SlideShare a Scribd company logo
Physics Lab Page 1 of 9
AMERICAN INTERNATIONAL UNIVERSITY–BANGLADESH (AIUB)
FACULTY OF SCIENCE & TECHNOLOGY
DEPARTMENT OF PHYSICS
PHYSICS LAB 1
Summer 2022-2023 Section: C-5, Group: 08
LAB REPORT ON
Determining the acceleration due to gravity applying linear least square regression method by
using a simple pendulum.
Supervised By
DR. KAMRUN NAHAR MUKTA
Submitted By
Name ID Contribution
Date of Submission: July 11, 2023
Physics Lab Page 2 of 9
TABLE OF CONTENTS
TOPICS Page
no.
I. Title Page………………………………………………… 1
II. Table of Contents…………………………………………. 2
1. Theory……………………………………………………. 3
2. Apparatus………………………………………………… 5
3. Procedure…………………………………………………. 5
4. Experimental Data……………………………………….. 6
5. Analysis and Calculation………………………………… 7
6. Result……………………………………………………… 8
7. Discussion…………………………………………………. 8
8. References………………………………………………… 9
Physics Lab Page 3 of 9
1. Theory:
Theoretically, the period of a pendulum is independent of its mass and depends on length
according to the power of relationship.
A simple pendulum is an arrangement consisting of a metal bob connected by a light thread
and hanging vertically from a fixed support. The time required for one complete oscillation of
a basic pendulum is known as the time required for one complete oscillation is known as the
time period & it is denoted by T. L stands for effective length, which is the distance from the
point of suspension to the center of the metal bob. A basic pendulum's time period for small-
angle oscillation is,
𝑇 =2π
√𝐿
𝑔
Here, g is the acceleration due to gravity.
Rigid support
Figure 1.1: A swinging simple pendulum with an effective length L and amplitude θ.
Physics Lab Page 4 of 9
By squaring both sides, the time period equation of a simple pendulum can be written as,
The equation of the straight line passing through the origin is y = mx. Comparing this equation with
the equation of time period, the value of g i,e. acceleration due to gravity can be determined as here m
is the slope of the T 2
vs L graph.
If there are two types(one is dependent and another one independent) of variables x and f(x), the
linear least square regression method can be used for N number of data points to find the best fitted
line which is the regression line as the figure shows below,
Figure 1.2: Way to get the best fitted line by finding the minimum value of
We can determine the slope of the regression line using the formula
m=
∑ 𝑖𝑥𝑖𝑦 𝑖−
(∑ 𝑖𝑥 𝑖)(∑ 𝑖𝑦𝑖)
𝑁
∑ 𝑖𝑥𝑖2−
(∑ 𝑖𝑥𝑖)2
𝑁
and intercept c =y
̅ -mx
̅ , where x
̅ and y
̅ are mean value of x and y.
Physics Lab Page 5 of 9
In the equation of slope:
2. Apparatus:
To contrast a Simple Pendulum
1. Metal bob
2. Apiece of string
3. Stand and Clamp
Measurement of L and T:
1. Stop Watch
2. Meter Scale
3. Procedure:
1. First, we tied a light length of rope to the metal bob's hook. We measured the length of the
pendulum from the point of suspension to the bob's midpoint using a meter scale.
2. The pendulum was then given a small angle swing of less than 10 degrees. We discovered the
time period (T). To do this we calculated the total time for 20 oscillations and divided it by
20. We repeated the operation for various lengths and logged the results in table 1.1.
