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What is Physics
Wednesday, December 15, 2010 | | 0 Comments »Analysing scientific Investigation
| | 0 Comments »A variable is a quantity that can vary in value.
Manipulated variable is a variable that is set or fixed before and experiment is carried out. it is usually plotted on x- axis.
Responding variable is a variable that changes according to and dependent to manipulated variable. it is usually plotted on y-axis.
Fixed variable is fixed and unchanged throughout the experiment.
Inference: state the relationship between two VISIBLE QUANTITIES in a diagram or picture.
Hypothesis: state the relation ship between two MEASURABLE VARIABLES that can be investigated in a lab.
How to tabulate data?
-the name or the symbols of the variables must be labelled with respective units.
-all measurements must be consistent with the sensitivity of the instruments used.
-all the calculated values must be correct.
-all the values must be consistent to the same number of decimal places.
A graph is cosidered well-plotted if it contains the following:
- a title to shoe the two variables and investigation.
- two axes labelled with correct variables and units
- scales must be chosen carefully and graph must occupy more than 50% of the graph paper.
-all the points are correctly drawn.
-the best line is drawn.
Understanding the Physics (and Errors) of the Measurement
| | 0 Comments »Understanding the Physics (and Errors) of the Measurement
Don't let the title put you off, it's pretty basic. The amount of light scattered back to the OTDR for measurement is quite small, about one-millionth of what is in the test pulse, and it is not necessarily constant. This affects the operation and accuracy of OTDR measurements.
Overload Recovery
Since so little of the light comes back to the OTDR for analysis, the OTDR receiver circuit must be very sensitive. That means that big reflections, which may be one percent of the outgoing signal, will saturate the receiver, or overload it. Once saturated, the receiver requires some time to recover, and until it does, the trace is unreliable for measurement as shown in Figure 5.
The most common place you see this as a problem is caused by the connector on the OTDR itself. The reflection causes an overload which can take the equivalent of 50 meters to one kilometre (170 to 3280 feet) to recover fully, depending on the OTDR design, wavelength and magnitude of the reflection. It is usually called the "Dead Zone". For this reason, most OTDR manuals suggest using a "pulse suppressor" cable, which doesn't suppress pulses, but simply gives the OTDR time to recuperate before you start looking at the fibre in the cable plant you want to test. They should be called "launch" cables.
Figure 5. OTDR launch pulse and launch cable
Ghosts
If you are testing short cables with highly reflective connectors, you will likely encounter "ghosts" like in Figure 6. These are caused by the reflected light from the far end connector reflecting back and forth in the fibre until it is attenuated to the noise level. Ghosts are very confusing, as they seem to be real reflective events like connectors, but will not show any loss. If you find a reflective event in the trace at a point where there is not supposed to be any connection, but the connection from the launch cable to the cable under test is highly reflective, look for ghosts at multiples of the length of the launch cable or the first cable you test. You can eliminate ghosts by reducing the reflections, using a trick we will share later.
Figure 6. OTDR "Ghosts"
Backscatter Variability Errors
Another problem that occurs is a function of the backscatter coefficient, a big term which simply means the amount of light from the outgoing test pulse that is scattered back toward the OTDR. The OTDR looks at the returning signal and calculates loss based on the declining amount of light it sees coming back.
Only about one-millionth of the light is scattered back for measurement, and that amount is not a constant. The backscattered light is a function of the attenuation of the fibre and the diameter of the core of the fibre. Higher attenuation fibre has more attenuation because the glass in it scatters more light. If you look at two different fibres connected together in an OTDR and try to measure splice or connector loss, you have a major source of error, the difference in backscattering from each fibre.
To more easily understand this problem, consider Figure 7 showing two fibres connected. If both fibres are identical, such as splicing a broken fibre back together, the backscattering will be the same on both sides of the joint, so the OTDR will measure the actual splice loss.
Figure 7. Loss errors in OTDR measurements
Looking the opposite way, from a low loss fibre to a high loss fibre, we find the backscatter goes up, making the measured loss less than it actually is. In fact, this often shows a "gainer", a major confusion to new OTDR users.
The difference in backscatter can be a major source of error. A difference in attenuation of 0.1 dB per km in the two fibres can lead to a splice loss error of 0.25 dB! While this error source is always present, it can be practically eliminated by taking readings both ways and averaging the measurements, and many OTDRs have this programmed in their measurement routines. This is the only way to test in line splices for loss and get accurate results.
Another common error can come from backscatter changes caused by variations in fibre diameter. A variation in diameter of 1% can cause a 0.1 dB variation in backscatter. This can cause tapered fibres to show higher attenuation in one direction, or we have in the past seen fibre with "waves" in the OTDR trace caused by manufacturing variations in the fibre diameter.
Overcoming Backscatter Errors
One can overcome these variations in backscatter by measuring with the OTDR in both directions and averaging the losses. The errors in each direction cancel out, and the average value is close to the true value of the splice or connector loss. Although this invalidates the main selling point of the OTDR, that it can measure fibre from only one end, you can't change the laws of physics.
Resolution Limitations
The next thing you must understand is OTDR resolution. The OTDR test pulse, Figure 8, has a long length in the fibre, typically 5 to 500 meters long (17 to 1700 feet). It cannot see features in the cable plant closer together than that, since the pulse will be going through both simultaneously. This has always been a problem with LANs or any cable plant with patchcords, as they disappear into the OTDR resolution. Thus two events close together can be measured as a single event, for example a connector that has a high loss stress bend near it will show up on the OTDR as one event with a total loss of both events. While it may lead you to think the connector is bad and try to replace it, the actual problem will remain.
