capacitors (everything) Flashcards
what are the propities of a dialectric
-insolator
-polerisable
capacitence equation
thereofre
give unit of capacitence
C=Q/V
=CV^-1
1 F (farad) = 1 CV^-1
what is the capacitence eqauation (not C=Q/V)
what does this equation assume
C=Aε0εr/d
A is area of parrelel plates
d is distence between parellel plates
ε0 is permetivity of free space
εr is reletive permativity
the plates are parallel
what are 3 ways to increse C
incresase A
incresease εr
decrease d
reletive permativity (or dialetic constent) equation
εr=ε1/ε0
where ε1 is the reletive permativity of meterial 1
molecules in the dielectric of an uncharged capacitor point __ _______ ______.
this means…
in random directions
the molecules and therefore the larger dielectric are unpolerised
Explain and decribe, with refrence to molecules, the effect of polarisation within a dialectric
- when charge is applied to a capacitor, an electric field is generated
- this means all the molecules in the dialectric will be polerised and orentate the negetive end of the molecules to the positeve charged plate and visa versa
- the polerised molecules now generat an elecric field of there own that opposes the capacitors elecrtic feild
- this reduces the overall electric feild, which reduces the pd across the capacitor, which reduces the p.d needed to charge the capacitor allowing more charge to be deposited at the plates, increaseing capacitence
↑C=Q/↓V
Q ∝…
draw a Q over p.d graph
what is the area
therefore
give an energy (E) equation
Q∝p.d
see pg133
enegy stored
E=1/2 QV
give all 3 E equations
E=1/2 QV
E=1/2 CV^2
E=1/2 (Q^2)/C
decribe the process of charging a capacitor in terms of the electrons
(Dubble check)
- when power supply is turned on charge starts to flow, negetive charge starts to build up on the capacitor plate conneted to the negetive terminal (e- flow opposite to flow of current)
- the build up of negetive charge repelse electrons off the opposing plate
- an equal but opposite charge builds up on each plate
- as there is more charge built up on each plate it becomes harder for charge to be deposited because of eectrostatic repulsion
- when p.d across the capacitor = p.d across the power supply
current fals to 0
for capacitors to build up charge the type of power supply must be…
dc
what is the area beneth a I/t graph
what is the graidint of a Q/t graph
charge Q
current I
when dischargeing current flows…
opposit direction to charging current
time taken to charge or discharge depends on…
capacitence C
and resistnece R
give all charging equations
sketch the graphs
Q = Q0(1-e^-t/RC)
V = V0(1-e^-t/RC)
I=Ioe^-t/RC