3. Using the Linear Least Squares Regression Method (LLSRM), we discovered the
regression line and from the value of slope we found g from the relation:
slope = 4π
2
/𝑔
4. We then displayed the same graph in Excel and calculated the value of g using the graph's
equation.
Physics Lab Page 6 of 9
4. Experimental Data:
Table 1.1: Time periods (T) for different lengths (L) of the simple pendulum
No.
of
Obs.
Effective
Length
L
(cm)
Time for 20
Oscillations
t
(s)
Time Period
T = t/20
(s)
𝑇²
(s²)
𝐿²
(cm²)
L.𝑇²
(cm.𝑠²)
1 110 42.22 2.11 4.4521 21000 975.4106
2 100 40.50 2.025 4.1006 10000 962.7473
3 90 38.81 1.9405 3.7655 8100 943.5818
4 80 36.78 1.839 3.382 6400 933.8478
5 70 33.97 1.698 2.8832 4900 958.4799
6 60 32.62 1.631 2.6601 3600 890.457
7 50 28.84 1.442 2.0793 2500 949.3199
Σ 560 23.2338 47600 6613.844
5. Analysis and Calculation:
Table 1.2: Finding the slope, m and intercept, c by using the linear least square regression method
N
∑ 𝑥𝑖
𝑖
∑ 𝑦𝑖
𝑖
∑ 𝑥𝑖𝑦𝑖
𝑖
2
(∑ 𝑥𝑖)
𝑖
∑ 𝑥𝑖²
𝑖
m c
7 560 23.3228 1974.641 313600 47600 0.03886 0.223
Equation: y = 0.03886 x +0.223
Physics Lab Page 7 of 9
A. The value of g using the LLSRM:
=
1974.641−
(560)(23.3228)
7
51600−
313600
7
= 0.03886
X
̅ =
𝑖 𝑖
∑ 𝑥
𝑁
=
560
7
=80
y
̅ =
𝑖∑ 𝑦𝑖
𝑁
=
23.3228
7
= 3.3318
Now intercept c = y
̅ -mx
̅ = 3.3318 – (0.03886) (80) = 0.223
Acceleration due to gravity by using LLSRM,
gL=
4π2
m
=
4(3.1416)2
0.03886
= 1015.91 cms-2
= 10.15 ms-2
m=
∑ 𝑖𝑥𝑖𝑦 𝑖−
(∑ 𝑖𝑥 𝑖)(∑ 𝑖𝑦 𝑖)
𝑁
∑ 𝑖𝑥𝑖2−
(∑ 𝑖𝑥𝑖)2
𝑁
Physics Lab Page 8 of 9
6613.844
7
=
B. The value of g from the graph of Excel:
Slope of the regression line, m = 0.0328 [comparing equation y = 0.03886x + 0.223 with y = mx +
c]
Acceleration due to gravity from the graph of Excel:
Gm
= 9.44 ms-2
C. Percentage of difference in g between Excel and LLSRM:
𝑔 ∼ 𝑔
𝐸 𝐿
𝑔
𝐸
× 100 = 9.8 – 9.44
9.8
× 100 = 3.673%
6. Result:
Method 2
Value of g (𝑚/𝑠 ) Comment
LLSRM 10.15 We have found small
difference in the value of g.
Mean 9.44
7. Discussion:
m=
∑ 𝑖𝑥𝑖𝑦 𝑖−
(∑ 𝑖𝑥 𝑖)(∑𝑖𝑦𝑖)
𝑁
∑ 𝑖𝑥𝑖2−
(∑ 𝑖𝑥𝑖)2
𝑁
1. The acceleration caused by gravity, symbolized by the letter "g," is the uniform acceleration
that the earth's gravitational pull causes in a body that is falling freely.
2. With the assistance of a length of rope, a stand, and a metal bob, a straightforward pendulum
can be simply built. The string ought to be massless and untraceable. Other than gravity, there
Lab Report page 9 of 9
shouldn't be any other forces produced by outside forces. To represent bob as a point, bob's
length to dimension ratio needs to be high.
3. The regression line can be obtained using the linear least square regression method (LLSRM)
by determining the minimum value of
4. For determining the slope of the regression line, the formula is and intercept 𝑐 = 𝑦 − 𝑚𝑥, where 𝑥
𝑎𝑛𝑑 𝑦 are mean value of x and y. Using these formulas we can find the slop and intercept for any
number of data.
5. This is how we can calculate the acceleration due to gravity where m = slope of the T²VS L Graph.
8. References:
 Fundamentals of Physics: Acceleration due to gravity (Chapter 13, page 360), Simple
pendulum (Chapter 15, page 425-426)
 Video Links,
 Simple pendulum: https://youtu.be/z6ZdhP167RY
 https://youtu.be/02w9lSii_Hs
 LLSRM: 1. https://youtu.be/NN62YDcr3eU
 https://youtu.be/1Q15fgz-lUk
Lab Report page 9 of 9

