Q.2 In vertical circular motion, the ratio of kinetic energy of a particle at highest point to that at lowest point is (A) 5 (B) 2 (C) 0.5 (D) 0.
|
|
- Baldric Kelley
- 7 years ago
- Views:
Transcription
1
2 Physics R Q. Fo a gas 0.4, whee R is the univesal gas constant and 'C v ' is mola specific heat at C v constant volume. The gas is made up of molecules which ae (A) Rigid diatomic Monoatomic Non-igid diatomic Polyatomic Q. In vetical cicula motion, the atio of kinetic enegy of a paticle at highest point to that at lowest point is (A) Q. Two wies having same length and mateial ae stetched by same foce. Thei diametes ae in the atio :. The atio of stain enegy pe unit volume fo these two wies (smalle to lage diamete) when stetched is (A) : 9 : 7 : 8 : Q.4 A ing and a disc oll on the hoizontal suface without slipping with same linea velocity. If both have same mass and total kinetic enegy of the ing is 4 J then total kinetic enegy of the disc is (A) J 4 J 5 J 6 J Q.5 When the obseve moves towads the stationay souce with velocity, 'V ', the appaent fequency of emitted note is F. When the obseve moves away fom the souce with velocity 'V ', F V the appaent fequency is F. If V is the velocity of sound in ai and then? F V (A) 4 5
3 Q.6 Wie having tension 5 N poduces six beats pe second when it is tuned with a fok. When tension changes to 56 N, it is tuned with the same fok, the numbe of beats emain unchanged. The fequency of the fok will be (A) 86 Hz 5 Hz 56 Hz 80 Hz Q.7 Assuming the expession fo the pessue exeted by the gas on the walls of the containe, it can be shown that pessue is (A) d d th kinetic enegy pe unit volume of a gas kinetic enegy pe unit volume of a gas kinetic enegy pe unit volume of a gas 4 Kinetic enegy pe unit volume of a gas Q.8 A mass m connected to a hoizontal sping pefoms S.H.M. with amplitude A. While mass m is passing though mean position anothe mass m is placed on it so that both the masses move A togethe with amplitude A. The atio of A is (m m ) (A) m m m m m m m m m m m m
4 Q.9 A paticle moves along a cicle of adius with constant tangential acceleation. If the velocity of the paticle is at the end of second evolution, afte the evolution has stated then the tangential acceleation is (A) Q.0 Two stings A and B of same mateial ae stetched by same tension. The adius of the sting A is double the adius of sting B. Tansvese wave tavels on sting A with speed V and on sting B with speed V B. The atio V V A B is A (A) 4 4 Q. The bob of a simple pendulum pefoms S.H.M. with peiod T in ai and with peiod T in wate. Relation between T and T is (neglect fiction due to wate, density of the mateial of the bob is 9 0 kg / m, density of wate g ) 8 cc (A) T T T T T T T T
5 Q. In a capillay tube of adius R, a staight thin metal wie of adius (R > ) is inseted symmetically and one end of the combination is dipped vetically in wate such that the lowe end of the combination is at same level. The ise of wate in the capillay tube is [T = suface tension of wate, = density of wate, g = gavitational acceleation] T (A) (R ) g T (R ) g T (R ) g (R ) g T Q. When open pipe is closed fom one end then thid ovetone of closed pipe is highe in fequency by 50 Hz than second ovetone of open pipe. The fundamental fequency of open end pipe will be (A) 75 Hz 50 Hz 5 Hz 00 Hz Q.4 A disc of adius R and thickness R 6 has moment of inetia I about an axis passing though its cente and pependicula to its plane. Disc is melted and ecast into a solid sphee. The moment of inetia of a sphee about its diamete is (A) I 5 I 6 I I 64 Q.5 Let a steel ba of length l, beadth b and depth d be loaded at the cente by a load W. Then the sag of bending of beam is (Y = Young s modulus of mateial of steel) (A) Wl bd Y Wl 4bd Y Wl bd Y Wl 4bd Y 4
6 Q.6 Which of the following quantity does NOT change due to damping of oscillations? (A) Angula fequency Time peiod Initial phase Amplitude Q.7 If the end coection of an open pipe is 0.8 cm then the inne adius of that pipe will be (A) cm cm cm 0. cm Q.8 A pogessive wave is epesented by y = sin (5t 4x) cm. On this wave, how fa away ae the two points having phase diffeence of 90? (A) cm cm 4 cm 8 cm 6 Q.9 Two paticles of masses m and 9m ae sepaated by a distance. At a point on the line joining them the gavitational field is zeo. The gavitational potential at that point is (G = Univesal constant of gavitation) (A) 4Gm 8Gm 6Gm Gm 5
7 Q.0 A black ectangula suface of aea A emits enegy E pe second at 7 C. If length and beadth ae educed to becomes (A) 4E 9 7E 9 0E 9 6E 9 d of initial value and tempeatue is aised to 7 C then enegy emitted pe second Q. A liquid dop having suface enegy E is spead into 5 doplets of same size. The final suface enegy of the doplets is (A) E 4E 8E E Q. Let M be the mass and L be the length of a thin unifom od. In fist case, axis of otation is passing though cente and pependicula to the length of the od. In second case axis of otation is passing though one end and pependicula to the length of the od. The atio of adius of gyation in fist case to second case is (A) 4 8 Q. A simple pendulum of length l has maximum angula displacement. The maximum kinetic enegy of the bob of mass m is (g = acceleation due to gavity) (A) mgl ( cos ) mgl ( cos ) mgl ( cos ) mgl (cos ) 6
8 Q.4 Angula speed of hou hand of a clock in degee pe second is (A) Q.5 The value of gavitational acceleation g at a height h above the eath s suface is g 4 then (R = adius of eath) (A) h = R h R h R h R 4 Q.6 In potentiomete expeiment, null point is obtained at a paticula point fo a cell on potentiomete wie x cm long. If the length of the potentiomete wie is inceased without changing the cell, the balancing length will (Diving souce is not changed) (A) incease decease not change becomes zeo Q.7 An ion od is placed paallel to magnetic field of intensity 000 A m. The magnetic flux though the od is Wb and its coss-sectional aea is cm. The magnetic pemeability of the od in Wb is A m (A)
