Class: Life-Science Subject: Physics

Similar documents
1.3 Hence, calculate a formula for the force required to break the bond (i.e. the maximum value of F)

CHAPTER 10 ROTATIONAL MOTION

Physics 207 Lecture 6

Elastic Collisions. Definition: two point masses on which no external forces act collide without losing any energy.

Linear Momentum. Center of Mass.

Physics 4B. Question and 3 tie (clockwise), then 2 and 5 tie (zero), then 4 and 6 tie (counterclockwise) B i. ( T / s) = 1.74 V.

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

Solutions to Practice Problems

PHYSICS - CLUTCH CH 28: INDUCTION AND INDUCTANCE.

> To construct a potential representation of E and B, you need a vector potential A r, t scalar potential ϕ ( F,t).

PHYS 1443 Section 002 Lecture #20

11. Dynamics in Rotating Frames of Reference

PHYSICS - CLUTCH 1E CH 28: INDUCTION AND INDUCTANCE.

Study Guide For Exam Two

Lecture 09 Systems of Particles and Conservation of Linear Momentum

Chapter 8. Potential Energy and Conservation of Energy

How does the momentum before an elastic and an inelastic collision compare to the momentum after the collision?

Physics 4B. A positive value is obtained, so the current is counterclockwise around the circuit.

Physics 3A: Linear Momentum. Physics 3A: Linear Momentum. Physics 3A: Linear Momentum. Physics 3A: Linear Momentum

Page 1. SPH4U: Lecture 7. New Topic: Friction. Today s Agenda. Surface Friction... Surface Friction...

Please initial the statement below to show that you have read it

( ) = ( ) + ( 0) ) ( )

First Law: A body at rest remains at rest, a body in motion continues to move at constant velocity, unless acted upon by an external force.

Linear Momentum. Center of Mass.

Physics 141. Lecture 14. Frank L. H. Wolfs Department of Physics and Astronomy, University of Rochester, Lecture 14, Page 1

Week 9 Chapter 10 Section 1-5

Moments of Inertia. and reminds us of the analogous equation for linear momentum p= mv, which is of the form. The kinetic energy of the body is.

Period & Frequency. Work and Energy. Methods of Energy Transfer: Energy. Work-KE Theorem 3/4/16. Ranking: Which has the greatest kinetic energy?

Chapter 3 and Chapter 4

THE CURRENT BALANCE Physics 258/259

Lecture 16. Chapter 11. Energy Dissipation Linear Momentum. Physics I. Department of Physics and Applied Physics

PHY2049 Exam 2 solutions Fall 2016 Solution:

Chapter 11 Angular Momentum

Physics 201 Lecture 9

PHYS 2211L - Principles of Physics Laboratory I

Demonstrate Teaching FEM, Particle Dynamics, and Simple MD Codes Using Matlab & Mathematica

Section 8.1 Exercises

Chapter 8. Momentum Impulse and Collisions. Analysis of motion: 2 key ideas. Newton s laws of motion. Conservation of Energy

Solutions for Homework #9

Physics 1202: Lecture 11 Today s Agenda

= 1.23 m/s 2 [W] Required: t. Solution:!t = = 17 m/s [W]! m/s [W] (two extra digits carried) = 2.1 m/s [W]

Chapter 7: Conservation of Energy

Modeling of Dynamic Systems

The equation of motion of a dynamical system is given by a set of differential equations. That is (1)

Electric Potential Energy & Potential. Electric Potential Energy. Potential Energy. Potential Energy. Example: Charge launcher

Physic 231 Lecture 14

Part C Dynamics and Statics of Rigid Body. Chapter 5 Rotation of a Rigid Body About a Fixed Axis

System in Weibull Distribution

ENGN 40 Dynamics and Vibrations Homework # 7 Due: Friday, April 15

Physics 231. Topic 8: Rotational Motion. Alex Brown October MSU Physics 231 Fall

Week 8: Chapter 9. Linear Momentum. Newton Law and Momentum. Linear Momentum, cont. Conservation of Linear Momentum. Conservation of Momentum, 2

Physics 114 Exam 2 Spring Name:

total If no external forces act, the total linear momentum of the system is conserved. This occurs in collisions and explosions.

Physics 114 Exam 3 Spring Name:

Chapter 7. Potential Energy and Conservation of Energy

Physics 207: Lecture 20. Today s Agenda Homework for Monday

Physics 2A Chapter 3 HW Solutions

DC Circuits. Crossing the emf in this direction +ΔV

Electricity and Magnetism Lecture 13 - Physics 121 Electromagnetic Oscillations in LC & LCR Circuits,

Week 6, Chapter 7 Sect 1-5

Applied Mathematics Letters

A Tale of Friction Basic Rollercoaster Physics. Fahrenheit Rollercoaster, Hershey, PA max height = 121 ft max speed = 58 mph