More Related Content

Similar to group 9 sec c3 .docx

Verification of Newton’s Law of Motion by Atwood Machine.
Verification of Newton’s Law of Motion by Atwood Machine.Verification of Newton’s Law of Motion by Atwood Machine.
Verification of Newton’s Law of Motion by Atwood Machine.
AbdulMubinBiswas
 
24 infinite 3 d cubic lattices of identical resistors
24  infinite 3 d cubic lattices of identical resistors24  infinite 3 d cubic lattices of identical resistors
24 infinite 3 d cubic lattices of identical resistors
Jihad H. Asad
 
Simulation of Simple Pendulum
Simulation of Simple PendulumSimulation of Simple Pendulum
Simulation of Simple Pendulum
inventionjournals
 
FEM 7 Beams and Plates.ppt
FEM 7 Beams and Plates.pptFEM 7 Beams and Plates.ppt
FEM 7 Beams and Plates.ppt
Praveen Kumar
 
Thesis - Design a Planar Simple Shear Test for Characterizing Large Strange B...
Thesis - Design a Planar Simple Shear Test for Characterizing Large Strange B...Thesis - Design a Planar Simple Shear Test for Characterizing Large Strange B...
Thesis - Design a Planar Simple Shear Test for Characterizing Large Strange B...Marshal Fulford
 
Lecture 1.ppt
Lecture 1.pptLecture 1.ppt
Lecture 1.ppt
SyedMuhammadTaqqiHai
 
EM_II_Project_London_Julia
EM_II_Project_London_JuliaEM_II_Project_London_Julia
EM_II_Project_London_JuliaJulia London
 
Fe33940945
Fe33940945Fe33940945
Fe33940945
IJERA Editor
 
Fe33940945
Fe33940945Fe33940945
Fe33940945
IJERA Editor
 
Numerical modeling of the welding defect influence on fatigue life of the wel...
Numerical modeling of the welding defect influence on fatigue life of the wel...Numerical modeling of the welding defect influence on fatigue life of the wel...
Numerical modeling of the welding defect influence on fatigue life of the wel...
inventy
 
Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...
Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...
Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...
SEENET-MTP
 
A Rapid Location Independent Full Tensor Gravity Algorithm
A Rapid Location Independent Full Tensor Gravity AlgorithmA Rapid Location Independent Full Tensor Gravity Algorithm
A Rapid Location Independent Full Tensor Gravity Algorithm
Pioneer Natural Resources
 
Shm 1
Shm 1Shm 1
Shm 1
syar 2604
 
1234567890-Chapter 11b_Dynamic Force Analysis.pptx
1234567890-Chapter 11b_Dynamic Force Analysis.pptx1234567890-Chapter 11b_Dynamic Force Analysis.pptx
1234567890-Chapter 11b_Dynamic Force Analysis.pptx
adonyasdd
 
Master's presentation (English)
Master's presentation (English)Master's presentation (English)
Master's presentation (English)Alexander Tsupko
 
Engineering physics lab manual
Engineering physics lab manualEngineering physics lab manual
Engineering physics lab manual
kveerabhadrarao1
 
Curve fitting - Lecture Notes
Curve fitting - Lecture NotesCurve fitting - Lecture Notes
Curve fitting - Lecture Notes
Dr. Nirav Vyas
 
Electronic structure
Electronic structureElectronic structure
Electronic structureHoshi94
 

Similar to group 9 sec c3 .docx (20)

Verification of Newton’s Law of Motion by Atwood Machine.
Verification of Newton’s Law of Motion by Atwood Machine.Verification of Newton’s Law of Motion by Atwood Machine.
Verification of Newton’s Law of Motion by Atwood Machine.
 
24 infinite 3 d cubic lattices of identical resistors
24  infinite 3 d cubic lattices of identical resistors24  infinite 3 d cubic lattices of identical resistors
24 infinite 3 d cubic lattices of identical resistors
 
Simulation of Simple Pendulum
Simulation of Simple PendulumSimulation of Simple Pendulum
Simulation of Simple Pendulum
 
FEM 7 Beams and Plates.ppt
FEM 7 Beams and Plates.pptFEM 7 Beams and Plates.ppt
FEM 7 Beams and Plates.ppt
 
Thesis - Design a Planar Simple Shear Test for Characterizing Large Strange B...
Thesis - Design a Planar Simple Shear Test for Characterizing Large Strange B...Thesis - Design a Planar Simple Shear Test for Characterizing Large Strange B...
Thesis - Design a Planar Simple Shear Test for Characterizing Large Strange B...
 
Lecture 1.ppt
Lecture 1.pptLecture 1.ppt
Lecture 1.ppt
 
DL_FinalProposal
DL_FinalProposalDL_FinalProposal
DL_FinalProposal
 
EM_II_Project_London_Julia
EM_II_Project_London_JuliaEM_II_Project_London_Julia
EM_II_Project_London_Julia
 
Fe33940945
Fe33940945Fe33940945
Fe33940945
 
Fe33940945
Fe33940945Fe33940945
Fe33940945
 
Magnetic Pendulum
Magnetic PendulumMagnetic Pendulum
Magnetic Pendulum
 
Numerical modeling of the welding defect influence on fatigue life of the wel...
Numerical modeling of the welding defect influence on fatigue life of the wel...Numerical modeling of the welding defect influence on fatigue life of the wel...
Numerical modeling of the welding defect influence on fatigue life of the wel...
 
Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...
Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...
Sergey Sibiryakov "Galactic rotation curves vs. ultra-light dark matter: Impl...
 
A Rapid Location Independent Full Tensor Gravity Algorithm
A Rapid Location Independent Full Tensor Gravity AlgorithmA Rapid Location Independent Full Tensor Gravity Algorithm
A Rapid Location Independent Full Tensor Gravity Algorithm
 
Shm 1
Shm 1Shm 1
Shm 1
 
1234567890-Chapter 11b_Dynamic Force Analysis.pptx
1234567890-Chapter 11b_Dynamic Force Analysis.pptx1234567890-Chapter 11b_Dynamic Force Analysis.pptx
1234567890-Chapter 11b_Dynamic Force Analysis.pptx
 
Master's presentation (English)
Master's presentation (English)Master's presentation (English)
Master's presentation (English)
 
Engineering physics lab manual
Engineering physics lab manualEngineering physics lab manual
Engineering physics lab manual
 
Curve fitting - Lecture Notes
Curve fitting - Lecture NotesCurve fitting - Lecture Notes
Curve fitting - Lecture Notes
 
Electronic structure
Electronic structureElectronic structure
Electronic structure
 

Recently uploaded

哪里卖(usq毕业证书)南昆士兰大学毕业证研究生文凭证书托福证书原版一模一样
哪里卖(usq毕业证书)南昆士兰大学毕业证研究生文凭证书托福证书原版一模一样哪里卖(usq毕业证书)南昆士兰大学毕业证研究生文凭证书托福证书原版一模一样
哪里卖(usq毕业证书)南昆士兰大学毕业证研究生文凭证书托福证书原版一模一样
axoqas
 
Sample_Global Non-invasive Prenatal Testing (NIPT) Market, 2019-2030.pdf
Sample_Global Non-invasive Prenatal Testing (NIPT) Market, 2019-2030.pdfSample_Global Non-invasive Prenatal Testing (NIPT) Market, 2019-2030.pdf
Sample_Global Non-invasive Prenatal Testing (NIPT) Market, 2019-2030.pdf
Linda486226
 
一比一原版(Coventry毕业证书)考文垂大学毕业证如何办理
一比一原版(Coventry毕业证书)考文垂大学毕业证如何办理一比一原版(Coventry毕业证书)考文垂大学毕业证如何办理
一比一原版(Coventry毕业证书)考文垂大学毕业证如何办理
74nqk8xf
 
一比一原版(IIT毕业证)伊利诺伊理工大学毕业证成绩单
一比一原版(IIT毕业证)伊利诺伊理工大学毕业证成绩单一比一原版(IIT毕业证)伊利诺伊理工大学毕业证成绩单
一比一原版(IIT毕业证)伊利诺伊理工大学毕业证成绩单
ewymefz
 
My burning issue is homelessness K.C.M.O.
My burning issue is homelessness K.C.M.O.My burning issue is homelessness K.C.M.O.
My burning issue is homelessness K.C.M.O.
rwarrenll
 
一比一原版(Deakin毕业证书)迪肯大学毕业证如何办理
一比一原版(Deakin毕业证书)迪肯大学毕业证如何办理一比一原版(Deakin毕业证书)迪肯大学毕业证如何办理
一比一原版(Deakin毕业证书)迪肯大学毕业证如何办理
oz8q3jxlp
 
一比一原版(UofM毕业证)明尼苏达大学毕业证成绩单
一比一原版(UofM毕业证)明尼苏达大学毕业证成绩单一比一原版(UofM毕业证)明尼苏达大学毕业证成绩单
一比一原版(UofM毕业证)明尼苏达大学毕业证成绩单
ewymefz
 
【社内勉強会資料_Octo: An Open-Source Generalist Robot Policy】
【社内勉強会資料_Octo: An Open-Source Generalist Robot Policy】【社内勉強会資料_Octo: An Open-Source Generalist Robot Policy】
【社内勉強会資料_Octo: An Open-Source Generalist Robot Policy】
NABLAS株式会社
 
一比一原版(TWU毕业证)西三一大学毕业证成绩单
一比一原版(TWU毕业证)西三一大学毕业证成绩单一比一原版(TWU毕业证)西三一大学毕业证成绩单
一比一原版(TWU毕业证)西三一大学毕业证成绩单
ocavb
 
