LAB_REPORT_2-1PH3 (1)
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MCMASTER – MOHAWK JOINT VENTURE
BACHELOR OF TECHNOLOGY PARTNERSHIP
FOUR-YEAR
UNIVERSITY DEGREE PROGRAMS
EXPERIMENT NO:
TITLE:
Submitted by:
Lab Section:
Partner:
Instructor:
Date lab performed:
Date of submission:
EXPERIMENT NO. 2
FORCE AND ACCELERATION
ENG TECH 1PH3
Page
1
PURPOSE:
To study the acceleration of a free falling body to determine g, the acceleration due to gravity,
and to study the effect of changing the mass and the force on acceleration.
APPARATUS:
Lab cart (Hall's carriage), Spark timing device, Power supply, Spark sensitive paper, Tape, Meter
stick, Weights, Clamps, Thread, Pulleys, Retort stand, Spring balance, Balance.
THEORY:
An object falling in a gravitational field picks up speed as it falls. This implies that its velocity
changes (in this case, increases) with time. The rate of change of velocity with time is called
acceleration. This may be written as:
Δ
v v
−
v
a
= =
0
t
t
where: a
= acceleration (m/s
2
)
v
= final velocity (m/s)
v
0
= initial velocity (m/s)
t = time (s)
For a period of constant acceleration the displacement, x, of a moving object (distance object
travels) is the average velocity times the time period for the motion. The average velocity is the
sum of starting velocity plus final velocity all divided by 2.
⎛
v
+
v
0
⎞
x
=
v
× =
t
⎜
⎟
×
t
⎝
2
⎠
From equation (1) it is possible to manipulate the equation to solve for v.
v
=
a
×
t
+
v
0
(1)
If we substitute this value for v into the equation that defines x, the displacement can be
expressed as:
⎛
v
+
v
0
⎞
x
=
⎜
⎟
×
t
⎝
2
⎠
⎛
a
×
t
+
v
0
+
v
0
⎞
x
=⎜
⎟×
t
⎝
2
⎠
⎛
a
×
t
+
2
v
0
⎞
x
=⎜
⎟×
t
⎝
2
⎠
a
×
t
2
+
2
v
0
×
t
x
=
2
ENG TECH 1PH3
Page
2
x
=
a
×
t
2
+
v
0
×
t
x
=
at
2
+
v
0
t
x
α
t
2
(2)
The displacement is proportional to t
2
, when v
0
is zero.
The acceleration of a free falling object is commonly referred to as the acceleration due to
gravity, g. This value is approximately constant for the earth and is 9.81 m/sec
2
. This acceleration
is a constant value because it depends on the mass and radius of the earth and does not depend on
the mass of the object. A force may be defined as a push or pull that changes or tends to change
the motion of an object. A change in motion is another term for acceleration. Newton's 2
nd
law
describes the relationship between force, mass and acceleration. It is a general description of the
effect an unbalanced force will have on an object, and may be written as:
force = mass
×
acceleration
or, more simply:
f = m
×
a = ma
where:
f = force acting on an object causing it to accelerate (Newtons, N)
m = mass of the object undergoing acceleration (kilograms, kg)
a = acceleration of the object (m/s
2
)
Newton's law of universal gravitation describes a particular force that exists because of mass. It is
an attractive force that pulls together two objects of masses
M
1
and M
2
.
This attraction decreases with the square of the distance between the masses. The universal
gravitational constant, G, compensates for our earth-based metric system. The force of gravity, f
g
is defined by:
G
×
M
1
×
M
2
GM
1
M
2
f
g
=
2
=
2
r
r
where:
f
g
= gravitational force (N)
M
1
= mass of first object (kg)
M
2
= mass of second object (kg)
r
=
distance between objects (m)
G
= universal gravitational constant
=
6.67×10
-11
(N-m
2
/kg
2
)
Now if we consider the gravity between the earth (mass M
e
) and an object of mass m that is
close to the surface of the earth, the distance between the object and the centre of the earth is
essentially the radius of the earth,
r
e
.
