Worksheet
5: Forces
Problem: Weight,
Normal force, and a Box
A box of mass 10.0-kg rests on a smooth table
as show in the figure.
a) Determine the weight of the box and
the normal force acting on it.
STEP 1: Draw the free-body diagram
STEP 2: The system is in equilibrium, therefore SF
= 0
FN - mg = 0
FN = mg = (10.0 kg)(9.80 m/s2)
= 98.0 N
b) You push down on the box with a force of
40.0 N. Now determine the normal force acting on the block.
STEP 1: Draw the free-body diagram
STEP 2: The system is in equilibrium, therefore SF
= 0
FN - mg - 40.0 N= 0
FN = 98.0 N + 40.0 N = 138 N
c) If you now try to pick up the box with
a force of 40.0 N, what would the normal force be now?
STEP 1: Draw the free-body diagram
STEP 2: The system is in equilibrium,
therefore SF
= 0
FN - mg + 40.0 N= 0
FN = mg - 40.0 N= 98.0 N - 40.0 N = 48.0
N
Problem 1: Solve the following force
problems
[A] What force is needed to accelerate a
child on a sled (total mass = 60.0 kg) at 1.15 m/s2?
F = ma = (60.0 kg)(1.15 m/s2) = 69.0 N
[B] A net force of 225 N accelerates a bike
and rider at 2.20 m/s2. What is the combined mass of the bike
and rider?
F = ma , therefore m = F/a
m = (225 N)/(2.20 m/s2) = 102 kg
Problem 2: Forces of 10.0 N north, 20.0 N
east, and 15.0 N south are simultaneously applied to a 4.00-kg mass. Find
the acceleration of the mass (both magnitude and direction).
Solution:
The vector equation for the forces acting on the object is:
Fnet = ( 10.0j+20.0i - 15.0j)N
= (20.0i - 5.0j)N
|F| = [(20.0)2 + (-5.0)2]1/2 =
20.6
N
q = tan-1[(-5.0)/(20.0)]
= -14.0o
Problem 3: Calculate the following:
[A] A person weighs 125 lb. Determine his
weight in Newton’s and her mass in kilograms.(1 lb. = 4.448 N)
F = 125 lb (4.448 N/lb) = 556 N
[B] What is the weight of a 66-kg astronaut
on earth?
Fg = mg = (66 kg)(9.80 m/s2) = 647 N
[C] What is the weight of the same 66-kg astronaut
on the moon? (g = 1.7 m/s2)
Fg = mg = (66 kg)(1.7 m/s2) = 112 N
[D] What is the weight of the same astronaut
in outer space traveling with constant velocity?
Since the astronaut is traveling with constant velocity, he is weightless:
Fg
= 0
Problem 4: A box weighing 70 N rests
on a table. A rope attached to that box runs up over a pulley and a second
box is attached to the other end. Determine the Normal force on the box
on that table if the hanging box weighs (a) 30 N, (b) 60 N, and (c) 90
N.
For the 70 N block: Since SF
= 0, then T + FN - 70 N = 0
FN = 70 N - T
For the hanging block: Since SF
= 0, then T = Fg
Therefore: FN = 70 N - Fg
a) Fg= 30 N
FN = 70 N - Fg = 70 N - 30 N = 40 N
b) Fg= 60 N
FN = 70 N - Fg = 70 N - 60 N = 10 N
c) Fg= 90 N
FN = 70 N - Fg = 70 N - 90 N = -20 N
=0
The block has lifted off the table, therefore the normal force is equal
to zero.
Problem 5: Two blocks on a horizontal
surface are in contact with each other as shown. The surface has friction.
A force F is applied to block 1.
(a) Draw a free body diagram for each block:
Note: FN1 and FN2 are the normal forces exerted by
the surface on block 1 and block 2 respectively, FR is
the reaction force caused by the blocks being in contact with each other,
fk1 and fk2 are the fricional forces associated with
block 1 and 2 respectively.
(b) calculate the acceleration of the system
(in terms of m1 and m2).
Solution:
Block 1: Block 1 is in equilibrium in the y-direction but accelerating
in the x-direction, therefore:
SFx
= m1a
SFy
= 0
F - FR - fk1 = m1a
FN1 = m1g
fk1= mkFN1
therefore fk1=
mkm1g
Block 2: Block 2 is in equilibrium in the y-direction but
accelerating in the x-direction, therefore:
SFx
= m2a
SFy
= 0
FR - fk2 = m2a
FN2 = m2g
fk2= mkFN2
therefore fk2=
mkm2g
This gives usthe following equations:
F - FR - fk1 = m1a (1)
fk1= mkm1g
(2)
FR - fk2 = m2a
(3)
fk2= mkm2g
(4)
Combining (1) and (2) gives us
F - FR - mkm1g
= m1a (5)
Combining (3) and (4) gives us
FR = mkm2g
+ m2a (6)
Combining (5) and (6) gives us
F - (mkm2g
+ m2a ) - mkm1g
= m1a
Now we can finally solve for a:
a = [F - mkg(m1
+m2)]/(m1
+m2)
(c) Calculate the net force on each block,
Block 1:
SFx
= m1a = m1{[F - mkg(m1
+m2)]/(m1
+m2)}
Block 2:
SFx
= m2a = m2{[F - mkg(m1
+m2)]/(m1
+m2)}
(d) calculate the contact force that each
box exerts on it’s neighbor.
FR = mkm2g
+ m2[F - mkg(m1
+m2)]/(m1
+m2)
Problem 6: A force of 40.0 N is needed
to move a 5.0-kg box across a horizontal concrete floor.
(a) What is the coefficient of static friction
between the box and the floor, just before the box moves?
Solution:
The system is in equilibrium, therefore:
SFx
=0
SFy
= 0
40.0 N = fs
FN = mg = 49.0 N
fs= msFN
ms=
fs/FN=(40.0 N)/(49.0 N) = 0.816
(b) If the 40.0 N force continues to act on
the box, the box accelerates at 0.70 m/s2. What is the coefficient
of
kinetic friction?
Solution:
The system is in not in equilibrium in the x-direction, therefore:
SFx
=ma
SFy
= 0
40.0 N - fk = ma
FN = mg = 49.0 N
fk= mkFN
mk=
fk/FN=(40.0 N - 3.50 N)/(49.0 N) = 0.745
Problem 7: A hockey puck is
on a frozen pond. It is hit and given an initial speed of 25.0 m/s. If
the puck remains on the ice at all times and comes to rest after traveling
115 m , determine the coefficient of kinetic friction between the puck
and the ice.
Solution:
The system is not in equilibrium because it is accelerating, so first,
we have to find the value of the acceleration. Knowns: Dx
= 115 m, vo = 25.0 m/s, v = 0, therefore
v2 = vo2 - 2aDx
a = (v2 - vo2)/2Dx
= -2.72 m/s2
-fk =ma
mk=
-ma/mg = -a/g = 2.72/9.80 = 0.277
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