一比一原版(Bradford毕业证书)布拉德福德大学毕业证如何办理
一比一原版(Bradford毕业证书)布拉德福德大学毕业证如何办理一比一原版(Bradford毕业证书)布拉德福德大学毕业证如何办理
一比一原版(Bradford毕业证书)布拉德福德大学毕业证如何办理
mbawufebxi
 
一比一原版(RUG毕业证)格罗宁根大学毕业证成绩单
一比一原版(RUG毕业证)格罗宁根大学毕业证成绩单一比一原版(RUG毕业证)格罗宁根大学毕业证成绩单
一比一原版(RUG毕业证)格罗宁根大学毕业证成绩单
vcaxypu
 
Adjusting primitives for graph : SHORT REPORT / NOTES
Adjusting primitives for graph : SHORT REPORT / NOTESAdjusting primitives for graph : SHORT REPORT / NOTES
Adjusting primitives for graph : SHORT REPORT / NOTES
Subhajit Sahu
 
Opendatabay - Open Data Marketplace.pptx
Opendatabay - Open Data Marketplace.pptxOpendatabay - Open Data Marketplace.pptx
Opendatabay - Open Data Marketplace.pptx
Opendatabay
 
做(mqu毕业证书)麦考瑞大学毕业证硕士文凭证书学费发票原版一模一样
做(mqu毕业证书)麦考瑞大学毕业证硕士文凭证书学费发票原版一模一样做(mqu毕业证书)麦考瑞大学毕业证硕士文凭证书学费发票原版一模一样
做(mqu毕业证书)麦考瑞大学毕业证硕士文凭证书学费发票原版一模一样
axoqas
 
一比一原版(UPenn毕业证)宾夕法尼亚大学毕业证成绩单
一比一原版(UPenn毕业证)宾夕法尼亚大学毕业证成绩单一比一原版(UPenn毕业证)宾夕法尼亚大学毕业证成绩单
一比一原版(UPenn毕业证)宾夕法尼亚大学毕业证成绩单
ewymefz
 
Best best suvichar in gujarati english meaning of this sentence as Silk road ...
Best best suvichar in gujarati english meaning of this sentence as Silk road ...Best best suvichar in gujarati english meaning of this sentence as Silk road ...
Best best suvichar in gujarati english meaning of this sentence as Silk road ...
AbhimanyuSinha9
 
FP Growth Algorithm and its Applications
FP Growth Algorithm and its ApplicationsFP Growth Algorithm and its Applications
FP Growth Algorithm and its Applications
MaleehaSheikh2
 
Levelwise PageRank with Loop-Based Dead End Handling Strategy : SHORT REPORT ...
Levelwise PageRank with Loop-Based Dead End Handling Strategy : SHORT REPORT ...Levelwise PageRank with Loop-Based Dead End Handling Strategy : SHORT REPORT ...
Levelwise PageRank with Loop-Based Dead End Handling Strategy : SHORT REPORT ...
Subhajit Sahu
 
Malana- Gimlet Market Analysis (Portfolio 2)
Malana- Gimlet Market Analysis (Portfolio 2)Malana- Gimlet Market Analysis (Portfolio 2)
Malana- Gimlet Market Analysis (Portfolio 2)
TravisMalana
 
一比一原版(BU毕业证)波士顿大学毕业证成绩单
一比一原版(BU毕业证)波士顿大学毕业证成绩单一比一原版(BU毕业证)波士顿大学毕业证成绩单
一比一原版(BU毕业证)波士顿大学毕业证成绩单
ewymefz
 

Recently uploaded (20)

哪里卖(usq毕业证书)南昆士兰大学毕业证研究生文凭证书托福证书原版一模一样
哪里卖(usq毕业证书)南昆士兰大学毕业证研究生文凭证书托福证书原版一模一样哪里卖(usq毕业证书)南昆士兰大学毕业证研究生文凭证书托福证书原版一模一样
哪里卖(usq毕业证书)南昆士兰大学毕业证研究生文凭证书托福证书原版一模一样
 
Sample_Global Non-invasive Prenatal Testing (NIPT) Market, 2019-2030.pdf
Sample_Global Non-invasive Prenatal Testing (NIPT) Market, 2019-2030.pdfSample_Global Non-invasive Prenatal Testing (NIPT) Market, 2019-2030.pdf
Sample_Global Non-invasive Prenatal Testing (NIPT) Market, 2019-2030.pdf
 
