Page 1
1. (c)
Force applied by the spring is F = – kx
? F = – k (2L?)
(? is the angular displacement from the equilibrium position). Further
Also,
?
?
2. (c) When the bob moves from maximum angular displacement ? to
mean position, then the loss of gravitational potential energy is
mgh
where h = l(1 – cos ?)
3. (a) K. E. =
At mean position, y = 0
K. E. =
P. E. =
At , y = ; P. E. = =
Ratio =
Page 2
1. (c)
Force applied by the spring is F = – kx
? F = – k (2L?)
(? is the angular displacement from the equilibrium position). Further
Also,
?
?
2. (c) When the bob moves from maximum angular displacement ? to
mean position, then the loss of gravitational potential energy is
mgh
where h = l(1 – cos ?)
3. (a) K. E. =
At mean position, y = 0
K. E. =
P. E. =
At , y = ; P. E. = =
Ratio =
=
4. (a) The two springs are in parallel.
Effective spring constant, K = K
1
+ K
2
Now, frequency of oscillation is given by
or, f = ....(i)
When both k
1
and k
2
are made four times their original values, the new
frequency is given by
= 2 f ; from eqn. (i)
5. (a) ;
Net force
t = 2t
0
Page 3
1. (c)
Force applied by the spring is F = – kx
? F = – k (2L?)
(? is the angular displacement from the equilibrium position). Further
Also,
?
?
2. (c) When the bob moves from maximum angular displacement ? to
mean position, then the loss of gravitational potential energy is
mgh
where h = l(1 – cos ?)
3. (a) K. E. =
At mean position, y = 0
K. E. =
P. E. =
At , y = ; P. E. = =
Ratio =
=
4. (a) The two springs are in parallel.
Effective spring constant, K = K
1
+ K
2
Now, frequency of oscillation is given by
or, f = ....(i)
When both k
1
and k
2
are made four times their original values, the new
frequency is given by
= 2 f ; from eqn. (i)
5. (a) ;
Net force
t = 2t
0
6. (d) K.E =
and P.E. =
At mean position d = 0. At extrement positions d = A
7. (b) For block A to move in S.H.M.
mg – N = m?
2
x
where x is the distance from mean position
For block to leave contact N = 0
8. (c) As we know, time period, T
When additional mass M is added then
or
or,
9. (d) Let the extension in the spring be x
0
at equilibrium. If F
0
be the
tension in the string then F
0
= kx
0
. Further if T
0
is the tension in the
Page 4
1. (c)
Force applied by the spring is F = – kx
? F = – k (2L?)
(? is the angular displacement from the equilibrium position). Further
Also,
?
?
2. (c) When the bob moves from maximum angular displacement ? to
mean position, then the loss of gravitational potential energy is
mgh
where h = l(1 – cos ?)
3. (a) K. E. =
At mean position, y = 0
K. E. =
P. E. =
At , y = ; P. E. = =
Ratio =
=
4. (a) The two springs are in parallel.
Effective spring constant, K = K
1
+ K
2
Now, frequency of oscillation is given by
or, f = ....(i)
When both k
1
and k
2
are made four times their original values, the new
frequency is given by
= 2 f ; from eqn. (i)
5. (a) ;
Net force
t = 2t
0
6. (d) K.E =
and P.E. =
At mean position d = 0. At extrement positions d = A
7. (b) For block A to move in S.H.M.
mg – N = m?
2
x
where x is the distance from mean position
For block to leave contact N = 0
8. (c) As we know, time period, T
When additional mass M is added then
or
or,
9. (d) Let the extension in the spring be x
0
at equilibrium. If F
0
be the
tension in the string then F
0
= kx
0
. Further if T
0
is the tension in the
thread then T
0
= mg and 2T
0
= kx
0
.
Let the mass m be displaced through a slight displacement x downwards.
Let the the new tension in the string and spring be T and F
respectively.
? and F = 2T
?
?
? Time period
10. (a) The displacement of a particle in S.H.M. is given by
y = a sin (?t + f)
velocity = = ?a cos (?t + f)
The velocity is maximum when the particle passes through the mean
position i.e.,
= ? a
The kinetic energy at this instant is given by
m = m?
2
a
2
= 8 × 10
–3
joule
or × (0.1) ?
2
× (0.1)
2
= 8 × 10
–3
Solving we get ? = ± 4
Substituting the values of a, ? and f in the equation of S.H.M., we get
y = 0.1 sin (± 4t + p/4) metre.
Page 5
1. (c)
Force applied by the spring is F = – kx
? F = – k (2L?)
(? is the angular displacement from the equilibrium position). Further
Also,
?
?
2. (c) When the bob moves from maximum angular displacement ? to
mean position, then the loss of gravitational potential energy is
mgh
where h = l(1 – cos ?)
3. (a) K. E. =
At mean position, y = 0
K. E. =
P. E. =
At , y = ; P. E. = =
Ratio =
=
4. (a) The two springs are in parallel.
Effective spring constant, K = K
1
+ K
2
Now, frequency of oscillation is given by
or, f = ....(i)
When both k
1
and k
2
are made four times their original values, the new
frequency is given by
= 2 f ; from eqn. (i)
5. (a) ;
Net force
t = 2t
0
6. (d) K.E =
and P.E. =
At mean position d = 0. At extrement positions d = A
7. (b) For block A to move in S.H.M.
mg – N = m?
2
x
where x is the distance from mean position
For block to leave contact N = 0
8. (c) As we know, time period, T
When additional mass M is added then
or
or,
9. (d) Let the extension in the spring be x
0
at equilibrium. If F
0
be the
tension in the string then F
0
= kx
0
. Further if T
0
is the tension in the
thread then T
0
= mg and 2T
0
= kx
0
.
Let the mass m be displaced through a slight displacement x downwards.
Let the the new tension in the string and spring be T and F
respectively.
? and F = 2T
?
?
? Time period
10. (a) The displacement of a particle in S.H.M. is given by
y = a sin (?t + f)
velocity = = ?a cos (?t + f)
The velocity is maximum when the particle passes through the mean
position i.e.,
= ? a
The kinetic energy at this instant is given by
m = m?
2
a
2
= 8 × 10
–3
joule
or × (0.1) ?
2
× (0.1)
2
= 8 × 10
–3
Solving we get ? = ± 4
Substituting the values of a, ? and f in the equation of S.H.M., we get
y = 0.1 sin (± 4t + p/4) metre.
11. (b)
Let BP = a, ? x = OM = a sin ? = a sin (2t)
Hence M executes SHM within the given time period and its acceleration
is opposite to x that means towards left.
12. (a) Applying linear momentum conservation,
0.5 × 3 = (1 + 0.5) v or v = 1 m/s
By conservation of energy,
After collision
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