9 Q.8 Altenating cuent of peak value ampee flows though the pimay coil of the tansfome. The coefficient of mutual inductance between pimay and seconday coil is heny. The peak e.m.f. induced in seconday coil is (Fequency of a.c. = 50 Hz) (A) 00 V 00 V V Q.9 An electon of mass m has de-boglie wavelength when acceleated though potential diffeence V. When poton of mass M, is acceleated though potential diffeence 9V, the de-boglie wavelength associated with it will be (Assume that wavelength is detemined at low voltage) (A) M m M m m M m M Q.0 Intefeence finges ae poduced on a sceen by using two light souces of intensities I and 9I. The phase diffeence between the beams is at point P and at point Q on the sceen. The diffeence between the esultant intensities at point P and Q is (A) I 4 I 6 I 8 I Q. Thee paallel plate ai capacitos ae connected in paallel. Each capacito has plate aea 'A' and the sepaation between the plates is d, d and d espectively. The equivalent capacity of combination is ( 0 = absolute pemittivity of fee space) (A) 7 0 A 8d 0 A 8d 0 A 8d 0 7 A 8d 8
10 Q. In an oscillato, fo sustained oscillations, Bakhausen citeion is A equal to (A = voltage gain without feedback, = feedback facto) (A) Zeo Q. Light of wavelength which is less than theshold wavelength is incident on a photosensitive mateial. If incident wavelength is deceased so that emitted photoelectons ae moving with same velocity then stopping potential will (A) incease decease be zeo become exactly half Q.4 A ay of light tavelling though ae medium is incident at vey small angle i on a glass slab and afte efaction its velocity is educed by 0%. The angle of deviation is (A) 8 5 4i 5 Q.5 The maximum fequency of tansmitted adio waves above which the adio waves ae no longe eflected back by ionosphee is (N = maximum electon density of ionosphee, g = acceleation due to gavity) (A) gn gn g N gn Q.6 In Boh s theoy of Hydogen atom, the electon jumps fom highe obit n to lowe obit p. The wavelength will be minimum fo the tansition (A) n = 5 to p = 4 n = 4 to p = n = to p = n = to p = 9
11 Q.7 Two identical paallel plate ai capacitos ae connected in seies to a battey of e.m.f. V. If one of the capacito is completely filled with dielectic mateial of constant K, then potential diffeence of the othe capacito will become K (A) V(K ) V K K KV V K(K ) Q.8 The LC paallel esonant cicuit (A) has a vey high impedance has a vey high cuent acts as esistance of vey low value has zeo impedance Q.9 A galvanomete of esistance 0 is connected to a battey of emf V with 970 esistance in seies. A full scale deflection of 0 divisions is obtained in the galvanomete. To educe the deflection to 0 divisions, the esistance in seies equied is (A) Q.40 Two coheent souces P and Q poduce intefeence at point A on the sceen whee thee is a dak band which is fomed between 4th bight band and 5th bight band. Wavelength of light used is 6000Å. The path diffeence between PA and QA is 4 (A).4 0 cm 4.70 cm cm cm 0
12 Q.4 The schematic symbol of light emitting diode is (LED) Q.4 The amount of wok done in inceasing the voltage acoss the plates of capacito fom 5V to 0V is W. The wok done in inceasing it fom 0V to 5V will be (A) W 0.6 W.5 W.67 W Q.4 Magnetic flux passing though a coil is initially 40 4 Wb. It educes to 0% of its oiginal value in t second. If the e.m.f induced is 0.7 mv then t in second is (A) Q. 44 Resolving powe of telescope inceases when (A) wavelength of light deceases wavelength of light inceases focal length of eye-piece inceases ( D) focal length of eye-piece deceases Q.45 When light of wavelength ' ' is incident on photosensitive suface, the stopping potential is V. When light of wavelength is incident on same suface, the stopping potential is 'V' 6. Theshold wavelength fo the suface is (A) 4 5 Q.46 Fom Bewste s law, except fo polished metallic sufaces, the polaising angle (A) depends on wavelength and is diffeent fo diffeent colous independent of wavelength and is diffeent fo diffeent colous independent of wavelength and is same fo diffeent colous depends on wavelength and is same fo diffeent colous
13 Q.47 Two paticles X and Y having equal chages afte being acceleated though same potential diffeence ente a egion of unifom magnetic field and descibe a cicula paths of adii and espectively. The atio of the mass of X to that of Y is (A) Q.48 When an electon in Hydogen atom evolves in stationay obit, it (A) does not adiate light though its velocity changes does not adiate light and velocity emains unchanged adiates light but its velocity is unchanged adiates light with the change of enegy Q.49 The magnetic field inside a long solenoid having n, tuns pe unit length and caying cuent T when ion coe is kept in it is ( 0 = pemeability of vacuum, = magnetic susceptibility) (A) ni( ) 0 ni 0 ni ( ) 0 ni( ) 0 Q.50 In balanced mete bidge, the esistance of idge wie is 0. / cm. Uknown esistance X is connected in left gap and 6 in ight gap, null point divides the wie in the ation :. Find the cuent dawn the battey of 5 V having negligible esistance. (A) A.5 A A 5 A
12. Rolling, Torque, and Angular Momentum
12. olling, Toque, and Angula Momentum 1 olling Motion: A motion that is a combination of otational and tanslational motion, e.g. a wheel olling down the oad. Will only conside olling with out slipping.
