IPhO第届国际物理奥林匹克竞赛理论试题与解答
国际物理林匹克竞赛试题25th_IPhO_1994
THE EXAMINATIONXXV INTERNATIONAL PHYSICS OLYMPIADBEIJING, PERPLE’S REPUBLIC CHINATHEORETICAL COMPETITIONJuly 13, 1994Time available: 5 hoursREAD THIS FIRST!INSTRUCTIONS:1. Use only the ball pen provided.2. Your graphs should be drawn on the answer sheets attached to the problem.3. Your solutions should be written on the sheets of paper attached to the problems.4. Write at the top of the first page of each problem:●The total number of pages in your solution to the problem●Your name and code numberTheoretical Problem 1RELATIVISTIC PARTICLEIn the theory of special relativity the relation between energy E and momentum P or a free particle with rest mass m 0 is242022mc c m c p E =+=When such a particle is subject to a conservative force, the total energy of the particle, which is the sum of42022c m c p + and the potential energy, is conserved. Ifthe energy of the particle is very high, the rest energy of the particle can be ignored (such a particle is called an ultra relativistic particle).1) consider the one dimensional motion of a very high energy particle (in which rest energy can be neglected) subject to an attractive central force of constant magnitude f . Suppose the particle is located at the centre of force with initial momentum p 0 at time t =0. Describe the motion of the particle by separately plotting, for at least one period of the motion: x against time t , and momentum p against space coordinate x . Specify the coordinates of the “turning points ” in terms of given parameters p 0 and f . Indicate, with arrows, the direction of the progress of the mothon in the (p , x ) diagram. There may be short intervals of time during which the particle is not ultrarelativistic. However, these should be neglected.Use Answer Sheet 1.2) A meson is a particle made up of two quarks. The rest mass M of the meson is equal to the total energy of the two-quark system divided by c 2.Consider a one--dimensional model for a meson at rest, in which the two quarks are assumed to move along the x -axis and attract each other with a force of constant magnitude f It is assumed they can pass through each other freely. For analysis of the high energy motion of the quarks the rest mass of the quarks can be neglected. At time t=0 the two quarks are both at x =0. Show separately the motion of the two quarks graphically by a (x , t ) diagram and a (p , x ) diagram, specify the coordinates of the “turning points ” in terms of M and f , indicate the direction of the process in your (p , x ) diagram, and determine the maximum distance between the two quarks. Use Answer Sheet 2.3) The reference frame used in part 2 will be referred to as frame S , the Lab frame, referred to as S , moves in the negative x -direction with a constant velocity v =0.6c . the coordinates in the two reference frames are so chosen that the pointx =0 in S coincides with the point 0='x in S '' at time 0='=t t . Plot the motion of the two quarks graphically in a (x ', t ') diagram. Specify the coordinates of the turning points in terms of M , f and c , and determine the maximum distance between the two quarks observed in Lab frame S '. Use Answer Sheet 3.The coordinates of particle observed in reference frames S and S '' are related by the Lorentz transformation⎪⎩⎪⎨⎧+='+=')()(c x t t ct x x βγβγwhere c v /=β,21/1βγ-= and v is the velocity of frame S moving relative to the frame S ''.4) For a meson with rest energy Mc 2=140 MeV and velocity 0.60c relative to theLab frame S '', determine its energy E ' in the Lab Frame S ''.ANSWER SHEET 1 ANSWER SHEET 2 1)2)OOtOxptx 1, x 2Ox 1p 1 Ox 2p 2Quark1Quark2The maximum distance betweenthe two quarks is d =ANSWER SHEET 3 3)Theoretical Problem 1—Solution1) 1a. Taking the force center as the origin of the space coordinate x and the zero potential point, the potential