B LEVEL PROBLEMS
1)A
child on a boat throws a 5.40-kg package out horizontally with a speed
of 10.0 m/s. Calculate the velocity of the boat immediately after, assuming
it was initially at rest. The mass of the child is 26.0 kg and the mass
of the boat is 55.0 kg.
SOLUTION:
During the throwing we use momentum conservation
for the one-dimensional motion:
The
initial momentum of the system is zero; the boat, child, and package are
all at rest.
Once
the package is thrown, the boat and child move with a single velocity while
the package moves with a velocity of qo m/s.
0
= (mboat + mchild)vboat+
mpackagevpackage;
0
= (55.0 kg + 20.0 kg)vboat + (5.40 kg)(10.0 m/s), which
gives
vboat=–
0.720 m/s (opposite to the direction of the package).
2)A
9500-kg boxcar travels on a level frictionless track with a constant speed
of 18.0 m/s. A 5750-kg additional load is dropped onto the car. What is
the new speed of the car after this additional load was dropped?
SOLUTION:
For
the one-dimensional motion, we take the direction of the first car for
the positive direction.
For
this perfectly inelastic collision, we use momentum conservation:
M1v1
+ M2v2 = (M1 + M2)V;
(9500
kg)(18 m/s) + 0 = (9500 kg + 5750 kg) V, which gives V
= 11.2 m/s
3)A
15-g bullet strikes and becomes embedded in a 1.10-kg block of wood on
a horizontal surface right in front of the gun. If the coefficient of kinetic
friction between the wood and the surface is equal to 0.25, and the impact
drives the block a distance of 9.5 m before it comes to rest, what was
the muzzle speed (initial speed) of the bullet?
SOLUTION:
On
the horizontal surface after the collision, the normal force is FN
= (m + M)g. This problem can be solved by looking
at the work done by friction in slowing the object to a stop, and by using
conservation of momentum during the collision. We find the common speed
of the block and bullet immediately after the embedding
by using the work-energy principle for the sliding motion:
Wfr
= Dk;
–
µk(m
+ M)gd = 0 – ½ (M
+ m)V2;
0.25(9.80
m/s2)(9.5 m) = ½V2,
which gives V = 6.82 m/s.
For
the collision, we use momentum conservation:
mv
+ 0 = (M + m)V;
(0.015
kg)v = (0.015 kg + 1.10 kg)(6.82 m/s), which gives v
= 5.1 ´
102 m/s.
4)An
atomic nucleus initially at rest radioactively decays into an alpha particle
and a smaller nucleus. What will be the speed of the recoiling nucleus
if the speed of the alpha particle is 3.8 x 105 m/s? Assume
that the recoiling nucleus has a mass 57 times greater than that of the
alpha particle.
SOLUTION:
The
new nucleus and the alpha particle will recoil in opposite directions.
Momentum
conservation gives us
0
= MV – mava,
0
= (57ma)V
– ma(3.8
´ 105 m/s),which gives V= 6.7
´ 103 m/s.
5)A
golf ball of mass 0.045 kg is hit off the tee at a speed of 45 m/s. The
golf club was in contact with the ball for 5.0 x 10-3 s. Find
(a) the impulse imparted to the golf ball and (b) the average force exerted
on the ball by the golf club.
SOLUTION:
(a)We
find the impulse on the ball from
Impulse
= Dp = m Dv
=(0.045 kg)(45 m/s – 0) = 2.0 N·s.
(b)The
average force is
F
= Impulse/Dt = (2.0 N·s)/(5.0
´ 10–3 s) = 4.0
´ 102 N.
6)A
ball of mass 0.440 kg moving east with a speed of 3.70 m/s collides head-on
with a 0.220-kg mass at rest. If the collision is perfectly elastic, what
is the speed and direction of each ball after the collision?
SOLUTION:
For
the elastic collision of the two balls, we use momentum conservation:
m1v1
+ m2v2
= m1v1¢
+ m2v2¢;
(0.440
kg)(3.70 m/s) + (0.220 kg)(0) = (0.440 kg)v1¢
+ (0.220 kg)v2¢.