Another place this problem shows up is in splice closures. An OTDR may show a bad splice, but it can actually be a crack or stress point somewhere else in the splice closure.
There is a tool that will help here. It is called a "visual fault locator". It injects a bright red laser light into the fibre to find faults. If there is a high loss, such as a bad splice, connector or tight bend stressing the fibre, the light lost may be visible to the naked eye. This will find events close to the OTDR or close to another event that are not resolvable to the OTDR. It's limitation is distance too, it only works over a range of about 2.5 miles or 4 km.
The visual fault locator is so valuable a tool that many OTDRs now have one built into them. If you are using an OTDR, you must have one to use it effectively.
Special Consideration for Multimode Fibre
Most OTDR measurements are made with singlemode fibre, since most outside plant cable is singlemode. But building and campus cabling are usually multimode fibre using light emitting diode sources for low and medium speed networks. The OTDR has problems with multimode fibre, since it uses a laser source to get the high power necessary to cause high enough backscatter levels to measure.
The laser light is transmitted by multimode fibre only in the centre of the core (Figure 9) because its emission angle is so low. LEDs, however, are transmitted throughout the core of the multimode fibre, due to their wider radiation pattern. As a result of the OTDR light being concentrated in the centre of the fibre, the loss of connectors is lower because the typical connector offset errors are not an effect. And even the fibre has lower loss, because the light in the centre of the core travels a shorter path than the light at the outer edges of the core.
Figure 9. OTDRs only see the middle of the multimode fibre core
Measuring Fibre, not Cable Distance
And finally, OTDRs measure fibre not cable length. While this may sound obvious, it causes a lot of problems in buried cable. You see, to prevent stress on the fibre, cable manufacturers put about 1% more fibre in the cable than the length of the cable itself, to allow for some "stretch." If you measure with the OTDR at 1000 metres (3300 feet), the actual cable length is about 990 metres (3270 feet). If you are looking for a spot where the rats chewed through your cable, you could be digging 10 metres (33 feet) from the actual location!
Understanding Scalar and Vector Quantities
| | 0 Comments »Understanding Derived and Base Quantities
| | 0 Comments »Understanding Derived and Base Quantities
Physical quantities are quantities that can be measured. e.g. Length, Temperature, Speed, Time.
Quantities or qualities that cannot be measured are not physical quantities. e.g. happiness, sadness etc.
Physical quantities can be divided into Base quantitied and Derived quantities.
(i) Physical quantities are quantities that can be measured or can be calculated.
(ii) The base quantities are “building block” quantities from which other quantities are derived from.
(iii) The base quantities and their S.I. units are:
- Base quantities S.I. units
- Mass kg
- Length m
- Time s
- Electric current A
- Thermodynamic
- temperature K
(iii) Derived quantities are quantities derived (iv) Examples of derived quantities.
- Derived quantities S.I. units
- area m2
- density kg m-3
- weight N
- velocity m s-1
Standard Notation: To express very large or very small numbers.
Example; A X 10 n (ten to the power of n), n must be an integer and 1 ≤ A <10
Understanding Physics
| | 0 Comments »Understanding Physics Text
Understanding Physics is built on the foundations of the 6th Edition of Halliday, Resnick, and Walker's Fundamentals of Physics which we often refer to as HRW 6th. The Following Description is Exerpted from the Preface:Why a Revised Text?
A physics major recently remarked that after struggling through the first half of his junior level mechanics course, he felt that the course was now going much better. What had changed? Did he have a better background in the material they were covering now? "No," he responded. "I started reading the book before every class. That helps me a lot. I wish I had done it in Physics One and Two." Clearly, this student learned something very important. It is something most physics instructors wish they could teach all of their students as soon as possible. Namely, no matter how smart your students are, no matter how well your introductory courses are designed and taught, your students will master more physics if they learn how to read an "understandable" textbook carefully.
We know from surveys that the vast majority of introductory physics students do not read their textbook carefully.We think there are two major reasons why: (1) many students complain that physics textbooks are impossible to understand and too abstract, and (2) students are extremely busy juggling their academic work, jobs, personal obligations, social lives and interests. So, they develop strategies for passing physics without spending time on careful reading.We address both of these reasons by making our revision to the sixth edition of Fundamentals of Physics easier for students to understand and by providing you as an instructor with more Reading Exercises (formerly known as Checkpoints) and additional strategies for encouraging students to read the text carefully. Fortunately, we are attempting to improve a fine textbook whose active author, Jearl Walker, has worked diligently to make each new edition more engaging and understandable.
In the next few sections we provide a summary of how we are building upon HRW 6th and shaping it into this new textbook.
A Narrative That Supports Student Learning
One of our primary goals is to help students make sense of the physics they are learning. We cannot achieve this goal if students see physics as a set of disconnected mathematical equations that each describe only to a small number of specific situations.We stress conceptual and qualitative understanding and continually make connections between mathematical equations and conceptual ideas.We also try to build on ideas that student can be expected to already understand, based on the resources they bring from their everyday experiences.