More informationFXA 2008. Candidates should be able to : Describe how a mass creates a gravitational field in the space around it.
Candidates should be able to : Descibe how a mass ceates a gavitational field in the space aound it. Define gavitational field stength as foce pe unit mass. Define and use the peiod of an object descibing
More informationExam 3: Equation Summary
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Depatment of Physics Physics 8.1 TEAL Fall Tem 4 Momentum: p = mv, F t = p, Fext ave t= t f t= Exam 3: Equation Summay total = Impulse: I F( t ) = p Toque: τ = S S,P
More informationDeflection of Electrons by Electric and Magnetic Fields
Physics 233 Expeiment 42 Deflection of Electons by Electic and Magnetic Fields Refeences Loain, P. and D.R. Coson, Electomagnetism, Pinciples and Applications, 2nd ed., W.H. Feeman, 199. Intoduction An
More informationAP Physics Electromagnetic Wrap Up
AP Physics Electomagnetic Wap Up Hee ae the gloious equations fo this wondeful section. F qsin This is the equation fo the magnetic foce acting on a moing chaged paticle in a magnetic field. The angle
More informationPY1052 Problem Set 8 Autumn 2004 Solutions
PY052 Poblem Set 8 Autumn 2004 Solutions H h () A solid ball stats fom est at the uppe end of the tack shown and olls without slipping until it olls off the ight-hand end. If H 6.0 m and h 2.0 m, what
More informationMagnetic Field and Magnetic Forces. Young and Freedman Chapter 27
Magnetic Field and Magnetic Foces Young and Feedman Chapte 27 Intoduction Reiew - electic fields 1) A chage (o collection of chages) poduces an electic field in the space aound it. 2) The electic field
More informationSolution Derivations for Capa #8
Solution Deivations fo Capa #8 1) A ass spectoete applies a voltage of 2.00 kv to acceleate a singly chaged ion (+e). A 0.400 T field then bends the ion into a cicula path of adius 0.305. What is the ass
More informationChapter 22. Outside a uniformly charged sphere, the field looks like that of a point charge at the center of the sphere.
Chapte.3 What is the magnitude of a point chage whose electic field 5 cm away has the magnitude of.n/c. E E 5.56 1 11 C.5 An atom of plutonium-39 has a nuclea adius of 6.64 fm and atomic numbe Z94. Assuming
More informationForces & Magnetic Dipoles. r r τ = μ B r
Foces & Magnetic Dipoles x θ F θ F. = AI τ = U = Fist electic moto invented by Faaday, 1821 Wie with cuent flow (in cup of Hg) otates aound a a magnet Faaday s moto Wie with cuent otates aound a Pemanent
More information(a) The centripetal acceleration of a point on the equator of the Earth is given by v2. The velocity of the earth can be found by taking the ratio of
Homewok VI Ch. 7 - Poblems 15, 19, 22, 25, 35, 43, 51. Poblem 15 (a) The centipetal acceleation of a point on the equato of the Eath is given by v2. The velocity of the eath can be found by taking the
More informationExperiment 6: Centripetal Force
Name Section Date Intoduction Expeiment 6: Centipetal oce This expeiment is concened with the foce necessay to keep an object moving in a constant cicula path. Accoding to Newton s fist law of motion thee
More informationVector Calculus: Are you ready? Vectors in 2D and 3D Space: Review
Vecto Calculus: Ae you eady? Vectos in D and 3D Space: Review Pupose: Make cetain that you can define, and use in context, vecto tems, concepts and fomulas listed below: Section 7.-7. find the vecto defined
More informationVoltage ( = Electric Potential )
V-1 of 9 Voltage ( = lectic Potential ) An electic chage altes the space aound it. Thoughout the space aound evey chage is a vecto thing called the electic field. Also filling the space aound evey chage
More informationVoltage ( = Electric Potential )
V-1 Voltage ( = Electic Potential ) An electic chage altes the space aound it. Thoughout the space aound evey chage is a vecto thing called the electic field. Also filling the space aound evey chage is
More informationGravitation. AP Physics C
Gavitation AP Physics C Newton s Law of Gavitation What causes YOU to be pulled down? THE EARTH.o moe specifically the EARTH S MASS. Anything that has MASS has a gavitational pull towads it. F α Mm g What
More information1240 ev nm 2.5 ev. (4) r 2 or mv 2 = ke2
Chapte 5 Example The helium atom has 2 electonic enegy levels: E 3p = 23.1 ev and E 2s = 20.6 ev whee the gound state is E = 0. If an electon makes a tansition fom 3p to 2s, what is the wavelength of the
