A-Level Physics OCR B H557

6.1.2: Charge and field

#6.1.2a(i)

uniform electric field E=VdE = \dfrac{V}{d}

#6.1.2a(ii)

the electric field of a charged object, and the force on a charge in an electric field; inverse square law for point charge

*Spherically symmetrical charged conductor is equivalent to a point charge at its centre *

#6.1.2a(iii)

electrical potential energy and electric potential due to a point charge; 1r\dfrac{1}{r} relationship

#6.1.2a(iv)

evidence for discreteness of charge on electron

Such as the Millikan oil drop experiment

#6.1.2a(v)

the force on a moving charged particle due to a uniform magnetic field

#6.1.2a(vi)

similarities and differences between electric and gravitational fields.

#6.1.2b

Make appropriate use of:

(i) the terms: charge, electric field, electric potential, equipotential surface, electronvolt

by sketching and interpreting:

(ii) graphs showing electric potential as area under a graph of electric field versus distance, graphs showing changes in electric potential energy as area under a graph of electric force versus distance between two distance values

(iii) graphs showing force as related to the tangent of a graph of electric potential energy versus distance, graphs showing field strength as related to the tangent of a graph of electric potential versus distance

(iv) diagrams of electric fields and the corresponding equipotential surfaces.

#6.1.2c(i)

for radial components Felectric=kqQr2F_{electric} = \dfrac{kqQ}{r^2}, Eelectric=Felectricq=kQr2E_{electric} = \dfrac{F_{electric}}{q} = \dfrac{kQ}{r^2} where k=14πε0k = \dfrac{1}{4πε_0}

#6.1.2c(ii)

Eelectric=dVelectricdrE_{electric} = -\dfrac{dV_{electric}}{dr} , Eelectric=VdE_{electric} = \dfrac{V}{d} (for a uniform field)

#6.1.2c(iii)

electrical potential energy = kQqr\dfrac{kQq}{r} , Velectric=kQrV_{electric} = \dfrac{kQ}{r}

#6.1.2c(iv)

F=qvBF = qvB

6.1.1
Electromagnetism
6.2.1
Probing deep into matter