In Understanding Physics we have tried to tell a story that flows from one chapter to the next. Each chapter begins with an introductory section that discusses why new topics introduced in the chapter are important and explains how the chapter builds on previous chapters and prepares students for those that follow. We place explicit emphasis on basic concepts that recur throughout the book.We use extensive forward and backward referencing to reinforce connections between topics. For example, in the introduction of Chapter 16 on Oscillations we state: "Although your study of simple harmonic motion will enhance your understanding of mechanical systems it is also vital to understanding the topics in electricity, magnetism, and light encountered in Chapters 30-37. Finally, a knowledge of SHM provides a basis for understanding the wave nature of light and how atoms and nuclei absorb and emit energy."
Emphasis on Observation and Experimentation
Observations and concrete, everyday experiences are the starting points for development of mathematical expressions. Experiment-based theory building is a major feature of the book.We build ideas on experience that students either already have or can easily gain through careful observation.
Whenever possible, the physical concepts and theories developed in Understanding Physics grow out of simple observations or experimental data that can be obtained in typical introductory physics laboratories. We want our readers to develop the habit of asking themselves:What do our observations, experiences and data imply about the natural laws of physics? How do we know a given statement is true? Why do we believe we have developed correct models for the world?
Toward this end, the text often starts a chapter by describing everyday observations that students are familiar with. This makes Understanding Physics a text that is both relevant to student's everyday lives and draws on existing student knowledge. We try to follow Arnold Arons' principle "idea first, name after." That is, we make every attempt to begin a discussion by using everyday language to describe common experiences. Only then do we introduce formal physics terminology to represent the concepts being discussed. For example, everyday pushes, pulls, and their impact on the motion of an object are discussed before introducing the term "force" or Newton's second law.We discuss how a balloon shrivels when placed in a cold environment and how a pail of water cools to room temperature before introducing the ideal gas law or the concept of thermal energy transfer.
The "idea first, name after" philosophy helps build patterns of association between concepts students are trying to learn and knowledge they already have. It also helps students reinterpret their experiences in a way that is consistent with physical laws.
Examples and illustrations in Understanding Physics often present data from modern computer based laboratory tools. These tools include computer-assisted data acquisition systems and digital video analysis software.We introduce students to these tools at the end of Chapter 1. Examples of these techniques are shown in Figs. P-1 and P-2 at the right and Fig. P-3 below. Since many instructors use these computer tools in the laboratory or in lecture demonstrations, they are part of the introductory physics experience for more and more of our students. The use of real data has a number of advantages. It connects the text to the students' experience in other parts of the course and it connects the text directly to real world experience. Regardless of whether data acquisition and analysis tools are used in the student's own laboratory, our use of realistic rather that idealized data helps students develop an appreciation of the role that data evaluation and analysis plays in supporting theory.
FIGURE P-1 A video analysis shows that the center of mass of a two-puck system moves at a constant velocity.
FIGURE P-2 Electronic temperature sensors reveal that if equal amounts of hot and cold water mix the final temperature is the average of the initial temperatures.
Using Physics Education Research
In re-writing the text we have taken advantage of two valuable findings of physics education research. One is the identification of concepts that are especially difficult for many students to learn. The other is the identification of active learning strategies to help students develop a more comprehensive understanding of physics concepts.
Addressing Learning Difficulties
Extensive scholarly research exists on the difficulties students have in learning physics.1 We have made a concerted effort to address these difficulties. In Understanding Physics, issues that are known to confuse students are discussed with care. This is true even for topics like the nature of force and its effect on velocity and velocity changes that may seem trivial to professional physicists. We write about subtle, often counter-intuitive topics with carefully chosen language and examples designed to draw out and remediate common alternative student conceptions. For example, we know that students have trouble understanding passive forces such as normal and friction forces.2 How can a rigid table exert a force on a book that rests on it? In Section 6-4 we present an idealized model of a solid that is analogous to an inner spring mattress with the repulsion forces between atoms acting as the springs. In addition, we invite our readers to push on a table with a finger and experience the fact that as they push harder on the table the table pushes harder on them in the opposite direction.
Incorporating Active Learning Opportunities
We designed Understanding Physics to be more interactive and to foster thoughtful reading.We have retained a number of the excellent Checkpoint questions found at the end of HRW 6th chapter sections (which we now call Reading Exercises). We have created many new Reading Exercises that require students to reflect on the material in important chapter sections. For example, just after reading Section 6-2 that introduces the two-dimensional free-body diagram, students encounter Reading Exercise 6-1. This multiple-choice exercise requires students to identify the free-body diagram for a helicopter that experiences three non-collinear forces. The distractors were based on common problems student have with the construction of free-body diagrams. When used in "Just-In-Time Teaching" assignments or for in-class group discussion, this type of reading exercise can help students learn a vital problem solving skill as they read.
FIGURE P-3 A video analysis of human motion reveals that in free fall the center of mass of an extended body moves in a parabolic path under the influence of the Earth's gravitational force.
FIGURE P-4 Compressing an innerspring mattress with a force.The mattress exerts an oppositely directed force, with the same magnitude, back on the finger.
We also created a set of Touchstone Examples. These are carefully chosen sample problems that illustrate key problem solving skills and help students learn how to use physical reasoning and concepts as an essential part of problem solving. We selected some of these touchstone examples from the outstanding collection of sample problems in HRW 6th, and we created some new ones. In order to retain the flow of the narrative portions of each chapter, we have reduced the overall number of sample problems to those necessary to exemplify the application of fundamental principles.Also, we chose touchstone examples that require students to combine conceptual reasoning with mathematical problem solving skills. Few, if any, of our touchstone examples are solvable using simple "plug-and-chug" or algorithmic pattern matching techniques.