一比一原版(Coventry毕业证书)考文垂大学毕业证如何办理
一比一原版(Coventry毕业证书)考文垂大学毕业证如何办理一比一原版(Coventry毕业证书)考文垂大学毕业证如何办理
一比一原版(Coventry毕业证书)考文垂大学毕业证如何办理
 
一比一原版(IIT毕业证)伊利诺伊理工大学毕业证成绩单
一比一原版(IIT毕业证)伊利诺伊理工大学毕业证成绩单一比一原版(IIT毕业证)伊利诺伊理工大学毕业证成绩单
一比一原版(IIT毕业证)伊利诺伊理工大学毕业证成绩单
 
My burning issue is homelessness K.C.M.O.
My burning issue is homelessness K.C.M.O.My burning issue is homelessness K.C.M.O.
My burning issue is homelessness K.C.M.O.
 
一比一原版(Deakin毕业证书)迪肯大学毕业证如何办理
一比一原版(Deakin毕业证书)迪肯大学毕业证如何办理一比一原版(Deakin毕业证书)迪肯大学毕业证如何办理
一比一原版(Deakin毕业证书)迪肯大学毕业证如何办理
 
一比一原版(UofM毕业证)明尼苏达大学毕业证成绩单
一比一原版(UofM毕业证)明尼苏达大学毕业证成绩单一比一原版(UofM毕业证)明尼苏达大学毕业证成绩单
一比一原版(UofM毕业证)明尼苏达大学毕业证成绩单
 
【社内勉強会資料_Octo: An Open-Source Generalist Robot Policy】
【社内勉強会資料_Octo: An Open-Source Generalist Robot Policy】【社内勉強会資料_Octo: An Open-Source Generalist Robot Policy】
【社内勉強会資料_Octo: An Open-Source Generalist Robot Policy】
 
一比一原版(TWU毕业证)西三一大学毕业证成绩单
一比一原版(TWU毕业证)西三一大学毕业证成绩单一比一原版(TWU毕业证)西三一大学毕业证成绩单
一比一原版(TWU毕业证)西三一大学毕业证成绩单
 
一比一原版(Bradford毕业证书)布拉德福德大学毕业证如何办理
一比一原版(Bradford毕业证书)布拉德福德大学毕业证如何办理一比一原版(Bradford毕业证书)布拉德福德大学毕业证如何办理
一比一原版(Bradford毕业证书)布拉德福德大学毕业证如何办理
 
一比一原版(RUG毕业证)格罗宁根大学毕业证成绩单
一比一原版(RUG毕业证)格罗宁根大学毕业证成绩单一比一原版(RUG毕业证)格罗宁根大学毕业证成绩单
一比一原版(RUG毕业证)格罗宁根大学毕业证成绩单
 
Adjusting primitives for graph : SHORT REPORT / NOTES
Adjusting primitives for graph : SHORT REPORT / NOTESAdjusting primitives for graph : SHORT REPORT / NOTES
Adjusting primitives for graph : SHORT REPORT / NOTES
 
Opendatabay - Open Data Marketplace.pptx
Opendatabay - Open Data Marketplace.pptxOpendatabay - Open Data Marketplace.pptx
Opendatabay - Open Data Marketplace.pptx
 
做(mqu毕业证书)麦考瑞大学毕业证硕士文凭证书学费发票原版一模一样
做(mqu毕业证书)麦考瑞大学毕业证硕士文凭证书学费发票原版一模一样做(mqu毕业证书)麦考瑞大学毕业证硕士文凭证书学费发票原版一模一样
做(mqu毕业证书)麦考瑞大学毕业证硕士文凭证书学费发票原版一模一样
 
一比一原版(UPenn毕业证)宾夕法尼亚大学毕业证成绩单
一比一原版(UPenn毕业证)宾夕法尼亚大学毕业证成绩单一比一原版(UPenn毕业证)宾夕法尼亚大学毕业证成绩单
一比一原版(UPenn毕业证)宾夕法尼亚大学毕业证成绩单
 
Best best suvichar in gujarati english meaning of this sentence as Silk road ...
Best best suvichar in gujarati english meaning of this sentence as Silk road ...Best best suvichar in gujarati english meaning of this sentence as Silk road ...
Best best suvichar in gujarati english meaning of this sentence as Silk road ...
 
FP Growth Algorithm and its Applications
FP Growth Algorithm and its ApplicationsFP Growth Algorithm and its Applications
FP Growth Algorithm and its Applications
 
Levelwise PageRank with Loop-Based Dead End Handling Strategy : SHORT REPORT ...
Levelwise PageRank with Loop-Based Dead End Handling Strategy : SHORT REPORT ...Levelwise PageRank with Loop-Based Dead End Handling Strategy : SHORT REPORT ...
Levelwise PageRank with Loop-Based Dead End Handling Strategy : SHORT REPORT ...
 
