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Physics Pop Quiz

  • 15-06-2007 7:31pm
    #1
    Registered Users, Registered Users 2 Posts: 348 ✭✭


    Hardly an original idea, but the exam is on Monday, and if it helps...


    Give three factors affecting the capacitance of a parallel plate capacitor.


«134567

Comments

  • Closed Accounts Posts: 131 ✭✭Tomlowe


    distance between plates
    permittivity of the medium between them
    area of plates

    three leptons and one property common to all leptons

    or

    one contribution made by nicholas callan


  • Closed Accounts Posts: 93 ✭✭microbiek


    permitivity and distance and dielectric?


  • Registered Users, Registered Users 2 Posts: 929 ✭✭✭sternn


    nedward wrote:
    Give three factors affecting the capacitance of a parallel plate capacitor.
    Distance between the plates
    Area of plates
    Material that the plates are made of

    State Newtons 2nd law


  • Closed Accounts Posts: 93 ✭✭microbiek


    too slow damn haha and wrong!!!


  • Closed Accounts Posts: 7,794 ✭✭✭JC 2K3


    Area of overlap of the plates.
    Distance between the plates.
    Permittivity of the medium between them.(dielectric)

    At B the sound intensity of a source is double the intensity at A. What is the difference in the sound intensity level between A and B?


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  • Closed Accounts Posts: 93 ✭✭microbiek


    3db


  • Closed Accounts Posts: 93 ✭✭microbiek


    distinguish between tranverse an longitudinal waves


  • Closed Accounts Posts: 7,794 ✭✭✭JC 2K3


    Tranverse Waves oscilate perpendicular to the plane of their direction.
    Longditudal Waves oscilate parallell to the plane of their direction.


  • Registered Users, Registered Users 2 Posts: 1,488 ✭✭✭mathew


    tomelowe wrote:
    three leptons and one property common to all leptons
    The electron, the negative muon and the negative tau.
    All leptons are fundamental particles, ie they cannot be broken down into smaller particles.

    define the ampere


  • Closed Accounts Posts: 7,794 ✭✭✭JC 2K3


    1 A = current in 2 infinitely long conductors with negligible cross section 1 m apart that put a force of 2*10^-7 N on each other in a vacuum.

    Explain how a depletion layer is formed in a PN Junction.


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  • Registered Users, Registered Users 2 Posts: 6,889 ✭✭✭tolosenc


    Holes move from P->N, and an equal number of electrons form N->P, or some such. Right?

    Why is Coulomb's Law an example of an inverse square law?


  • Registered Users, Registered Users 2 Posts: 7,046 ✭✭✭eZe^


    Because the resultant force is proportional to the square of the distance between the point charges.....



    Describe an experiment to find the critical angle of a medium.


  • Closed Accounts Posts: 93 ✭✭microbiek


    state keplers 3rd law


  • Registered Users Posts: 1,152 ✭✭✭carlowboy


    microbiek wrote:
    state keplers 3rd law

    Not on the syllabus
    Why is Coulomb's Law an example of an inverse square law?

    Force is proprtion to 1 over the square of the distance (I'm translating from irish to english so apologies for the poor wording.)


  • Closed Accounts Posts: 131 ✭✭Tomlowe


    critical angle of a solid medium

    put block of medium on a white piece of paper. place two pins at an angle to the medium and look through from the other side of the medium. find the line on which the further pin is hidden behind the nearer and insert two pins on that line

    trace around the medium, and find the tangents at the point of contact of the medium and the rays (if the medium is irregularly shaped)

    draw normals perpendicular to these tangents

    draw the lines which the pins are on, and connect the points at which they meet the medium. find the angles of incidence and refraction using a protractor. Find Sin(i)/Sin(r). this is the refractive index n. the inverse sin of 1/n is the critical angle C.



    Why does a metal covered by a piece of ordinary glass not emit electrons when incident photons are above the threshold frequency?

    (i actually dont know that one)


  • Registered Users, Registered Users 2 Posts: 7,046 ✭✭✭eZe^


    Tomlowe wrote:
    critical angle of a solid medium

    put block of medium on a white piece of paper. place two pins at an angle to the medium and look through from the other side of the medium. find the line on which the further pin is hidden behind the nearer and insert two pins on that line

    trace around the medium, and find the tangents at the point of contact of the medium and the rays (if the medium is irregularly shaped)

    draw normals perpendicular to these tangents

    draw the lines which the pins are on, and connect the points at which they meet the medium. find the angles of incidence and refraction using a protractor. Find Sin(i)/Sin(r). this is the refractive index n. the inverse sin of 1/n is the critical angle C.



    Why does a metal covered by a piece of ordinary glass not emit electrons when incident photons are above the threshold frequency?

    (i actually dont know that one)

    Ordinary glass doesnt transmit UV rays so the work function of the metal would not be overcome by the energy of the incident photon...


    Btw, with the critical angle experiment make sure the medium is a hemisphere, not a block, because otherwise the light will never be able to enter the normally and be bent properly.


  • Closed Accounts Posts: 131 ✭✭Tomlowe


    medium doesnt have anything to do with the shape of it... refractive index for a square block of glass is the same as a circular, cubic, elliptoidical, whatever block of the same glass

    do we not get a question from you?