Alternative problems have been added to the extensive, classroom tested endof- chapter problem sets selected from HRW 6th. The design of these new problems are based on the authors' knowledge of research on student learning difficulties. Many of these new problems require careful qualitative reasoning, that explicitly connect conceptual understanding to quantitative problem solving. In addition, estimation problems, video analysis problems, and "real life" or "context rich" problems have been included. The organization and style of Understanding Physics has been modified so that it can be easily used with other research based curricular materials that make up what we call The Physics Suite. The Suite and its contents are explained at more length at the end of this preface.
Reorganizing for Coherence and Clarity
For the most part we have retained the organization scheme inherited from HRW 6th. Instructors are used to the general organization and topics that are treated in a typical course sequence in calculus-based introductory physics. In fact, ordering of topics and their division into chapters is the same for 27 of the 38 chapters. The order of some topics has been modified to be more pedagogically coherent. Most of the reorganization was done in Chapters 3 through 10 where we adopted a sequence known as New Mechanics. In addition, we decided to move HRW 6th Chapter 25 on capacitors so it becomes the last chapter on electricity. Capacitors are now introduced in Chapter 28 in Understanding Physics.
The New Mechanics Sequence
HRW 6th and most other introductory textbooks use a similar sequence in the treatment of classical mechanics. It starts with the development of the kinematic equations to describe constantly accelerated motion. Then two-dimensional vectors and the kinematics of projectile motion are treated. This is followed by the treatment of dynamics in which Newton's Laws are presented and used to help students understand both one- and two-dimensional motions. Finally energy, momentum conservation, and rotational motion are treated.
About 12 years ago when Priscilla Laws, Ron Thornton, and David Sokoloff were collaborating on the development of research-based curricular materials, they became concerned about the difficulties students had working with two-dimensional vectors and understanding projectile motion before studying dynamics.
At the same time Arnold Arons was advocating the introduction of the concept of momentum before energy.3 Arons argued that (1) the momentum concept is simpler than the energy concept, in both historical and modern contexts and (2) the study of momentum conservation entails development of the concept of center-of-mass which is needed for a proper development of energy concepts.
In order to address these concerns about the traditional mechanics sequence a small group of physics education researchers and curriculum developers convened in 1992 to discuss the introduction of a new order for mechanics.4 One result of the conference was that Laws, Sokoloff, and Thornton have successfully incorporated a new sequence of topics in the mechanics portions of various curricular materials that are part of the Physics Suite discussed below.5 These materials include Workshop Physics, the RealTime Physics Laboratory Module in Mechanics, and the Interactive Lecture Demonstrations.This sequence is incorporated in this book and has required a signifi- cant reorganization and revisions of HRW 6th Chapters 2 through 10.
The New Mechanics sequence incorporated into Chapters 2 through 10 of understanding physics includes:
Just-in-Time Mathematics In general, we introduce mathematical topics in a "just-in-time" fashion. For example, we treat one-dimensional vector concepts in Chapter 2 along with the development of one-dimensional velocity and acceleration concepts.We hold the introduction of twoand three-dimensional vectors, vector addition and decomposition until Chapter 4, immediately before students are introduced to two-dimensional motion and forces in Chapters 5 and 6.We do not present vector products until they are needed.We wait to introduce the dot product until Chapter 9 when concept of physical work is presented. Similarly, the cross product is first presented in Chapter 11 in association with the treatment of torque. Notation Changes Mathematical notation is often confusing, and ambiguity in the meaning of a mathematical symbol can prevent a student from understanding an important relationship. It is also difficult to solve problems when the symbols used to represent different quantities are not distinctive. Some key features of the new notation include: 1 L. C. McDermott and E. F. Redish, "Resource Letter PER-1: Physics Education Research," Am. J. Phys. 67, 755-767 (1999) 2 John J. Clement, "Expert novice similarities and instruction using analogies," Int. J. Sci. Ed. 20, 1271-1286 (1998) 3 Private Communication between Arnold Arons and Priscilla Laws by means of a document entitled "Preliminary Notes and Suggestions,"August 19, 1990; and Arnold Arons, Development of Concepts of Physics (Addison-Wesley, Reading MA, 1965) 4 The New Mechanics Conference was held August 6-7, 1992 at Tufts University. It was attended by Pat Cooney, Dewey Dykstra, David Hammer, David Hestenes, Priscilla Laws, Suzanne Lea, Lillian McDermott, Robert Morse, Hans Pfister, Edward F. Redish, David Sokoloff, and Ronald Thornton. 5 Laws, P.W. "A New Order for Mechanics" pp. 125-136, Proceedings of the Conference on the Introductory Physics Course, Rennselaer Polytechnic Institute, Troy New York, May 20-23, Jack Wilson, Ed. 1993 (John Wiley & Sons, New York 1997) |
Understanding Physics
| | 0 Comments »I currently only have a skeleton of a book completed. The book is unstructured because it is a work in progress. I will be adding bits and pieces as I find time and motivation to write on a topic. With time it will eventually come together into a complete book.
My thinking is to test the waters by putting the bait out and see if the fish bite. My motivation to complete more chapters depends mostly on the feedback I receive from you. Email me your suggestions on which topics trouble you the most in Physics.
Power, Energy and Efficiency
| | 0 Comments » Work
1. Everyday we move or certain object to do work.
2. work is done when a force is exerted to move an object through a distance in the direction of the force.