Malana- Gimlet Market Analysis (Portfolio 2)
Malana- Gimlet Market Analysis (Portfolio 2)Malana- Gimlet Market Analysis (Portfolio 2)
Malana- Gimlet Market Analysis (Portfolio 2)
 
一比一原版(BU毕业证)波士顿大学毕业证成绩单
一比一原版(BU毕业证)波士顿大学毕业证成绩单一比一原版(BU毕业证)波士顿大学毕业证成绩单
一比一原版(BU毕业证)波士顿大学毕业证成绩单
 

group 9 sec c3 .docx

  • 1. Physics Lab Page 1 of 9 AMERICAN INTERNATIONAL UNIVERSITY–BANGLADESH (AIUB) FACULTY OF SCIENCE & TECHNOLOGY DEPARTMENT OF PHYSICS PHYSICS LAB 1 Summer 2022-2023 Section: C-5, Group: 08 LAB REPORT ON Determining the acceleration due to gravity applying linear least square regression method by using a simple pendulum. Supervised By DR. KAMRUN NAHAR MUKTA Submitted By Name ID Contribution Date of Submission: July 11, 2023
  • 2. Physics Lab Page 2 of 9 TABLE OF CONTENTS TOPICS Page no. I. Title Page………………………………………………… 1 II. Table of Contents…………………………………………. 2 1. Theory……………………………………………………. 3 2. Apparatus………………………………………………… 5 3. Procedure…………………………………………………. 5 4. Experimental Data……………………………………….. 6 5. Analysis and Calculation………………………………… 7 6. Result……………………………………………………… 8 7. Discussion…………………………………………………. 8 8. References………………………………………………… 9
  • 3. Physics Lab Page 3 of 9 1. Theory: Theoretically, the period of a pendulum is independent of its mass and depends on length according to the power of relationship. A simple pendulum is an arrangement consisting of a metal bob connected by a light thread and hanging vertically from a fixed support. The time required for one complete oscillation of a basic pendulum is known as the time required for one complete oscillation is known as the time period & it is denoted by T. L stands for effective length, which is the distance from the point of suspension to the center of the metal bob. A basic pendulum's time period for small- angle oscillation is, 𝑇 =2π √𝐿 𝑔 Here, g is the acceleration due to gravity. Rigid support Figure 1.1: A swinging simple pendulum with an effective length L and amplitude θ.
  • 4. Physics Lab Page 4 of 9 By squaring both sides, the time period equation of a simple pendulum can be written as, The equation of the straight line passing through the origin is y = mx. Comparing this equation with the equation of time period, the value of g i,e. acceleration due to gravity can be determined as here m is the slope of the T 2 vs L graph. If there are two types(one is dependent and another one independent) of variables x and f(x), the linear least square regression method can be used for N number of data points to find the best fitted line which is the regression line as the figure shows below, Figure 1.2: Way to get the best fitted line by finding the minimum value of We can determine the slope of the regression line using the formula m= ∑ 𝑖𝑥𝑖𝑦 𝑖− (∑ 𝑖𝑥 𝑖)(∑ 𝑖𝑦𝑖) 𝑁 ∑ 𝑖𝑥𝑖2− (∑ 𝑖𝑥𝑖)2 𝑁 and intercept c =y ̅ -mx ̅ , where x ̅ and y ̅ are mean value of x and y.
  • 5. Physics Lab Page 5 of 9 In the equation of slope: 2. Apparatus: To contrast a Simple Pendulum 1. Metal bob 2. Apiece of string 3. Stand and Clamp Measurement of L and T: 1. Stop Watch 2. Meter Scale 3. Procedure: 1. First, we tied a light length of rope to the metal bob's hook. We measured the length of the pendulum from the point of suspension to the bob's midpoint using a meter scale. 2. The pendulum was then given a small angle swing of less than 10 degrees. We discovered the time period (T). To do this we calculated the total time for 20 oscillations and divided it by 20. We repeated the operation for various lengths and logged the results in table 1.1. 3. Using the Linear Least Squares Regression Method (LLSRM), we discovered the regression line and from the value of slope we found g from the relation: slope = 4π 2 /𝑔 4. We then displayed the same graph in Excel and calculated the value of g using the graph's equation.