More information7 Circular Motion. 7-1 Centripetal Acceleration and Force. Period, Frequency, and Speed. Vocabulary
7 Cicula Motion 7-1 Centipetal Acceleation and Foce Peiod, Fequency, and Speed Vocabulay Vocabulay Peiod: he time it takes fo one full otation o evolution of an object. Fequency: he numbe of otations o
More informationThe Electric Potential, Electric Potential Energy and Energy Conservation. V = U/q 0. V = U/q 0 = -W/q 0 1V [Volt] =1 Nm/C
Geneal Physics - PH Winte 6 Bjoen Seipel The Electic Potential, Electic Potential Enegy and Enegy Consevation Electic Potential Enegy U is the enegy of a chaged object in an extenal electic field (Unit
More informationIntroduction to Fluid Mechanics
Chapte 1 1 1.6. Solved Examples Example 1.1 Dimensions and Units A body weighs 1 Ibf when exposed to a standad eath gavity g = 3.174 ft/s. (a) What is its mass in kg? (b) What will the weight of this body
More informationPHYSICS 111 HOMEWORK SOLUTION #13. May 1, 2013
PHYSICS 111 HOMEWORK SOLUTION #13 May 1, 2013 0.1 In intoductoy physics laboatoies, a typical Cavendish balance fo measuing the gavitational constant G uses lead sphees with masses of 2.10 kg and 21.0
More informationSELF-INDUCTANCE AND INDUCTORS
MISN-0-144 SELF-INDUCTANCE AND INDUCTORS SELF-INDUCTANCE AND INDUCTORS by Pete Signell Michigan State Univesity 1. Intoduction.............................................. 1 A 2. Self-Inductance L.........................................
More informationDetermining solar characteristics using planetary data
Detemining sola chaacteistics using planetay data Intoduction The Sun is a G type main sequence sta at the cente of the Sola System aound which the planets, including ou Eath, obit. In this inestigation
More informationThe Role of Gravity in Orbital Motion
! The Role of Gavity in Obital Motion Pat of: Inquiy Science with Datmouth Developed by: Chistophe Caoll, Depatment of Physics & Astonomy, Datmouth College Adapted fom: How Gavity Affects Obits (Ohio State
More informationLab M4: The Torsional Pendulum and Moment of Inertia
M4.1 Lab M4: The Tosional Pendulum and Moment of netia ntoduction A tosional pendulum, o tosional oscillato, consists of a disk-like mass suspended fom a thin od o wie. When the mass is twisted about the
More informationGauss Law. Physics 231 Lecture 2-1
Gauss Law Physics 31 Lectue -1 lectic Field Lines The numbe of field lines, also known as lines of foce, ae elated to stength of the electic field Moe appopiately it is the numbe of field lines cossing
More informationExperiment MF Magnetic Force
Expeiment MF Magnetic Foce Intoduction The magnetic foce on a cuent-caying conducto is basic to evey electic moto -- tuning the hands of electic watches and clocks, tanspoting tape in Walkmans, stating
More informationEpisode 401: Newton s law of universal gravitation
Episode 401: Newton s law of univesal gavitation This episode intoduces Newton s law of univesal gavitation fo point masses, and fo spheical masses, and gets students pactising calculations of the foce
More information2 r2 θ = r2 t. (3.59) The equal area law is the statement that the term in parentheses,
3.4. KEPLER S LAWS 145 3.4 Keple s laws You ae familia with the idea that one can solve some mechanics poblems using only consevation of enegy and (linea) momentum. Thus, some of what we see as objects
More informationProblems of the 2 nd and 9 th International Physics Olympiads (Budapest, Hungary, 1968 and 1976)
Poblems of the nd and 9 th Intenational Physics Olympiads (Budapest Hungay 968 and 976) Péte Vankó Institute of Physics Budapest Univesity of Technology and Economics Budapest Hungay Abstact Afte a shot
More informationPhys 2101 Gabriela González. cos. sin. sin
1 Phys 101 Gabiela González a m t t ma ma m m T α φ ω φ sin cos α τ α φ τ sin m m α τ I We know all of that aleady!! 3 The figue shows the massive shield doo at a neuton test facility at Lawence Livemoe
More information4a 4ab b 4 2 4 2 5 5 16 40 25. 5.6 10 6 (count number of places from first non-zero digit to
. Simplify: 0 4 ( 8) 0 64 ( 8) 0 ( 8) = (Ode of opeations fom left to ight: Paenthesis, Exponents, Multiplication, Division, Addition Subtaction). Simplify: (a 4) + (a ) (a+) = a 4 + a 0 a = a 7. Evaluate
More informationGravity. A. Law of Gravity. Gravity. Physics: Mechanics. A. The Law of Gravity. Dr. Bill Pezzaglia. B. Gravitational Field. C.