3. Work W is defined as product of the force and the displacement of an object in the direction of the force.
Work=Fs
Where,
F= the force acting
S= the displacement (or distance traveled in the direction of the force)
4 .Work is a scalar quantity and its unit is joule (J) or N m. 1 joule =1nm
Example:
A block which is at rest is acted on by force of magnitude 3 N in different direction. Determine the wok done by the block in each case.
a) The force act from the left, the object move to the right for 2 m.
b) The force act from the right, the object to the left for 2 m.
Solution
a) F=3 N b) F= -3 N
moving to the right for 2 m moving to the left for2 m (negative
Work done,W= Fs sign indicates object move to the left)
=3 N x (-2 m) Work done W = Fs
=6 Nm = -3 N x (-2m)
=6 Nm
5 .1 joule is the work done when a force of 1newton moves of an object for 1 m in the direction of the force .
6 .Work is not done when a force is exerted on an object but the object does not move.
7 .In short, work is not done :
a) The direction of motion is perpendicular to the direction of the force exerted
b) Force is exerted on the object but the object does not move.
Energy
1. We need energy to do work.
2. Energy is defined as the Potential or the ability to do work.
3. Energy is scalar quantity and its unit is the joule (J) or N m.
4. Energy can exist in various form. Examples potential energy, kinetic energy, heat energy, electrical energy and sound energy.
5. Energy cannot be created or destroyed. The work done related to the change of the form of the energy.
Example
A student of mass 50 kg walks up a flight of stairs 1.5 m high. What is…
a) the work done by the student?
Work = Fx s
=mg x s
=(50 x 10) N x 1.5 m
=750 J
b) energy needed = work done
=750 J
Work and Energy
| | 0 Comments »
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Work-Energy PrincipleThe change in the kinetic energy of an object is equal to the net work done on the object.This fact is referred to as the Work-Energy Principle and is often a very useful tool in mechanics problem solving. It is derivable from conservation of energy and the application of the relationships for work and energy, so it is not independent of the conservation laws. It is in fact a specific application of conservation of energy. However, there are so many mechanical problems which are solved efficiently by applying this principle that it merits separate attention as a working principle.For a straight-line collision, the net work done is equal to the average force of impact times the distance traveled during the impact. Average impact force x distance traveled = change in kinetic energyIf a moving object is stopped by a collision, extending the stopping distance will reduce the average impact force.
The rate of doing work is equal to the rate of using energy since the a force transfers one unit of energy when it does one unit of work. A horsepower is equal to 550 ft |
Understanding Elasticity
| | 0 Comments »Understanding Elasticity
Elasticity is the ability of a material to return to its original shape and size when the external force acting on it is removed.
It is due to the strong intermolecular forces between the molecules of the solid.
(you have to be able to explain elasticity in terms of intermolecular forces)
Hooke’s Law States that the extension of a spring is directly proportional to the applied force provided that the elastic limit is not exceeded.
Elastic limit of a spring is the maximum force that can be applied to a spring such that the spring will be able to be restored to its original length when the force is removed.
If the elastic limit is exceeded, the length of the spring is longer than the original length even though the force no longer acts on it. It is said to have permanent extension.
Hooke's law Graph
Force Vs Extension
k = force constant of the spring (equal of the gradient of the graph)
x = extension
Force constant is the force that is required to produce one unit of extension of the spring.It is the measure of the stiffness of the spring.
The curve at the end occurs represents the moment before the material breaks.
Factors influencing the elasticity of a spring:
a. Type of spring material
b. diameter of the coil of spring
c. diameter of the wire of spring
d. arrangement of the spring.
Point 1 is the Limit of Proportionality. Point 2 is the Elastic Limit. Point 3 is the Yield Point.
Before the limit of proportionality, the material obeys Hooke’s Law. After it, Force is no longer proportional to extension, and the graph begins to curve.
The Elastic Limit is the point when a material stops behaving elastically, and starts behaving plastically. The area before this point is called the elastic region; after it, the plastic region.
The Yield Point is the point where the material starts to stretch without applying any additional force.
Elastic Potential Energy, U
Elastic potential energy is the energy transferred to the spring when work is done on the spring.
k = force constant
x = spring extension
Source: http://stuffaboutphysics.wordpress.com/2009/01/11/forceextension-graphs/
Impulse and Impulsive force
| | 0 Comments »Impulse and impulsive Force
1. Impulse is defined as the change momentum
2. From F=ma
Ft=mv-mu (change of momentum)
3. Impulse is the product of the force F acting on a body and the time t for which the force acts.
Hence, impulse = Ft = mv – mu
4. The SI unit of impulse is kg m s⁻1 or N s.
5. Impulsive force is the rate of change of momentum.
Impulsive force = Impulse / time
6. The SI unit of impulse is kg m s⁻² or N.
The Effect of Time on an impulsive Force
1. From the formula for impulsive force, we get
Ft = mv – mu
F = (mv - mu) / t
This shows that the time of action is very important factor in the calculation of the impulsive force.
2.When the time of action is prolonged, the impulsive force will decrease.
3. On the other hand, if the time of action is shortened, the impulsive force will increase.
Ways to Reduce Impulsive Forces
The Design of a car
1. A car is mainly designed for the safety of the driver.
2. The front and the rear parts of the car are made of soft metal so that the car is easily crumpled during an accident.
a) During collision, the time taken for the change in speed (from a high speed to zero) is prolonged. Since the impulsive force
= Distance / Time , the force will decrease when the time increase.
b) This will decrease the impulsive force on the passengers and the driver.