Chapter 3. r r. Position, Velocity, and Acceleration Revisited

Physics 2102 Spring 2007 Lecture 10 Current and Resistance

Phys 331: Ch 7,.2 Unconstrained Lagrange s Equations 1

On the number of regions in an m-dimensional space cut by n hyperplanes

EXAMPLES of THEORETICAL PROBLEMS in the COURSE MMV031 HEAT TRANSFER, version 2017

Frequency dependence of the permittivity

Chapter 11 Torque and Angular Momentum

ˆ (0.10 m) E ( N m /C ) 36 ˆj ( j C m)

PHYS 1101 Practice problem set 12, Chapter 32: 21, 22, 24, 57, 61, 83 Chapter 33: 7, 12, 32, 38, 44, 49, 76

Physics 231. Topic 8: Rotational Motion. Alex Brown October MSU Physics 231 Fall

Physics 111 Final Exam, Fall 2013, Version A

Math1110 (Spring 2009) Prelim 3 - Solutions

Lecture #4 Capacitors and Inductors Energy Stored in C and L Equivalent Circuits Thevenin Norton

Advanced Circuits Topics - Part 1 by Dr. Colton (Fall 2017)

Section 8.3 Polar Form of Complex Numbers

10/2/2003 PHY Lecture 9 1

A particle in a state of uniform motion remain in that state of motion unless acted upon by external force.

Description of the Force Method Procedure. Indeterminate Analysis Force Method 1. Force Method con t. Force Method con t

EMU Physics Department

Army Ants Tunneling for Classical Simulations

Chapter Seven - Potential Energy and Conservation of Energy

AP Physics 1 & 2 Summer Assignment

Electricity and Magnetism Review Faraday s Law

Physics 114 Exam 2 Fall 2014 Solutions. Name:

MAE140 - Linear Circuits - Winter 16 Midterm, February 5

Dynamics of Rotational Motion

EMF induced in a coil by moving a bar magnet. Induced EMF: Faraday s Law. Induction and Oscillations. Electromagnetic Induction.

Physics 607 Exam 1. ( ) = 1, Γ( z +1) = zγ( z) x n e x2 dx = 1. e x2

Chapter 8 Potential Energy and Conservation of Energy Important Terms (For chapters 7 and 8)

Remark: Positive work is done on an object when the point of application of the force moves in the direction of the force.

Physics 40 HW #4 Chapter 4 Key NEATNESS COUNTS! Solve but do not turn in the following problems from Chapter 4 Knight

Quantum Mechanics I Problem set No.1

EN40: Dynamics and Vibrations. Homework 7: Rigid Body Kinematics

RE 11.e Mon. Review for Final (1-11) HW11: Pr s 39, 57, 64, 74, 78 Sat. 9 a.m. Final Exam (Ch. 1-11)

INDUCTANCE. RC Cicuits vs LR Circuits

Momentum and Collisions. Rosendo Physics 12-B

Chapter 8. Momentum, Impulse and Collisions (continued) 10/22/2014 Physics 218

Physics 207 Lecture 13. Lecture 13

Transcription:

Class: Lfe-Scence Subject: Physcs Frst year (6 pts): Graphc desgn of an energy exchange A partcle (B) of ass =g oves on an nclned plane of an nclned angle α = 3 relatve to the horzontal. We want to study the energy exchange between the syste (B, Earth) and the envronent A O For ths purpose, we launch (B) at te t =, fro O along the lne of greatest slope of the nclned plane Ox, wth an ntal velocty / s. Frctonal forces are v 6 equvalent to f at an opposte drecton to the velocty and of value f =,N.. The echancal energy of the syste (B, Earth) s not conserved. Justfed?. Deterne the echancal energy of the syste at pont O. 3. The ball (B ) passes at a te t by a pont A of abscssa OA = x. a) Deterne as functon of x, the expresson of the echancal energy of the syste (B, Earth) at te t. b ) Deterne as functon of x, the expresson of the gravtatonal potental energy of the syste at te t. 4 a) Draw n the sae syste of axs the curves gvng the varatons, dependng on x, of E and Epp. scale on the x-axs : c. on the energy axs : c.j b ) Use the graph to deterne the speed of (B) at x =. c) Fro the graph, deterne the value X of x for whch the speed s nll. d) The syste (B, Earth) then exchange energy wth the envronent. In what for and how uch?

Second year ( 7 pts ) Collson and echancal oscllator - ABC a track s consttuted by a horzontal plane BC, and nclned plane AB by an angle α = 3 wth the horzontal such that AB = 9 c. - A ass less sprng of stffness K= N /. t s fxed at one end n C, the other end beng connected to a punctual sold ( S ) of ass = 4g. The orgn O of the reference poston concdes wth the center of nerta of the sold ( S ) when the sprng s at rest. We neglect all the forces of frcton on (CB). - A punctual sold ( S ) of ass = 6 g placed n A. The horzontal plane BC s taken as the reference level of the gravtatonal potental energy of the syste. (g = /s ). A- Neglectng all frcton on (AB) : S S C B O. (S ), let go fro A wthout ntal speed. Deterne the velocty vector of (S v ) n O.. It copresses the sprng 6 c, then left the ass wthout ntal speed. Deterne the velocty vector of ( S ) at O. 3. ( S ) coes nto a frontal collson wth ( S ) at O ( equlbru poston ), thus forng a sngle ateral pont ( S ). Deterne the velocty vector of ( S ) edately after the shock. 4. The set ( S, R ) for a horzontal sprng pendulu, ( S ) oscllatng around ts equlbru poston O. a) Establsh the dfferental equaton of x of the oscllatons. b ) The soluton of the dfferental equaton s of the for x = X cos ( - Gve the eanng of each ter n ths expresson. ) t T