  • Registered Users Posts: 1,152 ✭✭✭carlowboy


    I'll start again. Derive F=QVB

    That's on the syllabus isn't it?


  • Registered Users, Registered Users 2 Posts: 7,046 ✭✭✭eZe^


    Tomlowe wrote:
    medium doesnt have anything to do with the shape of it... refractive index for a square block of glass is the same as a circular, cubic, elliptoidical, whatever block of the same glass

    do we not get a question from you?

    Im talking about critical angle, a special specified activity on the syllabus though. Not the refractive index question... oh ya, em...



    State the laws of electromagnetic induction.


  • Closed Accounts Posts: 131 ✭✭Tomlowe


    Faraday - The electromotive force is proportional to the rate of change of magnetic flux linkage

    lenz - The induced emf acts in such a way as to oppose the action inducing it.

    Im pretty sure the derivation of bvq isnt on the syllabus, at least i hope it isnt...

    Define Power.


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  • Registered Users Posts: 1,152 ✭✭✭carlowboy


    Work done over time.

    Oh and derive s=ut +at^2/2


  • Registered Users, Registered Users 2 Posts: 7,046 ✭✭✭eZe^


    Tomlowe wrote:
    Faraday - The electromotive force is proportional to the rate of change of magnetic flux linkage

    lenz - The induced emf acts in such a way as to oppose the action inducing it.

    Im pretty sure the derivation of bvq isnt on the syllabus, at least i hope it isnt...

    Define Power.

    Work done per unit time... bnqv derivation is on the syllabus, its very easy though...

    take a current carrying conductor of lenght L in a magnetic field of flux density B...

    I = nq/t and v = d/t (where v linear speed of charges)
    v = L/t
    L = vt


    F = BIL
    F = B (nq/t)(vt)
    therefore, F = Bnqv....
    for one charge, n = 1


    F = Bnqv.

    Derive the 3 accelerated linear motion equations.


  • Registered Users, Registered Users 2 Posts: 7,046 ✭✭✭eZe^


    carlowboy wrote:
    Work done over time.

    Oh and derive s=ut +at^2/2



    v = u + at
    ds/dt = u + at
    Integral ds = Integral u +at dt
    s = ut + at^2/2 + c
    when t = 0, s = 0, therefore c = 0..

    therefore s = ut + 1/2 (at^2)


    Derive the other 2.


  • Closed Accounts Posts: 131 ✭✭Tomlowe


    s = Integral(v)dt
    v = Integral(a)dt

    Integral(a)dt
    = at + c
    = v (acceleration is taken to be a constant)

    let t=0 => c=u since u is initial velocity

    Integral(v)dt
    =Integral(at + u)dt
    =1/2at^2 + ut + c

    let t=0
    =>c=0 as initial displacement is zero

    therefore
    s = ut + 1/2at^2


  • Closed Accounts Posts: 131 ✭✭Tomlowe


    damn, i hate my life


  • Closed Accounts Posts: 7,794 ✭✭✭JC 2K3


    carlowboy wrote:
    I'll start again. Derive F=QVB

    That's on the syllabus isn't it?
    Yes, but the derviation in the book is ridiculous.

    In a conductor with charge, q, flowing with speed v ina magnetic field with flux density B:
    F = BIl
    I = q/t
    l = vt
    F = Bqvt/t
    F = qvB


  • Registered Users, Registered Users 2 Posts: 1,269 ✭✭✭cocoa


    eZe^ wrote:
    Btw, with the critical angle experiment make sure the medium is a hemisphere, not a block, because otherwise the light will never be able to enter the normally and be bent properly.
    <annoying pedant>actually, it is still possible, it's just a major pain to set up.</annoying pedant>
    of course, that is totally irrelevant and in an exam (or anywhere else) it is definitely a good idea to use the 'ole hemispherical block.


  • Registered Users, Registered Users 2 Posts: 7,046 ✭✭✭eZe^


    cocoa wrote:
    <annoying pedant>actually, it is still possible, it's just a major pain to set up.</annoying pedant>
    of course, that is totally irrelevant and in an exam (or anywhere else) it is definitely a good idea to use the 'ole hemispherical block.

    Could you explain to me how? Because I was arguing with my physics teacher that there definitely must be another way, and he was saying that other shapes would mean it can only enter normally one way, therefore you would have to have loads of different shapes to find the critical angle. I lost the argument! :D


  • Registered Users Posts: 1,152 ✭✭✭carlowboy


    eZe^ wrote:
    v = u + at
    ds/dt = u + at
    Integral ds = Integral u +at dt
    s = ut + at^2/2 + c
    when t = 0, s = 0, therefore c = 0..

    therefore s = ut + 1/2 (at^2)


    Derive the other 2.

    a= rate of change of velocity so
    a v/t-u/t
    at=v-u
    v=u +at

    v= u +at
    square both sides
    v^2= u^2 +2uat+(at)^2
    .....= u^2 +2a(ut +at^2/2)
    v^2= u^2 +2as

    Is mine too simplistic?


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  • Closed Accounts Posts: 7,794 ✭✭✭JC 2K3


    I presume you just measure the angle differently? Like, the angle you shine the ray at the block at would not be C, but you could get C from that...

    EDIT: Or actually, yeah, could you not just mark where the ray enters and make sure the incident ray hits a point under which you've already marked and connect em, then get C like that?


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