3. The seats of the passengers are strengthened to protect the passengers.
4. Safety belts:
a) Passengers have to fasten the safety belts. When the car stops suddenly, the inertia of the passengers will result in the passengers being flung to the front and hitting the windscreen of the car.
b) Hence, safety belts will slow down the motion of the passengers.
5. Airbags are built in some cars. When an accident happens, the airbags will be filled with air. This will prolong the time of action and reduce the impulsive force on the passenger.
Ways to utilize impulsive force
Material arts player break a few pieces of bricks
- A martial arts player ia able to break a pile of bricks with ease.
- This is because the hand of the player moves very fast and stops when it hits the top brick.
- Hence, the time of contact of the hand with the brick is short and this will increase the impulsive force on the bricks.
- The bricks are easily broken because of the big impulsive force.
The pestle and mortar
- The pestle and mortar are made of hard materials.
- During pounding or grinding, the pestle moves very fast. The mortar stops the motion of the pestle in a short time.
- A strong impulsive force is produced and the food can be broken into pieces easily.
The pile and the pile driver
- A pile driver is made of hard steel alloy.
- The pile driver is released very fast hit the hard pile.
- The time taken to hit the pile is short because both surfaces are hard.
- Hence, a big impulsive force is produced on the pile and it will be driven into the ground to support the foundation of the structure of a tall building.
Analysing Momentum II
| | 0 Comments »Conservation of Momentum
1. The term conservation is derived from the root word “conserve” which means constant.
2. The principle of conservation of momentum states that in the absence of an external force, the total momentum of a system remains unchanged.
3. An example of external force is friction and this can be contact friction or air friction.
4. An isolated or closed system the sum of external forces is zero, thus, the principle of conservation of momentum is true for a closed system.
Collisions
1. There are two types of collision:
(a) Elastic collision
(b) Inelastic collisions
2. In Elastic collision: Two objects collide and move apart again after a collision. Momentum is conserved. Total energy is conserved. Kinetic energy is conserved.
Formula: m1u1+m2u2 = m1v1+m2v2
3. In Inelastic collision: Two objects combine and stop or move together with a same velocity after a collision. Momentum is conserved. Total energy is conserved. Kinetic energy is not conserved (the total kinetic energy after the collision is less than the total kinetic energy before collision, excess energy is released as heat, sound energy etc).
Formula: m1u1+m2u2 = (m1+m2)v
Analysing Momentum
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(1000kg)(20m/s)=20,000Ns
the momentum of Car S is
(1200kg)(-10m/s)=-12,000Ns (but in the opposite direction of R so we will call this direction negative)
take the sum of the two momenta to get 8,000Ns
the new momentum is 8,000Ns and the mass of the system is 2200kg. so plug this into the momentum equation
p=mv
8000Ns=(2200kg)(v)
v=3.636m/s
Understanding Inertia
| | 0 Comments »Understanding inertia
Newtons Three Laws of Motion
| | 1 Comment »Let us begin our explanation of how Newton changed our understanding of the Universe by enumerating his Three Laws of Motion.
Newton's First Law of Motion:
I. Every object in a state of uniform motion tends to remain in that state of motion unless an external force is applied to it. |
Newton's Second Law of Motion:
II. The relationship between an object's mass m, its acceleration a, and the applied force F is F = ma. Acceleration and force are vectors (as indicated by their symbols being displayed in slant bold font); in this law the direction of the force vector is the same as the direction of the acceleration vector. |
This is sometimes summarized by saying that under Newton, F = ma, but under Aristotle F = mv, where v is the velocity. Thus, according to Aristotle there is only a velocity if there is a force, but according to Newton an object with a certain velocity maintains that velocity unless a force acts on it to cause an acceleration (that is, a change in the velocity). As we have noted earlier in conjunction with the discussion of Galileo, Aristotle's view seems to be more in accord with common sense, but that is because of a failure to appreciate the role played by frictional forces. Once account is taken of all forces acting in a given situation it is the dynamics of Galileo and Newton, not of Aristotle, that are found to be in accord with the observations.
Newton's Third Law of Motion:
III. For every action there is an equal and opposite reaction. |
Distance, Displacement, Speed, Velocity, and Acceleration Review?
| | 0 Comments »Distance, Displacement, Speed, Velocity, and Acceleration Review?
--------------------------------------…
What was his average velocity for the entire trip?
4 miles/hour
54 miles/hour, West\
3 miles/hour, West
\0.05 miles/minute, West
33 miles/hour
5 miles/hour, West
1 mile/hour, East
5 miles/hour
1 mile/hour
5. Sometimes the numerical part of an acceleration is given as a negative number. How is a negative acceleration different from a positive acceleration?
6. Is the object accelerating in the following example? Choose yes or no and an explanation.
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A motorcycle speeds up from rest.
yes
yes, decrease in velocity
change in direction
no
increase in velocity
no, no change in direction or velocity
decrease in velocity
yes, increase in velocity
yes, change in direction
7. Is the object accelerating in the following example? Choose yes or no and an explanation.
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A car slows to a stop for a red light.
yes
yes, decrease in velocity
change in direction
no
increase in velocity
no, no change in direction or velocity
decrease in velocity
yes, increase in velocity
yes, change in direction
8. Is the object accelerating in the following example? Choose yes or no and an explanation.
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A boat cruises in a straight line at 30 knots.
yes
yes, decrease in velocity
change in direction
no
increase in velocity
no, no change in direction or velocity
decrease in velocity
yes, increase in velocity
yes, change in direction
9. Is the object accelerating in the following example? Choose yes or no and an explanation.
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A boat, still traveling at 30 knots, turns around and heads back.
yes
yes, decrease in velocity
change in direction
no
increase in velocity
no, no change in direction or velocity
decrease in velocity
yes, increase in velocity
yes, change in direction
10. A descendant of Galileo drops a bowling ball, baseball, and crow's wing feather from the top of the Leaning Tower of Pisa.