The force of gravity, f
g
, is:
G
×
M
e
×
m
GM
1
M
2
f
g
=
2
=
2
r
e
r
But force is also defined by:
f
=
m
×
a
ENG TECH 1PH3
Page
3
Since f must equal f
g
, we can equate the equations to get:
Dividing by m we get
G
×
M
×
m
m
×
a
=
2
e
r
e
G
×
M a
=
2
e
r
e
G,
M
e
, the mass of the earth and
r
e
,
the mean radius of the earth, are all constant. The
acceleration caused by gravity (close to the surface of the earth) is also constant and is equal to
9.81 m/s
2
. If objects of different masses fall at different rates, such as a nail and a feather, it is
because the force of air friction acting on the feather is greater than the air friction acting on the
nail.
In a vacuum, the feather and the nail fall at the same rate (see
Figure 2.1).
In this
experiment, the student will determine the acceleration of gravity at the surface of the earth, g,
and measure changes in acceleration as mass and the accelerating force are changed. In order to
measure acceleration the student will use a timing device that marks a moving paper tape at
regular time intervals (see
Figure 2.2
). The distance between the marks should be increasing if
the object is undergoing acceleration because although the time difference between when the
dots are made is the same, the actual distance between the dots is increasing with time as the
tape is be speeding up. In this particular case, the time between dots is l/60
th
of a second.
Figure 2.1
Figure 2.2
1
By measuring the distance from the first dot to consecutive dots we can calculate the velocity at
every newl/60
th
of a second interval. Knowing the change in velocity from a period of l/60
th
of a
second to the next allows the student to calculate the acceleration due to gravity.
Figure 2.3
shows the paper tape connected to a thread which is run through a series of pulleys in order to
allow the mass to fall from a greater height and permit sufficient points on the tape to make the
1 Nakamura Spark Timer, Sargent-Welch, www.sargentwelch.ca.
ENG TECH 1PH3
Page
4
necessary calculations. Different masses can be used in the experiment to show that for any mass,
the acceleration due to gravity is a constant.
Figure 2.3
Figure 2.4
The mass undergoing acceleration, shown in the set-up in
Figure 2.3
, can be varied. The
accelerating force, which is caused by gravity, is directly proportional to this mass. In the set-up
shown in
Figure 2.4,
it is possible to vary the mass of the object undergoing acceleration without
necessarily increasing the accelerating force. With a frictionless (low friction) lab cart tied to the
thread, the mass of the system being accelerated can be increased while the accelerating force
pulling the system at the other end of the thread stays the same. Or this force can be increased
while simultaneously increasing the mass on the cart. Knowing the mass of the entire system, cart
+ falling mass, and the gravity acting on the falling mass, Newton's second law concerning
acceleration can be verified by comparing the ratio
of f/m
with the measured acceleration on the
tape. This acceleration is determined by measuring the increasing space between dots on the tape.
How can the force causing the acceleration be measured? The measure of any unknown force is
best determined by comparing the unknown force to a known force. This is the principle of a
spring scale shown in
Figure 2.5
. The restoring force in the spring acts against the force of
gravity. We commonly refer to the force of gravity as the weight. When the weight is balanced by
the extension of the spring in a hanging scale or the compression of the spring in a bathroom
scale, the calibration of the spring indicates how much force is causing the extension or
compression.
Figure 2.6
shows the internal construction of a typical spring scale. Mass on the
other hand is measured by a balance, which compares a known mass to an unknown mass as
shown in
Figure 2.7.
Note that often mass and weight are used in an interchangeable manner such as using kilogram
for weight instead of the correct unit, which is of course the Newton. The mass of an object is a
constant value and does not change unlike the weight, which does vary as an object moves
further away from the earth.
ENG TECH 1PH3
Page
5
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