  • 6. Physics Lab Page 6 of 9 4. Experimental Data: Table 1.1: Time periods (T) for different lengths (L) of the simple pendulum No. of Obs. Effective Length L (cm) Time for 20 Oscillations t (s) Time Period T = t/20 (s) 𝑇² (s²) 𝐿² (cm²) L.𝑇² (cm.𝑠²) 1 110 42.22 2.11 4.4521 21000 975.4106 2 100 40.50 2.025 4.1006 10000 962.7473 3 90 38.81 1.9405 3.7655 8100 943.5818 4 80 36.78 1.839 3.382 6400 933.8478 5 70 33.97 1.698 2.8832 4900 958.4799 6 60 32.62 1.631 2.6601 3600 890.457 7 50 28.84 1.442 2.0793 2500 949.3199 Σ 560 23.2338 47600 6613.844 5. Analysis and Calculation: Table 1.2: Finding the slope, m and intercept, c by using the linear least square regression method N ∑ 𝑥𝑖 𝑖 ∑ 𝑦𝑖 𝑖 ∑ 𝑥𝑖𝑦𝑖 𝑖 2 (∑ 𝑥𝑖) 𝑖 ∑ 𝑥𝑖² 𝑖 m c 7 560 23.3228 1974.641 313600 47600 0.03886 0.223 Equation: y = 0.03886 x +0.223
  • 7. Physics Lab Page 7 of 9 A. The value of g using the LLSRM: = 1974.641− (560)(23.3228) 7 51600− 313600 7 = 0.03886 X ̅ = 𝑖 𝑖 ∑ 𝑥 𝑁 = 560 7 =80 y ̅ = 𝑖∑ 𝑦𝑖 𝑁 = 23.3228 7 = 3.3318 Now intercept c = y ̅ -mx ̅ = 3.3318 – (0.03886) (80) = 0.223 Acceleration due to gravity by using LLSRM, gL= 4π2 m = 4(3.1416)2 0.03886 = 1015.91 cms-2 = 10.15 ms-2 m= ∑ 𝑖𝑥𝑖𝑦 𝑖− (∑ 𝑖𝑥 𝑖)(∑ 𝑖𝑦 𝑖) 𝑁 ∑ 𝑖𝑥𝑖2− (∑ 𝑖𝑥𝑖)2 𝑁
  • 8. Physics Lab Page 8 of 9 6613.844 7 = B. The value of g from the graph of Excel: Slope of the regression line, m = 0.0328 [comparing equation y = 0.03886x + 0.223 with y = mx + c] Acceleration due to gravity from the graph of Excel: Gm = 9.44 ms-2 C. Percentage of difference in g between Excel and LLSRM: 𝑔 ∼ 𝑔 𝐸 𝐿 𝑔 𝐸 × 100 = 9.8 – 9.44 9.8 × 100 = 3.673% 6. Result: Method 2 Value of g (𝑚/𝑠 ) Comment LLSRM 10.15 We have found small difference in the value of g. Mean 9.44 7. Discussion: m= ∑ 𝑖𝑥𝑖𝑦 𝑖− (∑ 𝑖𝑥 𝑖)(∑𝑖𝑦𝑖) 𝑁 ∑ 𝑖𝑥𝑖2− (∑ 𝑖𝑥𝑖)2 𝑁 1. The acceleration caused by gravity, symbolized by the letter "g," is the uniform acceleration that the earth's gravitational pull causes in a body that is falling freely. 2. With the assistance of a length of rope, a stand, and a metal bob, a straightforward pendulum can be simply built. The string ought to be massless and untraceable. Other than gravity, there
  • 9. Lab Report page 9 of 9 shouldn't be any other forces produced by outside forces. To represent bob as a point, bob's length to dimension ratio needs to be high. 3. The regression line can be obtained using the linear least square regression method (LLSRM) by determining the minimum value of 4. For determining the slope of the regression line, the formula is and intercept 𝑐 = 𝑦 − 𝑚𝑥, where 𝑥 𝑎𝑛𝑑 𝑦 are mean value of x and y. Using these formulas we can find the slop and intercept for any number of data. 5. This is how we can calculate the acceleration due to gravity where m = slope of the T²VS L Graph. 8. References:  Fundamentals of Physics: Acceleration due to gravity (Chapter 13, page 360), Simple pendulum (Chapter 15, page 425-426)  Video Links,  Simple pendulum: https://youtu.be/z6ZdhP167RY  https://youtu.be/02w9lSii_Hs  LLSRM: 1. https://youtu.be/NN62YDcr3eU  https://youtu.be/1Q15fgz-lUk
  • 10. Lab Report page 9 of 9