Physics: Mechanics 1 Gavity D. Bill Pezzaglia A. The Law of Gavity Gavity B. Gavitational Field C. Tides Updated: 01Jul09 A. Law of Gavity 3 1a. Invese Squae Law 4 1. Invese Squae Law. Newton s 4 th law
More informationSolutions for Physics 1301 Course Review (Problems 10 through 18)
Solutions fo Physics 1301 Couse Review (Poblems 10 though 18) 10) a) When the bicycle wheel comes into contact with the step, thee ae fou foces acting on it at that moment: its own weight, Mg ; the nomal
More informationVISCOSITY OF BIO-DIESEL FUELS
VISCOSITY OF BIO-DIESEL FUELS One of the key assumptions fo ideal gases is that the motion of a given paticle is independent of any othe paticles in the system. With this assumption in place, one can use
More informationTORQUE AND ANGULAR MOMENTUM IN CIRCULAR MOTION
MISN-0-34 TORQUE AND ANGULAR MOMENTUM IN CIRCULAR MOTION shaft TORQUE AND ANGULAR MOMENTUM IN CIRCULAR MOTION by Kiby Mogan, Chalotte, Michigan 1. Intoduction..............................................
More informationPhysics 235 Chapter 5. Chapter 5 Gravitation
Chapte 5 Gavitation In this Chapte we will eview the popeties of the gavitational foce. The gavitational foce has been discussed in geat detail in you intoductoy physics couses, and we will pimaily focus
More informationCarter-Penrose diagrams and black holes
Cate-Penose diagams and black holes Ewa Felinska The basic intoduction to the method of building Penose diagams has been pesented, stating with obtaining a Penose diagam fom Minkowski space. An example
More informationF G r. Don't confuse G with g: "Big G" and "little g" are totally different things.
G-1 Gavity Newton's Univesal Law of Gavitation (fist stated by Newton): any two masses m 1 and m exet an attactive gavitational foce on each othe accoding to m m G 1 This applies to all masses, not just
More informationCharges, Coulomb s Law, and Electric Fields
Q&E -1 Chages, Coulomb s Law, and Electic ields Some expeimental facts: Expeimental fact 1: Electic chage comes in two types, which we call (+) and ( ). An atom consists of a heavy (+) chaged nucleus suounded
More informationDisplacement, Velocity And Acceleration
Displacement, Velocity And Acceleation Vectos and Scalas Position Vectos Displacement Speed and Velocity Acceleation Complete Motion Diagams Outline Scala vs. Vecto Scalas vs. vectos Scala : a eal numbe,
More informationStructure and evolution of circumstellar disks during the early phase of accretion from a parent cloud
Cente fo Tubulence Reseach Annual Reseach Biefs 2001 209 Stuctue and evolution of cicumstella disks duing the ealy phase of accetion fom a paent cloud By Olusola C. Idowu 1. Motivation and Backgound The
More informationMultiple choice questions [60 points]
1 Multiple choice questions [60 points] Answe all o the ollowing questions. Read each question caeully. Fill the coect bubble on you scanton sheet. Each question has exactly one coect answe. All questions
More information2. Orbital dynamics and tides
2. Obital dynamics and tides 2.1 The two-body poblem This efes to the mutual gavitational inteaction of two bodies. An exact mathematical solution is possible and staightfowad. In the case that one body
More informationPhysics HSC Course Stage 6. Space. Part 1: Earth s gravitational field
Physics HSC Couse Stage 6 Space Pat 1: Eath s gavitational field Contents Intoduction... Weight... 4 The value of g... 7 Measuing g...8 Vaiations in g...11 Calculating g and W...13 You weight on othe
More informationwww.sakshieducation.com
Viscosity. The popety of viscosity in gas is due to ) Cohesive foces between the moecues ) Coisions between the moecues ) Not having a definite voume ) Not having a definite size. When tempeatue is inceased
More informationChapter 17 The Kepler Problem: Planetary Mechanics and the Bohr Atom
Chapte 7 The Keple Poblem: Planetay Mechanics and the Boh Atom Keple s Laws: Each planet moves in an ellipse with the sun at one focus. The adius vecto fom the sun to a planet sweeps out equal aeas in
More informationThe force between electric charges. Comparing gravity and the interaction between charges. Coulomb s Law. Forces between two charges
The foce between electic chages Coulomb s Law Two chaged objects, of chage q and Q, sepaated by a distance, exet a foce on one anothe. The magnitude of this foce is given by: kqq Coulomb s Law: F whee
More informationChapter 2. Electrostatics
Chapte. Electostatics.. The Electostatic Field To calculate the foce exeted by some electic chages,,, 3,... (the souce chages) on anothe chage Q (the test chage) we can use the pinciple of supeposition.
