PH2 2015 Flashcards
(33 cards)
Electric current, I
This is the rate of flow of electric charge. I=Q/t
Unit:A
Efficiency of a
system
%Efficiency = 100 x usefelwork / work put in
Potential
difference (pd), V
The pd between two points is the energy converted from
electrical potential energy to some other form per coulomb of
charge flowing from one point to the other. Unit: V [= J C-1]
Ohm’s law
The current in a metal wire at constant temperature is
proportional to the pd across it.
Electrical
resistance, R
The resistance of a conductor is the pd (V) placed across it
divided by the resulting current (I) through it. R= V/I
V= IR
Unit: Ω [= V A-1]
Resistivity, ρ
The resistance, R, of a metal wire of length L and crosssectional
area A is given by R= ρL/ A in which ρ the resistivity,
is a constant (at constant temperature) for the material of the
wire. Unit: Ω m
Superconducting
transition
temperature, Tc
The temperature at which a material, when cooled, loses all its electrical resistance, and becomes super-conducting. Some materials (e.g. copper) never become superconducting
however low the temperature becomes
The law of
conservation of
charge
Electric charge cannot be created or destroyed, (though
positive and negative charges can neutralise each other).
Charge cannot pile up at a point in a circuit.
Emf, E
The emf of a source is the energy converted from some other
form (e.g. chemical) to electrical potential energy per coulomb
of charge flowing through the source. Unit: V
Progressive
wave
A pattern of disturbances travelling through a medium and
carrying energy with it, involving the particles of the medium
oscillating about their equilibrium positions.
Transverse wave
A transverse wave is one where the particle oscillations are at
right angles to the direction of travel (or propagation) of the
wave.
Longitudinal
wave
A longitudinal wave is one where the particle oscillations are in line with (parallel to) the direction of travel (or propagation) of the wave
Polarised wave
A polarised wave is a transverse wave in which particle
oscillations occur in only one of the directions at right angles to
the direction of wave propagation
In phase
Waves arriving at a point are said to be in phase if they have
the same frequency and are at the same point in their cycles
at the same time.
[Wave sources are in phase if the waves have the same
frequency and are at the same point in their cycles at the
same time, as they leave the sources.]
Wavelength of a
progressive wave
The wavelength of a progressive wave is the minimum
distance (measured along the direction of propagation)
between two points on the wave oscillating in phase.
Frequency of a
wave
The frequency of a wave is the number of cycles of a wave
that pass a given point in one second, [or equivalently the
number of cycles of oscillation per second performed by any
particle in the medium through which the wave is passing.]
Speed of a wave
The speed of a wave is the distance that the wave profile
moves per unit time
Diffraction
Diffraction is the spreading out of waves when they meet
obstacles, such as the edges of a slit. Some of the wave’s
energy travels into the geometrical shadows of the obstacles
The principle of
superposition
The principle of superposition states that if waves from two
sources [or travelling by different routes from the same source]
occupy the same region then the total displacement at any
one point is the vector sum of their individual displacements at
that point.
Phase difference
Phase difference is the difference in position of 2 points within
a cycle of oscillation. It is given as a fraction of the cycle or as
an angle, where one whole cycle is 2π or 360], together with a
statement of which point is ahead in the cycle.
Coherence
Waves or wave sources, which have a constant phase
difference between them (and therefore must have the same
frequency) are said to be coherent.
Stationary (or
standing) wave
A stationary wave is a pattern of disturbances in a medium, in
which energy is not propagated. The amplitude of particle
oscillations is zero at equally-spaced nodes, rising to maxima
at antinodes, midway between the nodes.
Refractive
index, n
For light, Snell’s law may be written: n1 sin theta1 = n2 sin theta2 in which theta1 and theta2 are angles to the normal for light passing
between medium 1 and medium 2; n1 and n2 are called the refractive indices of medium 1 and medium 2 respectively.
The refractive index of a vacuum is fixed by convention as exactly 1. For air, n = 1.000
Snell’s law
At the boundary between any two given materials, the ratio of
the sine of the angle of incidence to the sine of the angle of
refraction is a constant