- Deterne the expresson of the proper perod T and calculate ts value. - Deterne nuercally the constants X and own the experence. Derve the nuercal expresson of x (t). B- In fact, the speed of ( S ) n O s / s. frcton are not neglgble n (AB) : a) Calculate the value of the assued constant frcton. b ) the syste ( S, R ) does not oscllate after pact. Justfed? Thrd year ( 7pts ) Use of a col A- Frst Experence A bar agnet ay be oved along the axs of a col ( x axs ), the ternals A and C are connected to an ohc conductor of resstance R = 3Ω N S x A R C The south pole of the agnet s approached to the sde A of the col. Gve the nae of the phenoenon deonstrated n ths experent?. Indcate the nductng source and the nductor. 3. Is there appearance of a current n the crcut? Why? 4. Indcate and justfy the drecton of the nduced current n R. 5. Represent the proper agnetc feld created n the col. B- Second experent The col s fored by N = turns at each secton of S = c, and nternal resstance of r = Ω. Assue that the agnet durng ts oveent through the col creates a unfor agnetc feld parallel to x x of vector B = B. The varaton of B as a functon of te s shown n the graph n the fgure aganst. ) Indcate on the segent the lne of acton and the drecton of the noral vector n ) Deterne the agnetc flux ( ) n the te nterval [, 3s ], [ 3 s, 5 s ] and [ 5s, 7s ]

3) Deterne the nduced electrootve force ( e) n the precedng ntervals. 4) Calculate n the prevous ntervals, the ntensty of the nduced current and deterne the drecton of the nduced current n R. 5) Represent the voltage U AC as functon of te. B(T) 3,5,5,5 t(s) O 4 6 Good Luck

The Correcton Preer exercse. We have frcton forces. Syste (B, Earth) Reference level E o E o E o c pp v,.36 3,6 j (/) 3. a) we apply the varaton of echancal energy between et t: E E t E o w. f E E o f x 3,6, x (x en ; E en j) (/) b) E pp (A) = gz A = gxsnα = x ( x en ; E en j) (/) 4. a) graph ( - ) b) At x = ; E pp = j et E = 3, j (/) E c = E - E pp = 3, =, j., v, v 3,46 (/), s c) v = E pp =E = 3 j. (/) X = 3. d) heat Q = ΔE = 3,6-3 =,6 j.

Second Exercse : A. Syste (S, Earth) Reference level f E s conserved E A = E o E co + E ppo = E ca + E ppa sn v gab v gab sn 9 3 s v 3. s. Syste (S, Earth) E = E o kx v k v x 3 s v 3 s. 3. Collson : the lnear oentu s conserved P av P ap v v v,6.3, 4.3 v

,6 v,6 s 4. a) Syste (S, R, Earth) E = E c + E pél = v kx E de cte dt x x kx k x x b) - X : apltude ; T o : perod ; : ntal phase - x X cos t T x X sn t T T 4 x X cos t T T 4 x x T k 4 T T k,98 s. x - v,6 s

x X cos cos v X sn, 6 sn T (/) X,65c,65cos 33,3 x t t B- a) Syste (S, Earth) We have frcton between A et B. We apply the varaton of echancal energy A et B. E w f E E f AB A. v gab sn f. AB,5.,5.4 5.,9.,5,9.f f,5,389 N.,9 b) The speed of S after collson P av P ap v v v, 6., 4.3. v v v

The speed of S after collson s null at O then the syste does not oscllate. Thrd exercse A-. Electroagnetc nducton. agnet: source of nductng ; col: nductor 3. when we dsplace the agnet close to the col the value of B vared n the col the flux vared, close crcut ; we have current n the crcut 4. Accordng to Lenz law le pole the current passes n R fro C toa. 5. A B p C B-. Fgure. nb, NSB cos n, B,B Pour t ;3s 3 B t SI 8. 3. 8. 3. 3 4 t SI Pour t 3 s;5s

B 5. 4 T 5 5. wb Pour t 5 s;7s 4 B t SI 3, 45. 45. 5 t SI d 3. Faraday s law e dt t s;3s e = 8. -3 v. t 3 s;5s e =. t 5 s;7s e = - - v. 4. ub u R e r R e r R 8. 5 3 3,6. A crculate n the postve drecton 5 3 3. A crculate n the negatve drecton 5. u R = R u = 4,8. -3 v. u = v. u 3 = -6. -3 v. fgure (/)