More informationGravitation and Kepler s Laws Newton s Law of Universal Gravitation in vectorial. Gm 1 m 2. r 2
F Gm Gavitation and Keple s Laws Newton s Law of Univesal Gavitation in vectoial fom: F 12 21 Gm 1 m 2 12 2 ˆ 12 whee the hat (ˆ) denotes a unit vecto as usual. Gavity obeys the supeposition pinciple,
More informationNUCLEAR MAGNETIC RESONANCE
19 Jul 04 NMR.1 NUCLEAR MAGNETIC RESONANCE In this expeiment the phenomenon of nuclea magnetic esonance will be used as the basis fo a method to accuately measue magnetic field stength, and to study magnetic
More informationTECHNICAL DATA. JIS (Japanese Industrial Standard) Screw Thread. Specifications
JIS (Japanese Industial Standad) Scew Thead Specifications TECNICAL DATA Note: Although these specifications ae based on JIS they also apply to and DIN s. Some comments added by Mayland Metics Coutesy
More informationChapter 30: Magnetic Fields Due to Currents
d Chapte 3: Magnetic Field Due to Cuent A moving electic chage ceate a magnetic field. One of the moe pactical way of geneating a lage magnetic field (.1-1 T) i to ue a lage cuent flowing though a wie.
More informationAnalytical Proof of Newton's Force Laws
Analytical Poof of Newton s Foce Laws Page 1 1 Intouction Analytical Poof of Newton's Foce Laws Many stuents intuitively assume that Newton's inetial an gavitational foce laws, F = ma an Mm F = G, ae tue
More informationFigure 2. So it is very likely that the Babylonians attributed 60 units to each side of the hexagon. Its resulting perimeter would then be 360!
1. What ae angles? Last time, we looked at how the Geeks intepeted measument of lengths. Howeve, as fascinated as they wee with geomety, thee was a shape that was much moe enticing than any othe : the
More informationMultiple choice questions [70 points]
Multiple choice questions [70 points] Answe all of the following questions. Read each question caefull. Fill the coect bubble on ou scanton sheet. Each question has exactl one coect answe. All questions
More informationLesson 7 Gauss s Law and Electric Fields
Lesson 7 Gauss s Law and Electic Fields Lawence B. Rees 7. You may make a single copy of this document fo pesonal use without witten pemission. 7. Intoduction While it is impotant to gain a solid conceptual
More informationLab #7: Energy Conservation
Lab #7: Enegy Consevation Photo by Kallin http://www.bungeezone.com/pics/kallin.shtml Reading Assignment: Chapte 7 Sections 1,, 3, 5, 6 Chapte 8 Sections 1-4 Intoduction: Pehaps one of the most unusual
More informationChapter 19: Electric Charges, Forces, and Fields ( ) ( 6 )( 6
Chapte 9 lectic Chages, Foces, an Fiels 6 9. One in a million (0 ) ogen molecules in a containe has lost an electon. We assume that the lost electons have been emove fom the gas altogethe. Fin the numbe
More informationCRRC-1 Method #1: Standard Practice for Measuring Solar Reflectance of a Flat, Opaque, and Heterogeneous Surface Using a Portable Solar Reflectometer
CRRC- Method #: Standad Pactice fo Measuing Sola Reflectance of a Flat, Opaque, and Heteogeneous Suface Using a Potable Sola Reflectomete Scope This standad pactice coves a technique fo estimating the
More information10. Collisions. Before During After
10. Collisions Use conseation of momentum and enegy and the cente of mass to undestand collisions between two objects. Duing a collision, two o moe objects exet a foce on one anothe fo a shot time: -F(t)
More informationFluids Lecture 15 Notes
Fluids Lectue 15 Notes 1. Unifom flow, Souces, Sinks, Doublets Reading: Andeson 3.9 3.12 Unifom Flow Definition A unifom flow consists of a velocit field whee V = uî + vĵ is a constant. In 2-D, this velocit
More informationMotion Control Formulas
ems: A = acceleation ate {in/sec } C = caiage thust foce {oz} D = deceleation ate {in/sec } d = lead of scew {in/ev} e = lead scew efficiency ball scew 90% F = total fictional foce {oz} GR = gea atio J
More informationChapter 4: Fluid Kinematics
Oveview Fluid kinematics deals with the motion of fluids without consideing the foces and moments which ceate the motion. Items discussed in this Chapte. Mateial deivative and its elationship to Lagangian
More informationModel Question Paper Mathematics Class XII
Model Question Pape Mathematics Class XII Time Allowed : 3 hous Maks: 100 Ma: Geneal Instuctions (i) The question pape consists of thee pats A, B and C. Each question of each pat is compulsoy. (ii) Pat
More informationAn Introduction to Omega
An Intoduction to Omega Con Keating and William F. Shadwick These distibutions have the same mean and vaiance. Ae you indiffeent to thei isk-ewad chaacteistics? The Finance Development Cente 2002 1 Fom
More informationGAUSS S LAW APPLIED TO CYLINDRICAL AND PLANAR CHARGE DISTRIBUTIONS ` E MISN-0-133. CHARGE DISTRIBUTIONS by Peter Signell, Michigan State University
MISN-0-133 GAUSS S LAW APPLIED TO CYLINDRICAL AND PLANAR CHARGE DISTRIBUTIONS GAUSS S LAW APPLIED TO CYLINDRICAL AND PLANAR CHARGE DISTRIBUTIONS by Pete Signell, Michigan State Univesity 1. Intoduction..............................................
