Physics - Rigid Body Dynamics solutions
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Transcript of Physics - Rigid Body Dynamics solutions
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RESONANCE SOL090313 - 1
HINTS & SOLUTIONS
DATE : 09-03-2013COURSE NAME : VIKAAS (JA) & VIPUL (JB)
TEST - 11TARGET : JEE (IITs) 2014
COURSE CODE : CLINIC CLASSES PHYSICS - Simple Harmonic Motion
1. (B)
Sol. 100TT
= 1002
1
is not valid as is not small.
g2T1
g22T2
% change = 1
12T
TT 100
= 100)12( = 41.4.2. (B)Sol. Phase of the motion is (t + ).
Using x = A sin (t + )and V = A cos(t + )for conditions at t = 0 x = A and V = 0 then = /2
When it passes equilibrium position for the first time t = 4T
Phase = 24T
.
T2
=
3. (B)Sol. Time period is independent of amplitute in SHM. Hence the time
between 2nd and 3rd collision is 2T
where
T = 2 km
Time between 2nd and 3rd collision is
t = 2T
= km
4. (B)
Sol. KA
2a
3a2
=
2a
mg A = Kmg3
5. (A)
Sol. T = g/2 TT
= 21
= 2
1 .t
So, the fractional change in the time period of a pendulum onchanging the temperature is independent of length of pendulum.
6. (D)Sol. (D) = k
0.1 = k(1.0), where k is torsional constant of the wire.
k = 101
T = 2 k
= 210/1
)2(.2552 2
= 2 102.2.10 = 4 second Ans.
7. (B)
Sol. f0 = 21
mg
where, is distance between point of suspension andcentre of mass of the body.Thus, for the stick of length L and mass m :
f0 = 21
)12/mL(2L
.g.m2
=
21
Lg6
when bottom half of the stick is cut off
f0 = 21
12)2/L(
2m
4L
.g.2m
2 = Lg12
21
= 2 f0 Ans.
8. (A)Sol. X1 = 4cost
X2 = 3sintso X = 4cost + 3sint
= 5
tsin53tcos
54
= 5 [cos37. cost + sin37. sint]= 5 cos(t 37)so phase diffrence between X1 and X2 is 37
9. (B)
Sol. Just after cutting the string extension in spring = kmg3
The extension in the spring when block is in mean position = kmg
Amplitude of oscillation
A = kmg3
kmg
= kmg2
.
10. (C)
Sol. Spring constant K = 1.04.6
= 64 N/m.
Now T = 2 km
or 64m2
4
m = 1 kg
11. (B)Sol. Speed of block is maximum at mean position. At mean position
upper spring is extended and lower spring is compressed.
-
RESONANCE SOL090313 - 2
12. (B)Sol. Potential energy U = mV
U = (50x2 + 100) 102
F = dxdU
= (100x) 102
m2x = (100 102 ) x10 103 2x = 100 102 x 2 = 100, = 10
f = 2 = 2
10 =
5
13. (C)Sol. U = 2 20 x + 5x2
F = dxdU
= 20 10x
At equilibrium position ; F = 020 10x = 0 x = 2
Since particle is released at x = 3, therefore amplitude ofparticle is 5.
5
03
5
2 7It will oscillate about x = 2 with an amplitude of 5. maximum value of x will be 7.
14. (D)
Sol.
We know that if the particle was at point B at t = 0; Thenequation of SHM will bex = A cos (t)As the phase difference between point O and P is 30, sothat between P and B is 60.And as the particle is moving towards left at t = 0, so it willbe leading the SHM x = Acos (t) by 60 Hence
x = A cos
3t
T2
15. (A)16. (A,B)17. (A,B,D)
Sol. = m
K = 10 rad/s
T = s1022
Maximum speed will be at the natural length of the spring T/
4 = 4102
= 20
s.
Time taken to cover 0.1 m is 204T s
Time taken to cover 21
0.1m is 32
4T
= s3032
4102
18. (B,C)Sol. bob will oscillate about equilibrium position
with amplitude = tan1
ga
for any value of a.If a < < g, motion will be SHM, and then
extremeegl
=tan1ag
time period will be 2
22 ga
.
19. (A,B,C,D)Sol. At t = 0
Displacement x = x1 + x2 = 4 sin 3
= 32 m.
Resulting Amplitude
A= 2881643/cos)4)(2(242 22 = 72 m
Maximum speed = A = 720 m/s
Maximum acceleration = A2 = 7200 m/s2
Energy of the motion = 21
m2 AA2 = 28 J Ans.
20. (B,C,D)Sol. At max. extension both should move with equal velocity.
k = 1120 N/m5kg 2kg
By momentum conservation,(5 3) + (2 10) = (5 + 2)VV = 5 m/sec.
Now, by energy conservation
21
5 32 + 21
2 102 = 21 (5 + 2)V2 + 2
1kx2
Put V and k
xmax= m41
= 25 cm.
Also first maximum compression occurs at ;
t = 4T3
= 43
k2 = 4
311207102
= 56
3 sec.
(where reduced mass , = 21
21mm
mm
).
21. (A,B,C)22. (A,C,D)
Sol. Kmax = 21
KA2
Eavg = 21
KA2
Vrms = 2V0
, Vavg = 0V2