1.628
kg m/s = (0.440 kg)v1¢
+ (0.220 kg)v2¢
Because
the collision is elastic, kinetic energy is constant:
½
m1 v21
+ ½m2 v22
= ½ m1v1’2 + ½ m2v2’2,
½
(0.440 kg)(3.70 m/s)2 + 0 = ½ (0.440 kg)v1’2
+ ½ (0.220 kg)v2’2
6.02
kg m2/s2 = (0.440 kg)v1’2 +
(0.220 kg)v2’2
Combining
these two equations, we get
v1¢
= 1.23 m/s,andv2¢
= 4.93 m/s.
7)An
explosion breaks an object into two pieces one of which has 1.5 times the
mass of the other. If 7500 J were released during the explosion, how much
kinetic energy did each piece acquire?
SOLUTION:
Momentum
conservation gives
0
= m1v1¢
+ m2v2¢;
But
m2 = 1.5 m1, therefore:
0
= m1v1¢
+ 1.5m1v2¢,or
v1¢
= – 1.5v2¢.
The
kinetic energy of each piece is
k2
= ½m2v2¢2;
k1
= ½m1v1¢2
= ½ (m2/1.5)(– 1.5v2¢)2
= (1.5) ½m2v2¢2
= 1.5k2 .
The
energy supplied by the explosion produces the kinetic energy:
e
= k1 + k2
= 2.5k2;
7500
J = 2.5k2 , which
gives k2
= 3000 J.
For
the other piece we have
k1
= e – k2
=
7500 J – 3000 J = 4500 J.
Thus
k(heavier)
= 3000 J; k(lighter)
= 4500 J.
8)A
1.0 x 103 kg Toyota collides into the rear end of a 2.2 x 102
kg Cadillac stopped at a red light. The bumpers lock, the breaks are locked,
and the two cars skid forward 2.8 m before stopping. The police officer,
who is aware that the coefficient of friction between the tires and road
is 0.40, calculates the speed of the Toyota at impact. What was the speed?
SOLUTION:
On
the horizontal surface after the collision, the normal force on the joined
cars is FN = (m + M)g.
We
find the common speed of the joined cars immediately after the collision
by using the work-energy principle for the sliding motion:
Wfr
= DK;
–
µk(m
+ M)gd = 0 – ½ (M + m)V2;
0.45(9.80
m/s2)(2.8 m) = ½V2, which gives V
= 4.68 m/s.
For
the collision, we use momentum conservation:
mv
+ 0 = (m + M)V;
(1.0
´ 103 kg)v = (1.0
´ 103 kg + 2.2
´ 103 kg)(4.68 m/s), which gives v
= 15 m/s (54 km/h).
9)Four
masses m1 =2.0 kg, m2 = 1.5 kg, m3
= 1.0 kg, m4 = 0.5 kg, are at the positions r1
= (0.0,0.0) m, r2 = (2.0, 0.0) m, r3 = (-2.0,-1.0)
m, r4= (1.0,-1.0) m respectively, on the xy-plane. Find
the coordinates of the center of mass of this system.
SOLUTION:
X(cm)
= Smixi/Smi
= [(2.0 kg)(0.0) + (1.5 kg)(2.0 m) + (1.0 kg)(-2.0 m) + (0.5 kg)(1.0 m)]/(2.0
+ 1.5 + 1.0 + 0.5) kg
=
[0 + 3.0 kg-m – 2.0 kg-m + 0.5 kg-m]/(5.0 kg) = (1.5 kg-m)/(5.0 kg) =0.30
m
Y(cm)
= Smiyi/Smi
= [(2.0 kg)(0.0) + (1.5 kg)(0.0 m) + (1.0 kg)(-1.0 m) + (0.5 kg)(-1.0 m)]/(2.0
+ 1.5 + 1.0 + 0.5) kg
=
[0 + 0 – 1.0 kg-m - 0.5 kg-m]/(5.0 kg) = (-1.5 kg-m)/(5.0 kg) = -0.30
m
(0.30,
-0.30) m