is achange of current in another coil linked with this coil
#7.126
understand how to use Lenz’s law to predict the direction of an induced e.m.f., and how the prediction relates to energy conservation
#7.127
understand how to use Faraday’s law to determine the magnitude of an induced e.m.f. and be able to use the equation that combines Faraday’s and Lenz's laws
\(ℰ = \dfrac{-d(Nφ)}{dt}\)
#7.128
understand what is meant by the terms frequency, period, peak value and root-mean-square value when applied to alternating currents and potential differences
#7.129
be able to use the equations \(V_{rms} = \dfrac{V_0}{\sqrt{2}}\) and \(I_{rms} = \dfrac{I_0}{\sqrt{2}}\)