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PHYSICS 182A/195L LAB REPORT - LAB 5: NEWTON’S SECOND LAW
Lab 5: Newton’s Second Law
San Diego State University
Department of Physics
Physics 182A/195L
TA:
Alvin Yassuiae
Lab partner 1:
Matthew Ying, Olivia Sekimoto
Lab partner 2:
Tyler Shonnard, Emily Gerken
Date:
October 3, 2023
Score:
Theory
Newton's second law of motion explains the relationship between forces and the acceleration of
bodies.
“If a net external force acts on a body, the body accelerates. The direction of acceleration is the
same as the direction of the net force. The mass of the body times the acceleration vector of the
body equals the net force vector.”
This can be expressed by the vector equation:
where
is the sum of all forces acting on a mass m, and
is the acceleration of that mass. If
we are dealing with a one-dimensional system, then Newton’s law simplifies to:
Tension
Tension (T) represents the net force present on a rope, string, wire, etc. It is constrained by the
forces on either end, and remains constant as long as the rope is considered rigid and
unchanging in length. By hanging a mass on one end, and attaching the other end to a separate
mass, a system is developed.
Cart and hanging mass system
In this lab we will be analyzing the car and hanging mass system shown in the figure below.
1 Department of Physics
A cart of some mass
is tied on one end of the string with some accessory mass
attached, and the other end of the string is held over a pulley by a hanging mass
.
Assuming the only external force in the system occurs from gravity pulling on the hanging mass
, a system of equations can be used to find the net acceleration of the system. This system
of equations will be entirely one-dimensional.
First let’s consider the cart and the hanging mass separately. Using Newton’s second law, we
can relate the forces acting on the cart to the tension in the string
:
.
We treat the cart stacked with mass as a single object with mass
. When it comes to
the hanging mass, there are two forces included in the sum: the force downward from gravity
and the force upward from the tension
:
.
Careful thought will reveal that the accelerations
and
are the same. If the string
connecting the masses has a fixed length, then any displacement of
results in the same
displacement of
, and so all three masses have the same velocities and accelerations. A
definition will be made to replace these accelerations,
.
The tension is also the same for both bodies; one can be substituted into the other to form a
single equation,
.
Isolating
, this is then rewritten into the form:
.
We now define
to be the force from the hanging mass and
to be the total mass of the
system:
,
.
PHYSICS 182A/195L LAB REPORT - LAB 5: NEWTON’S SECOND LAW
So that we can write:
.
Finally, the acceleration of all masses
can be solved for by dividing the above equation by the
total mass
:
.
Procedure
Setup
1.
Measure and record the masses of the Smart Cart (scale should be located at the front
of the lab). Record the value in SI units in Table 1 and the first row of Table 2 below.
2.
Check that the PASCO Universal Interface is turned on and connect the Smart Cart via
the Hardware Setup tab (left side of the screen).
3.
Level the track with the Torpedo Level. Once the track is level, the Smart Cart should not
move in either direction when placed on the track.
4.
Check that a gate with elastic band (shown in Figure 2) or a magnetic End-Stop is
located on the end of the track between the Smart Cart and the pulley. We do not want
the Smart Cart to hit the pulley or fall off the track.
5.
Check that the Common Rate is set to 40.00 Hz (located at the bottom of the screen
next to Recording Conditions
.)
6.
Drag over 3 graphs, one for each of the parts below. They should be set to track velocity.
7.
Tie a loop in both ends of a braided physics string. Loop one end on the Smart Cart
hook, pass the string under the elastic band (or through the End-Stop hole), and hang a
mass hanger on the string over the pulley.
8.
Make sure that the string is parallel with the track from the Smart Cart hook to the pulley
(i.e. the pulley and hook should be at the same height).
The string should not touch any
other part of the setup between the hook and the pulley.
Part A
1.
Place 0.040 kg in the Smart Cart in order to set
kg.
2.
The mass hanger weighs 0.005 kg. Add a 0.015 kg mass from the Mass and Hanger set
for a total hanging mass of 0.020 kg.
3.
Pull the Smart Cart back as far as possible without allowing the mass hanger to touch
the pulley. Allow the pulley to come to rest (we do not want it to be swinging wildly when
recording data).
4.
Start Recording and release the Smart Cart.
5.
Click Stop after the Smart Cart strikes the elastic band (or End-Stop).
6.
Click on the Data Summary button (left Toolbar). Right click on the run you just made
and rename the data ‘Part A’.
7.
Use the data selection tool (yellow pen icon) to select only the linear portion of your data.
3 Department of Physics
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Layout
ReferenceS
Matlings
Review
View
Help
" Aa▼ | Ao|:、三、、|E T
AaBbCcl AaBbC AaBbCcI AABBCCD
=|三|.。
Emphasis
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Subtitle
Paragraph
Styles
EXPERIMENT ONE
The
purpose
of this experiment is to use the given data to plot graphs and determine the
experimental values of the acceleration due to gravity.
A. The table below shows data taken in a free-fall experiment. Measurements were m
the distance fall (y) at each of four precisely measured times. Complete the table. F
off to same number of decimal places, even if you carry extra digits during your
intermediate calculations.
Time, t
(s)
(s-)
yı(m)
y2(m)
y3(m)
y4(m)
ys(m)
0.00
0.00
0.00
0.00
0.00
0.00
0.00
0.00
0.50
1.0
1.4
1.1
1.4
1.5
1.28
0.25
0.75
2.6
3.2
2.8
2.5
3.1
2.84
0.5625
1.00
4.8
4.4
5.1
4.7
4.8
4.76
1.25
8.2
7.9
7.5
8.1
7,4
7.82
1.5625
1.50
cn寸|
1249
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What units will this answer be in?
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Draw arrows to illustrate the direction
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Label these two forces by name.
Do not use numbers yet.
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Assign the + value to the stronger force.
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Fill in the names of these two forces in the
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Net Force = +
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Net…
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