trial stpm_physics term 2_module 1_ms

7
1 PENGGAL 2 960/2 STPM 2015 JABATAN PENDIDIKAN NEGERI KELANTAN SIJIL TINGGI PERSEKOLAHAN MALAYSIA MARKING SCHEME PHYSICS 2 (960/2) MODULE 1

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Soalan Percubaan STPM Physics Penggal 2_Modul 1_MS

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  • 1

    PENGGAL 2

    960/2 STPM 2015

    JABATAN PENDIDIKAN NEGERI KELANTAN

    SIJIL TINGGI PERSEKOLAHAN MALAYSIA

    MARKING SCHEME

    PHYSICS 2 (960/2)

    MODULE 1

  • 2

    Marking Scheme

    1. A 6.B 11.A

    2.B 7.A 12.A

    3.D 8.A 13.B

    4.B 9.A 14.D

    5.A 10.C 15.D

    16. (a) (i) Sphere X,

    0

    1

    2

    10

    11

    4

    r

    QE

    1 M

    Sphere Y,

    0

    2

    2

    20

    22

    4

    r

    QE 1 M

    The ratio

    2

    1

    2

    1

    E

    E 1M

    (ii) Charge flow until the electric potential of the spheres are the same.

    Hence 12

    1 V

    V

    1M 1M

    (b) ErV

    Since 12

    1 V

    V

    So 1

    22

    11 rE

    rE

    from 2

    1

    2

    1

    E

    E

    Then 122

    11 r

    r

    1M

    So

    1

    2

    2

    1

    r

    r

    1M

    Total 7 M

  • 3

    17 (a) dIE L

    dt

    Symbol explained

    E = induced e.m.f. in a coil

    dI

    dt= rate of change of current in the/a same coil

    Alternative 1:

    N = LI N is the number of turns/loops

    is the magnetic flux through a coil L is the self-inductance I is the current flowing in the the/a same conductor/coil

    Alternative 2:

    = LI

    is the magnetic flux linkage L is the self-inductance I is the current flowing in the the/a same conductor/coil

    Alternative 3:

    N = LI N is the number of turns/loops

    is the magnetic flux through a coil L is the self-inductance I is the current flowing in the the/a same conductor/coil

    Alternative 4: The ratio of (magnitude) of induced/back e.m.f in a coil to the rate of change of current in the coil.

    2M/0

    (b) (i)

    dILdt

    f iI IdI

    dt t

    If = 13 4(2)

    = 5.0 A

    Alternative 1:

    dI

    Ldt

    f iI IdI

    dt t

    = 21.0 A

    1M 1M 1M OR 1M 1M 1M

    (ii) = LI

    = (0.26)(5.0) = 1.3 Wb or 5.5 Wb

    1M 1M 1M

    Total 8 M

  • 4

    18 (a) (i)

    Hzffrequency

    f

    50,

    3142

    1M

    (ii)

    V

    VVrms

    14.1

    2

    0.2

    1M 1M

    (b) (i) When ac flows in the inductor:

    magnetic flux linkage through the inductor varies sinusoidally.

    the change in magnetic flux linkage produces a back-e.m.f. // electromagnetic induction occurred inside the inductor. According to Len's law: the direction of the back-e.m.f. opposes the supply e.m.f

    1M 1M 1M

    (ii) VVE appliedback 0.1

    1M

    (iii)

    A

    A

    fL

    V

    X

    VI

    RMS

    L

    RMSRMS

    9.0

    )105502(

    41.1

    2

    3

    1M 1M

    (c) (i)

    Axis : 1M

    Magnitude : 1M (by comparindg) Shape within Period : 1M

    3M

    (ii) During t = 0 to T

    4

    1 : Power P is negative

    1M

  • 5

    power is returned completely by the inductor to the supply.

    During t = TT2

    1 to

    4

    1: Power P is positive

    -power supplied to inductors. Hence mean power = 0.

    1M 1M

    Total 15 M

    19 (a) The normal operating voltage is 240 V.

    When a voltage of 240 V is supplied, the power dissipated by the electric iron is 1.2 kW

    1 M 1M

    (b) (i) The average/mean velocity of the charge carrier/electron/ taking into

    consideration the collision with positive ions 1

    along/opposite direction of/in an electric field/potential difference applied 1

    1M 1M

    (ii)

    mV

    AN

    nV

    AN

    m

    363.5 108900

    AN

    (NA) = 8.44 1028 m3

    I nAve

    I

    vnAe

    28 3 2 19

    0.15

    8.44 10 (1.0 10 ) 1.6 10v

    Cross sectional area

    = 3.54 10-6 ms1 or 3.5 10-6 ms1 1

    1M 1M 1M 1M 1M 1M

    (c) (i) Current density

    A

    IJ

    = 3 2

    15

    (4 10 ) Area

    = 9.375 105 A m2 or 9.4 105 A m2 1

    1M 1M 1M

  • 6

    (ii) The resistance of the copper rod

    A

    lR

    8

    3 2

    1.69 10 60

    (4.0 10 )

    = 6.34 102

    1M 1M

    Total 15 M

    20 (a) (a) The hall effect is the phenomenon in which a transverse voltage is set up in a conductor carrying a current in a magnetic field

    Place a piece of n-type or p-type semiconductor in a magnetic field B Let a current I flow in the semiconductor, A millivoltmeter connected across XY of the semiconductor records the Hall voltage Or

    2M 1M 1M 1M Or 3M

    (b)

    (i) Voltage Hall HV

    ME FF

    BeeE

    acAneA

    I

    c

    VE H ,, where

    Bnea

    Ie

    c

    Ve H

    1M 1M 1M 1M

  • 7

    nea

    IBVH

    (ii) Polarities of HV ; Front edge is negative, Back edge is positive

    Or

    2M OR 2M

    (iii) The Hall effect Potential Different HV :

    Magnitude of n

    VH1

    Large HV implies ihai volume density of charge carriers is small //

    Small HV implies that volume density of charge carriers is large.

    Direction of HV perpendicular to the current in a conductor.

    If direction of HV , is as shown in the above figure, it implies that charge

    carriers are negatively charged // If direction of HV is in the opposite

    direction, its implies that carriers are positively charged.

    1M 1M 1M 1M

    Total 15 M