Tell which of the objects hits first, second, and third.
Explain your answer.
11. A car is traveling along at 50 mph, according to the speedometer. Thelma is driving and Louise is in the passenger's seat.
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What is Louise's speed from Thelma's point of view (frame of reference)?
50 miles/hour
not enough information to tell
over 100 miles/hour
0 miles/hour
100 miles/hour
between 0 miles/hour and 50 miles/hour
between 50 miles/hour and 100 miles/hour
12. Explain your answer to question #11.
13. A car is traveling along at 50 mph, according to the speedometer. Thelma is driving and Louise is in the passenger's seat.
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Wayne is standing at the curb as the car passes him. What is Louise's speed from Wayne's frame of reference?
not enough information to tell
between 50 mph and 100 mph
100 mph
50 mph
between 0 mph and 50 mph
over 100 mph
0 mph
14. Explain your answer to #13.
15. A car is traveling along at 50 mph, according to the speedometer. Thelma is driving and Louise is in the passenger's seat.
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A police helicopter is hovering directly over the car as it moves along. What is Louise's speed from the pilot's frame of reference?
over 100 mph
between 0 mph and 50 mph
not enough information to tell
50 mph100 mph
between 50 mph and 100 mph
0 mph
16. Explain your answer in #15.
I know its alot I know i should do this myself Ireally need help badly my mom or myself cannot get the answers HELP ME PLEASE!!!!!!!!!!!! I AM BEGGING YOU PLEASE
Analysing Linear Motion
| | 0 Comments »This lab measures the linear motion of a cart on an air track with a motion sensor. In the first experiment the air track was level. Two data plots were taken of this motion and stored in the Logger Pro program for analysis using the supplied data table. The track was tilted in the second experiment. Three data plots were taken of the motion and stored in Logger Pro. Some of the graphs created by the data in Logger Pro will appear later in this analysis.
Analysis of the motion along the air track helps the beginning physics student understand motion in both the horizontal and vertical direction. Slanting the air track at a slight angle allows for the easy calculation of the cart acceleration and allows the student to see how the acceleration affects the cart along the horizontal plane. This lab reinforces the use of derivatives and integration to understand the relationship between distance, velocity and acceleration.
The first part of the experiment required the cart to be accelerated along the air track by hand while the sensor collected the data in the Logger Pro program. Two experiments were done with the data collected and saved in the program. The second part of the experiment required the track to be tilted and three experiments done with the data saved in the Logger Pro program. The data was analyzed according to the instructions and put in the data table which appears at the end of this report. During the analysis fourteen questions were asked while compiling the data for the table. The answers to these questions are the basis for the results of this analysis.
A: Distance vs. Time
5. Evaluate the derivative at tmax. What does this value represent?
B: Velocity vs time
Yes! The mean value is the same average velocity derived from part one using the slope of the distance vs. time curve.
7. Find the area under the velocity vs. time curve. What does this represent? Is it a reasonable value?
A. When you integrate (v dt) it gives the distance value back. As shown in the distance vs time data table the distance traveled by the cart was 0.314 m. The integral given in the velocity vs. time chart indicates 0.313 m. The difference is most likely from the program rounding in different graphs and tables.
B. Yes. This represents the distance traveled over the 1.2 seconds the integral was evaluated at that average velocity.
B. Yes
A: Distance vs time
t = .75 s
This derivative gives the velocity of the cart as it slides down the air track. Note that the velocity is negative (-0.321 m/s) indicating the cart is sliding down the track.
This is the acceleration over t = 0.75 s.
Part II
B: Velocity vs time
a. This derivative represents the acceleration of the cart as it slides down the air track.
b. Yes, although it seems to be slightly low at 0.77 m/s2 for a six degree angle.
a. The integral of the velocity equation returns the distance traveled by the cart or 0.599 m.
b. Yes-This is the distance traveled over the 0.75 seconds along the track.
Part II
C: Acceleration vs time
a. The integration of the acceleration returns the velocity of the cart over the selected time span of 0.75 seconds.
b. Yes.
3. Integrating the values gives the area under the acceleration curve which equates to the distance traveled for the cart over a set time period.
Agreement between theoretical and experimental values:
In this experiment the sin of was given as 0.10452 or six degrees. The acceleration values for this angle should approach approximately 1 m/s2, but only reach values between 0.827 to 0.835 m/s2. These values are off by approximately 18%, leading me to believe that the person responsible for measuring the angle did not accurately measure it. The angle was given as ± one degree. At minus one degree the angle does approach the values given by analysis of the graphs. This certainly would account for the uncertainty of the theoretical value.
Other areas of decreasing acceleration values could be some slight air resistance by the sail attached to the cart, although it is expected that value would be minimal over the short distance traveled by the cart. There was a lot of trouble getting the sensor to work properly in these experiments. This will surely induce error into the values derived by the sensor data and the motion recorded by the sensor.