More informationQuantity Formula Meaning of variables. 5 C 1 32 F 5 degrees Fahrenheit, 1 bh A 5 area, b 5 base, h 5 height. P 5 2l 1 2w
1.4 Rewite Fomulas and Equations Befoe You solved equations. Now You will ewite and evaluate fomulas and equations. Why? So you can apply geometic fomulas, as in Ex. 36. Key Vocabulay fomula solve fo a
More informationLecture 16: Color and Intensity. and he made him a coat of many colours. Genesis 37:3
Lectue 16: Colo and Intensity and he made him a coat of many colous. Genesis 37:3 1. Intoduction To display a pictue using Compute Gaphics, we need to compute the colo and intensity of the light at each
More informationThe Gravity Field of the Earth - Part 1 (Copyright 2002, David T. Sandwell)
1 The Gavity Field of the Eath - Pat 1 (Copyight 00, David T. Sandwell) This chapte coves physical geodesy - the shape of the Eath and its gavity field. This is just electostatic theoy applied to the Eath.
More informationAN IMPLEMENTATION OF BINARY AND FLOATING POINT CHROMOSOME REPRESENTATION IN GENETIC ALGORITHM
AN IMPLEMENTATION OF BINARY AND FLOATING POINT CHROMOSOME REPRESENTATION IN GENETIC ALGORITHM Main Golub Faculty of Electical Engineeing and Computing, Univesity of Zageb Depatment of Electonics, Micoelectonics,
More information8.4. Motion of Charged Particles in Magnetic Fields
Motion of Chaged Paticles in Magnetic Fields Atos and olecules ae paticles that ae the building blocks of ou uniese. How do scientists study the natue of these sall paticles? The ass spectoete shown in
More informationMultiband Microstrip Patch Antenna for Microwave Applications
IOSR Jounal of Electonics and Communication Engineeing (IOSR-JECE) ISSN: 2278-2834, ISBN: 2278-8735. Volume 3, Issue 5 (Sep. - Oct. 2012), PP 43-48 Multiband Micostip Patch Antenna fo Micowave Applications
More informationChapter 4: Fluid Kinematics
4-1 Lagangian g and Euleian Desciptions 4-2 Fundamentals of Flow Visualization 4-3 Kinematic Desciption 4-4 Reynolds Tanspot Theoem (RTT) 4-1 Lagangian and Euleian Desciptions (1) Lagangian desciption
More informationDIFFERENT TYPES OF HUMAN HEAD SHAPES FOR CELLULAR PHONE EXPOSURE ON ELECTROMAGNETIC ABSORPTION
DIFFERENT TYPES OF HUMAN HEAD SHAPES FOR CELLULAR PHONE EXPOSURE ON ELECTROMAGNETIC ABSORPTION Mohammad Rashed Iqbal Fauque* #1, Mohammad Taiqul Islam* 2, Nobahiah Misan* #3 * Institute of Space Science
More informationDipole moments 1 2.10 DETERMINATION OF DIPOLE MOMENT FROM RELATIVE PERMITTIVITY AND REFRACTIVE INDEX. Plates applying external electric field
Dipole moments 1.10 DETERMINATION OF DIPOLE MOMENT FROM RELATIVE PERMITTIVITY AND REFRACTIVE INDEX (4 points) Plates applying extenal electic field Suface chages on dielectic block Figue 1. Polaization
More information1D STEADY STATE HEAT
D SEADY SAE HEA CONDUCION () Pabal alukda Aociate Pofeo Depatment of Mecanical Engineeing II Deli E-mail: pabal@mec.iitd.ac.in Palukda/Mec-IID emal Contact eitance empeatue ditibution and eat flow line
More informationSpirotechnics! September 7, 2011. Amanda Zeringue, Michael Spannuth and Amanda Zeringue Dierential Geometry Project
Spiotechnics! Septembe 7, 2011 Amanda Zeingue, Michael Spannuth and Amanda Zeingue Dieential Geomety Poject 1 The Beginning The geneal consensus of ou goup began with one thought: Spiogaphs ae awesome.
More informationElectrostatic properties of conductors and dielectrics
Unit Electostatic popeties of conductos and dielectics. Intoduction. Dielectic beaking. onducto in electostatic equilibium..3 Gound connection.4 Phenomena of electostatic influence. Electostatic shields.5
More informationFinancing Terms in the EOQ Model
Financing Tems in the EOQ Model Habone W. Stuat, J. Columbia Business School New Yok, NY 1007 hws7@columbia.edu August 6, 004 1 Intoduction This note discusses two tems that ae often omitted fom the standad
More informationChapter 3 Savings, Present Value and Ricardian Equivalence
Chapte 3 Savings, Pesent Value and Ricadian Equivalence Chapte Oveview In the pevious chapte we studied the decision of households to supply hous to the labo maket. This decision was a static decision,
More informationSkills Needed for Success in Calculus 1
Skills Needed fo Success in Calculus Thee is much appehension fom students taking Calculus. It seems that fo man people, "Calculus" is snonmous with "difficult." Howeve, an teache of Calculus will tell
More informationMechanics 1: Motion in a Central Force Field
Mechanics : Motion in a Cental Foce Field We now stud the popeties of a paticle of (constant) ass oving in a paticula tpe of foce field, a cental foce field. Cental foces ae ve ipotant in phsics and engineeing.
