electro Flashcards

1
Q

insulator v conductor

A

electrons held close to nuclei vs not

insulators do not distribute charge over surface, conductors do

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2
Q

Coulombs law

A

= magnitude of electrostatic force between two charges

Fe = k(q1q2)/ r^2

k = electrostatic constant
q1 q2= two charges
r = distance between charges

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3
Q

Electric field

A

every electric sets up electric field around it

  • make their presence known by exerting forces on other charges
  • attract/repell force- determine through test charge
  • vector quantity, has direction
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4
Q

Find magnitude of electric field

Method #1

A

method 1: E= Fe/ q
electrostatic force divided by q

method 2: E = kQ / r^2
without test charge q

q = test charge 
Q = source of the force felt by the test charge 

electric field = vector so this is magnitude, how to find direction?
use R hand rule:

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5
Q

Magnitude of electric field

Method #2

A

does not require test charge
need to know:
- magnitude of source charge Q
- distance between Q and some point in space at which we want to measure the E- field

method 2: E = kQ / r^2

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6
Q

Electric field vector

A

direction that a positive test charge would move in the presence of a source charge

  • would repel away from another +
  • would come toward another -

positive charges have field vectors that radiate outward
negative charges have field vectors that radiate inward

field is stronger where field lines are closer together

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7
Q

Electric Field vector and direction of e- force

A

in regards to e- field and direction of
electrostatic force:
- for a positive test charge q, the force is in the direction of the e- field
- for a negative test charge q, the force is in the direction opposite of the e- field

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8
Q

Electric potential energy

A

4th form of potential energy

EPE= U = kQq / r
measured in joules

a positive EPE = charges are like, repel, loaded

a negative EPE= charges are opp, attract, will become increasingly negative as charges are brought closer
here increasingly negative–> decreasing value

EPE also = the amount of work necessary to being the charge from infinity to that point

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9
Q

Electric potential energy as work

A

= the amount of work necessary to being the charge from infinity to that point

EPE= U = W = Fdcos (theta) = kQq/r
measured in Joules

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10
Q

Electric potential

A

= ratio of the magnitude of the electric potential energy and the magnitude of the charge itself
its EPE over its charge

V = EPE/q = U/q
measured in volts, 1 volt = 1 J/C

is a scalar quantity, sign determined by Q:

  • Q is + then V is +
  • Q is - then V is -
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11
Q

Find Electric potential without test charge

A

V = kQ/ r

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12
Q

Voltage

A

since two different points at two different places will have different electric potentials,
they are said to have potential difference

voltage = potential difference 
voltage = deltaV = Vb - Va
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13
Q

Voltage and work

A

voltage = deltaV = Vb- Va = Wab/q

where Wab is the work it would take to move a test charge q through an e- field from point a to point b

point a and b are not charges, just places

For a +q:
will move to decrease electric potential
moving from higher potential to lower potential is spont:
so if Va > Vb then deltaV will be negative
then work will be negative, represents decrease in EPE

For a -q:
will move to increase electric potential V
opposite is true, work is negative if Va < Vb
W (-) / q(-) = positive delta V
work is still negative so EPE still decrease

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14
Q

equation chart

A

pg `161

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15
Q

Equitpotent lines

A

Lines where potential is the same at any point along the line

ex: electron orbital, potential only varies when u jump to another orbital (work done, depends on the potential difference or voltage)

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16
Q

Calculate the electric potential at some point P near the dipole

A

need picture

V= (kq/r1) - (kq/r2)

For points relatively distant from the dipole,

V = (kqd)/r^2 x cos theta
what is theta

17
Q

dipole moment

A

p=qd

18
Q

perpendicular bisector of the dipole

A

along this, electric potential = 0

19
Q

Magnetic field & types

A

created by any moving charge.
measured in Tesla

diamagnetic = atoms of no unpaired e-, no net mag field

  • slightly repelled by magnetic, weakly anti-magnetic
  • i.e.: wood, plastic, glass, skin

paramagnetic = have unpaired e-, become weakly magnetized and align dipoles in e- field presence

  • but reorient randomly upon removal
  • i.e.: aluminum, copper, gold

ferromagnetic = unpaired e-, strongly magnetized in mag field,

20
Q

Magnitude of magnetic field for linear wire

A

B = (uo)I / 2pi(r)
gives magnitude at any perpendicular distance r from the wire

I = current 
uo = permeability of free space constant

straight wires form mag field lines in concentric way:

to determine direction:
R hand rule, closed palm, fingers wrap:
thumb = current
wrapped fingers = magnetic field lines

21
Q

Magnitude of magnetic field for looped wire

A

B = (uo)I/2r
missing pi

gives magnitude only at center

to determine direction:
R hand rule, closed palm, fingers wrap:
thumb = current
wrapped fingers = magnetic field lines

22
Q

Force on moving charge

A

magnitude:

Fb = qvB sin theta

q= the charge 
B= mag of magnetic field
v= velocity 
theta = minimal angle bw B and v

to determine direction of force= 2nd R hand rule

  • open palm = Fb, force direction
  • thumb = velocity way
  • fingers = field lines of B mag field
23
Q

Force on current carrying wire

A

Fb = ILB sin theta

theta is angle bw B and L
L = length of wire

24
Q

Lorentz force

A

Sum of electrostatic and magnetic forces on a body