Overall the experimental values given by the sensor and Logger Pro graph analysis are consistent with the expected distance, velocity and accelerations values.
Bernoulli's Principle Applied to Fluid Flow in Tubes
| | 0 Comments »For instance, if you were standing at the top of a building holding a baseball over the side, the ball would have a certain quantity of potential energy—the energy that an object possesses by virtue of its position. Once the ball is dropped, it immediately begins losing potential energy and gaining kinetic energy—the energy that an object possesses by virtue of its motion. Since the total energy must remain constant, potential and kinetic energy have an inverse relationship: as the value of one variable decreases, that of the other increases in exact proportion.
The ball cannot keep falling forever, losing potential energy and gaining kinetic energy. In fact, it can never gain an amount of kinetic energy greater than the potential energy it possessed in the first place. At the moment before the ball hits the ground, its kinetic energy is equal to the potential energy it possessed at the top of the building. Correspondingly, its potential energy is zero—the same amount of kinetic energy it possessed before it was dropped.
Then, as the ball hits the ground, the energy is dispersed. Most of it goes into the ground, and depending on the rigidity of the ball and the ground, this energy may cause the ball to bounce. Some of the energy may appear in the form of sound, produced as the ball hits bottom, and some will manifest as heat. The total energy, however, will not be lost: it will simply have changed form.
Bernoulli was one of the first scientists to propose what is known as the kinetic theory of gases: that gas, like all matter, is composed of tiny molecules in constant motion. In the 1730s, he conducted experiments in the conservation of energy using liquids, observing how water flows through pipes of varying diameter. In a segment of pipe with a relatively large diameter, he observed, water flowed slowly, but as it entered a segment of smaller diameter, its speed increased.
It was clear that some force had to be acting on the water to increase its speed. Earlier, Robert Boyle (1627-1691) had demonstrated that pressure and volume have an inverse relationship, and Bernoulli seems to have applied Boyle's findings to the present situation. Clearly the volume of water flowing through the narrower pipe at any given moment was less than that flowing through the wider one. This suggested, according to Boyle's law, that the pressure in the wider pipe must be greater.
As fluid moves from a wider pipe to a narrower one, the volume of that fluid that moves a given distance in a given time period does not change. But since the width of the narrower pipe is smaller, the fluid must move faster in order to achieve that result. One way to illustrate this is to observe the behavior of a river: in a wide, unconstricted region, it flows slowly, but if its flow is narrowed by canyon walls (for instance), then it speeds up dramatically.
The above is a result of the fact that water is a fluid, and having the characteristics of a fluid, it adjusts its shape to fit that of its container or other solid objects it encounters on its path. Since the volume passing through a given length of pipe during a given period of time will be the same, there must be a decrease in pressure. Hence Bernoulli's conclusion: the slower the rate of flow, the higher the pressure, and the faster the rate of flow, the lower the pressure.
Bernoulli published the results of his work in Hydrodynamica (1738), but did not present his ideas or their implications clearly. Later, his friend the German mathematician Leonhard Euler (1707-1783) generalized his findings in the statement known today as Bernoulli's principle.
Read more: http://www.scienceclarified.com/everyday/Real-Life-Chemistry-Vol-3-Physics-Vol-1/Bernoulli-s-Principle.html#ixzz18Cxh5dIT
Understanding Bernoulli's Principle
| | 0 Comments »Airplanes get a part of their lift by taking advantage of Bernoulli's principle. Race cars employ Bernoulli's principle to keep their rear wheels on the ground while traveling at high speeds.
The Continuity Equation relates the speed of a fluid moving through a pipe to the cross sectional area of the pipe. It says that as a radius of the pipe decreases the speed of fluid flow must increase and visa-versa. This interactive tool lets you explore this principle of fluids. You can change the diameter of the red section of the pipe by dragging the top red edge up or down.
The main point of the theory is that square of displacement r2 of Brownian particle from initial position, averaged by many Brownian particles, changes proportionally to time (diffusion law): r2 = D * T. Coefficient of diffusion D is proportional to the absolute temperature T. Einstein's theory was experimentally proven in experiments of French physicist G. Perrene (1908).
Application of Archimedes' Principle
| | 0 Comments »Archimedes PrincipleTake a spring balance, a piece of stone, a measuring cylinder and water. Measure the weight of stone in air by tying the string around in a loop, and hanging it from the spring balance. Take water in a measuring cylinder and note its volume level. Then dip the stone in the water while it is still hanging from the spring balance. You will see that the stone is weighing less!! If you see the water level now, you will see it has risen. Now from the volume of the water displaced, calculate the weight of water from the following equation for density : Mass of water (in gm) Density of water is 1 gm/cm3. You will see that the mass of water displaced is exactly equal to the reduction in weight of the stone in water.Density of water = Volume of water (in cubic cm) |
Consider the figure alongside, here a square piece of iron is immersed in liquid. The piece of iron is experiencing forces from all sides and they are:
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H=0 and
3. Application of Archimedes’ Principle to determine densities of liquids
Density of substance Density of water Density of water is 1 gm/cm3. (Density changes with temperature; density of water is 1 gm/cm3 at 4oC. It is taken as the same at all temperatures unless the temperatures are close to 0oC or 100oC , where water changes to ice or steam respectively) To determine the density of an unknown liquid by Archimedes’ method, please do the following :
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R. D = X
Volume of the displaced liquid Weight of the water displaced
(W1 - W2 )