Lab #3: 1-Dimensional Motion
Class: University Physics 1, Sec1, 11am Monday
Date: 2-2-15
Group Members: Tanner Rich and Austin May
Introduction:
This labs purpose is to investigate motion in 1 dimension and to familiarize ourselves
with the lab equipment
Lab #3: 1-Dimensional Motion
Class: University Physics 1, Sec1, 11am Monday
Date: 2-2-15
Group Members: Tanner Rich and Austin May
Introduction:
This labs purpose is to investigate motion in 1 dimension and to familiarize ourselves
with the lab equipment
Title: Forces
Names: Tanner Rich, Austin May, Zak Rush
Date: 3-9-15
Time: Monday, 11 am
Class: University Physics1 sec1
The data and graphs of the position vs time and velocity vs
time are shown below:
time
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0.45
0.5
0.5
Names: Zak Rush, Tanner Rich, Austin May
Class: University Physics 1 Sec.1
Time: Monday 11am 2-23-15
Free Falling Lab
Intro: The purpose of this lab was to investigate how gravity affects falling items. There is a
mathematical relationship between the fal
Tanner Rich, Stanley Archer, Donald French
University Physics 2 sec1
Thursday @ 2pm
Lab Began:9-24-15
Lab Due:10-1-15
Ohms Law and Circuit Resistance
Intro:
This experiments purpose is for the students to get acquainted with Ohms Law and apply it to
some
Tanner Rich, Stanley Archer, Donald French
University Physics 2 sec1
Thursday @ 2pm
9-10-15
Exploring the Behavior of Charges and Fields
Intro:
The purpose of this simulated lab was to the relationship between charge and the electric field.
The simulation
Linear Fit for: Latestl Potential
Pot = mx+b
g , m (Slope): 8.828 VIA
a 0 0 ‘ b (Y-Intercept): 0.01632 V
E ‘ Correlation: 09999
9 — RMSE. 0.003732 v
8 -o.27
-o.4 r r r r r
0.1 0.3
(-00047, 41090) Current 2 (A)
E
E
E
‘5
o
E
N
E
E
5
0 0,0 0.1 0.
University Physics II
Time
(seconds)
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
average time
(s)
0.5
Distance (meters)
1.355
2.937
4.643
6.788
8.277
8.68
9.852
10.938
11.613
11.622
11.25
average distance
(m)
7.995909091
Time (s) vs distance of a tossed ball
Tanner Rich, Stanley Archer, Donald French
University Physics 2 sec1
Thursday @ 2pm
9-3-15
Electrostatic Phenomena
Intro:
This labs purpose was to get us familiar with electricity and how it works. Electricity is basically
the flow of different charged el
1. The electrical potential is its greatest closest to the test charge.
2. The electric potential magnitude is the same weather or not it is positive or negative, the only
difference is that the sign will change according to whether it is + or charged.
3.
Tanner Rich, Stanley Archer, Donald French
University Physics 2 sec1
Thursday @ 2pm
Lab Began:9-24-15
Lab Due:10-1-15
Ohms Law and Circuit Resistance
Intro:
This experiments purpose is for the students to get acquainted with Ohms Law and apply it to
some
Tanner Rich, Stanley Archer, Donald French
University Physics 2 sec1
Thursday @ 2pm
9-10-15
Exploring the Behavior of Charges and Fields
Intro:
The purpose of this simulated lab was to the relationship between charge and the electric field.
The simulation
Tanner Rich, Stanley Archer, Donald French
University Physics II
Section 001
Thursday @ 2pm
9/24/15
Resistance and Multimeters
Introduction:
This lab was conducted at Arkansas State University Lab science east room 307.
The objective of this lab was to in
Tanner Rich, Stanley Archer, Donald French
University Physics 2 sec1
Thursday @ 2pm
9-3-15
Electrostatic Phenomena
Intro:
The purpose of this simulated lab was to the relationship between charge and the electric field.
The simulation was set up so that we
Tanner Rich, Stanley Archer, Donald French
University Physics II
Section 001
Thursday @ 2pm
10/29/15
Faradays Law
Introduction:
The purpose of this lab was for the students to get firsthand experience with how
Faradays Law applies in the real world. Given
Tanner Rich, Stanley Archer, Donald French
University Physics 2 sec1
Thursday @ 2pm
9-3-15
Electrostatic Phenomena
Intro:
This labs purpose was to get us familiar with electricity and how it works. Electricity is basically
the flow of different charged el
Section 5.1 Areas and Distances
th
Notes are in reference to Calculus: Early Transcendentals (7 Edition), James Stewart
The Area Problem
We begin by attempting to solve the area problem: Find the area
( ) from to .
of the region that lies under the curve
Section 5.2 The Definite Integral
th
Notes are in reference to Calculus: Early Transcendentals (7 Edition), James Stewart
Suppose we had a curve of
( ) with
rectangles we use, then
. Let
subintervals of width
(
. Let
be the number of
)
(
) be the endpoint
Section 4.1 Maximum and Minimum Values
Notes are in reference to Calculus: Early Transcendentals (7th Edition), James Stewart
Some of the most important applications of differential calculus are
optimization problems, in which we are required to find the
Section 4.8 Newtons Method
th
Notes are in reference to Calculus: Early Transcendentals (7 Edition), James Stewart
The Newtons method can be used to approximate the solutions of ( )
intercepts) of a function).
. (i.e. find the roots ( -
The geometry behin
Section 4.9 Antiderivatives
Notes are in reference to Calculus: Early Transcendentals (7th Edition), James Stewart
Suppose a physicist who knows the velocity of a particle might wish to know
its position at a given time or an engineer who can measure the
Section 4.9 Antiderivatives
th
Notes are in reference to Calculus: Early Transcendentals (7 Edition), James Stewart
Suppose a physicist who knows the velocity of a particle might wish to know its position at a given
time or an engineer who can measure the
Section 4.7 Optimization Problems
th
Notes are in reference to Calculus: Early Transcendentals (7 Edition), James Stewart
The methods we have learned in this chapter for finding extreme values have practical applications in
many areas of life. In solving
Section 3.10 Linear Approximations and Differentials
th
Notes are in reference to Calculus: Early Transcendentals (7 Edition), James Stewart
We have seen that a curve lies very close to its tangent line near
the point of tangency. In fact, by zooming in t
Section 3.10 Linear Approximations and Differentials
Notes are in reference to Calculus: Early Transcendentals (7th Edition), James Stewart
We have seen that a curve lies very close to its tangent line near the point
of tangency. In fact, by zooming in to
Section 3.7 Rates of Change in the Natural and Social Sciences
th
Notes are in reference to Calculus: Early Transcendentals (7 Edition), James Stewart
( ), then the derivative
We know that if
can be interpreted as the rate of change of
with
respect to . I