More informationGravitational Mechanics of the Mars-Phobos System: Comparing Methods of Orbital Dynamics Modeling for Exploratory Mission Planning
Gavitational Mechanics of the Mas-Phobos System: Compaing Methods of Obital Dynamics Modeling fo Exploatoy Mission Planning Alfedo C. Itualde The Pennsylvania State Univesity, Univesity Pak, PA, 6802 This
More informationDYNAMICS AND STRUCTURAL LOADING IN WIND TURBINES
DYNAMIS AND STRUTURAL LOADING IN WIND TURBINES M. Ragheb 12/30/2008 INTRODUTION The loading egimes to which wind tubines ae subject to ae extemely complex equiing special attention in thei design, opeation
More informationA r. (Can you see that this just gives the formula we had above?)
24-1 (SJP, Phys 1120) lectic flux, and Gauss' law Finding the lectic field due to a bunch of chages is KY! Once you know, you know the foce on any chage you put down - you can pedict (o contol) motion
More informationCHAPTER 5 GRAVITATIONAL FIELD AND POTENTIAL
CHATER 5 GRAVITATIONAL FIELD AND OTENTIAL 5. Intoduction. This chapte deals with the calculation of gavitational fields and potentials in the vicinity of vaious shapes and sizes of massive bodies. The
More informationCoordinate Systems L. M. Kalnins, March 2009
Coodinate Sstems L. M. Kalnins, Mach 2009 Pupose of a Coodinate Sstem The pupose of a coodinate sstem is to uniquel detemine the position of an object o data point in space. B space we ma liteall mean
More informationChapte 3 Is Gavitation A Results Of Asymmetic Coulomb Chage Inteactions? Jounal of Undegaduate Reseach èjurè Univesity of Utah è1992è, Vol. 3, No. 1, pp. 56í61. Jeæey F. Gold Depatment of Physics, Depatment
More informationSupplementary Material for EpiDiff
Supplementay Mateial fo EpiDiff Supplementay Text S1. Pocessing of aw chomatin modification data In ode to obtain the chomatin modification levels in each of the egions submitted by the use QDCMR module
More informationDesign of Wind Energy System on the Building Tower Applications
ISSN(Online): 39-8753 ISSN (Pint) :347-67 (An ISO 397: 7 Cetified Oganization) Vol. 4, Issue, Febuay 5 Design of Wind Enegy System on the Building owe Applications D.Anusha, L V Suesh Kuma, G.V. Nagesh
More informationExam in physics, El-grunder (Electromagnetism), 2014-03-26, kl 9.00-15.00
Umeå Univesitet, Fysik 1 Vitly Bychkov Em in physics, El-gunde (Electomgnetism, 14--6, kl 9.-15. Hjälpmedel: Students my use ny book(s. Mino notes in the books e lso llowed. Students my not use thei lectue
More information3 Molecules in Electric and Magnetic Fields
Chapte, page Molecules in Electic and Magnetic Fields. Basic Equations fom Electodynamics The basis of the desciption of the behaviou of molecules in electic and magnetic fields ae the mateial equations
More informationEpdf Sulf petroleum, Eflecti and Eeflecti
ANALYSIS OF GLOBAL WARMING MITIGATION BY WHITE REFLECTING SURFACES Fedeico Rossi, Andea Nicolini Univesity of Peugia, CIRIAF Via G.Duanti 67 0615 Peugia, Italy T: +9-075-585846; F: +9-075-5848470; E: fossi@unipg.it
More informationPhysics Core Topic 9.2 Space
Physics 9. Space Syllabus Notes Physics Coe Topic 9. Space Summay of Contextual Outline Scientists daw on othe aeas of science to deelop iable spacecaft Launch, e enty and landing ae dangeous Huge foces
More informationTHERMAL ISOLATION TECHNIQUES FOR CURE MONITORING USING FBG OPTICAL SENSORS
THERMAL OLATION TECHNIQUES FOR CURE MONITORING USING FBG OPTICAL SENSORS E.K.G. Boateng, P.J. Schubel, N.A. Waio Polyme Composites Goup Division of Mateials, Mechanics and Stuctues Faculty of Engineeing
More informationMolecular Dynamics Simulations and Neutron Scattering: Polymer Melt and Solution Dynamics
Molecula Dynamics Simulations and Neuton Scatteing: Polyme Melt and Solution Dynamics Gant D. Smith Depatment of Mateials Science and Engineeing Univesity of Utah Polyme Dynamics and Relaxation Richad
More informationNURBS Drawing Week 5, Lecture 10
CS 43/585 Compute Gaphics I NURBS Dawing Week 5, Lectue 1 David Been, William Regli and Maim Pesakhov Geometic and Intelligent Computing Laboato Depatment of Compute Science Deel Univesit http://gicl.cs.deel.edu
More informationAdvanced Control of Active Filters. in a Battery Charger Application. Martin Bojrup
Advanced Contol of Active Filtes in a Battey Chage Application Matin Bojup Lund 999 ii Cove pictue Measuement on the dynamic esponse of the MRI hamonic filte contolle: load cuent (top), esulting line cuent
More informationMoment and couple. In 3-D, because the determination of the distance can be tedious, a vector approach becomes advantageous. r r
Moment and couple In 3-D, because the detemination of the distance can be tedious, a vecto appoach becomes advantageous. o k j i M k j i M o ) ( ) ( ) ( + + M o M + + + + M M + O A Moment about an abita
More information