trial stpm_physics term 2_module 1_ms
DESCRIPTION
Soalan Percubaan STPM Physics Penggal 2_Modul 1_MSTRANSCRIPT
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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
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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
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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
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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
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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
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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
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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