energy of the particle is||)(x f x U =(1)The total energy is||42022x f c m c p W ++=.1b. Neglecting the rest energy, we get||||x f c p W +=,(2)Since W is conserved throughout the motion, so we havec p x f c p W 0||||=+=,(3)Let the x axis be in the direction of the initial momentum of the particle,cp fx pc c p fx pc c p fx pc cp fx pc 0000=--=-=+-=+⎪⎪⎭⎪⎪⎬⎫<<><<>>>.0,0;0,0;0,0;0,0p x p x p x p x (4)The maximum distance of the particle from the origin, let it be L , corresponds to p =0. It isf c p L /0=.1c. From Eq. 3 and Newton ’s law⎩⎨⎧<>-==;0,;0,x f x f F dt dp(5)we can get the speed of the particle asc dtdp f c dt dx ==, (6)tx 1′, x 2′OThe maximum distance between the two quarks observed in S ′frame is d ′=when when when wheni.e. the particle with very high energy always moves with the speed of light except that it is in the region extremely close to the points L x ±=. The time for the particle to move from origin to the point L x =, let it be denoted by τ, isf p c L //0==τ.So the particle moves to and for between L x = and L x -= with speed c and periodf p /440=τ. The relation between x and t is⎪⎪⎭⎪⎪⎬⎫≤≤-=≤≤-=≤≤-=≤≤=,43,4,32,2,2,20,τττττττt L ct x t ct L x t ct L x t ct x(7)The required answer is thus as given in Fig. 1 and Fig. 2.Fig. 12) The total energy of the two-quark system can be expressed as||||||21212x x f c p c p Mc -++=,(8)where 1x ,2x are the position coordinates and 1p , 2p are the momenta of quark 1 and quark 2 respectively. For the rest meson, the total momentum of the two quarks is zero and the two quarks move symmetrically in opposite directions, we have021=+=p p p , 21p p -=, 21x x -=.(9)Let p 0 denote the momentum of the quark 1 when it is at x =0, then we havec p Mc 022=or2/0Mc p =(10)From Eq. 8, 9 and 10, the half of the total energy can be expressed in terms of 1p and1x of quark 1:||||110x f c p c p +=,(11)just as though it is a one particle problem as in part 1 (Eq. 3) with initial momentumL= p 0/fc/f2/0Mc p =. From the answer in part 1 we get the (x , t ) diagram and (p , x ) diagram of the motion of quark 1 as shown in Figs. 3 and 4. For quark 2 the situation is similar except that the signs are reversed for both x and p ; its (x , t ) and (p , x ) diagrams are shown in Figs. 3 and 4.The maximum distance between the two quarks as seen from Fig. 3 isf Mc f c p L d //2220===. (12)Fig. 3Fig. 4a Quark1 Fig. 4bQuark23) The reference frame S moves with a constant velocity V =0.6c relative to the Lab frame S '' in the x ' axis direction, and the origins of the two frames are coincident at the beginning (0='=t t ). The Lorentz transformation between these two frames is given by:),/(),(c x t t ct x x βγβγ+='+='(13)where c V /=β, and 21/1βγ-=. With c V 6.0=, we have 5/3=β, and4/5=γ. Since the Lorenta transformation is linear, a straight line in the (x , t ) diagram2L=Mc 2/2fx 1: solid linetransforms into a straight line the (x ', t ') diagram, thus we need only to calculate the coordinates of the turning points in the frame S '.For quark 1, the coordinates of the turning points in the frames S and S ' are as follows:Frame SFrame S ' 1x 1t)(111ct x x βγ+=' )/(111e x t t βγ+=' 114345ct x +=c x t /434511+= 0 0 0L τL L 2)1(=+βγ ττβγ2)1(=+τ2L L 232=γβτγτ252=L - τ3 L L =-)13(βγττβγ3)3(=-0 τ4L L 34=γβτγτ54=where f Mc f c p L 2//20==, f Mc f p 2//0==τ.For quark 2, we have Frame SFrame S ' 2x 2t)(222ct x x βγ+=' )/(222c x t t βγ+=' 224345ct x +=c x t /434522+= 0 0 0L - τL L 21)1(-=--βγττβγ21)1(=-τ2 L L 232=γβτγτ252=L τ3 L L 27)13(=+βγττβγ29)3(=+τ4L L 34=γβτγτ54=With the above results, the (x ', t ') diagrams of the two quarks are shown in Fig. 5.The equations of the straight lines OA and OB are:t c t x '='')(1; ττβγ2)1(0=+≤'≤t ; (14a) t c t x '-='')(2;ττβγ21)1(0=-≤'≤t(14b)The distance between the two quarks attains its maximum d ' when τ21='t , thus wehave maximum distancefMc L c d 2)1(2)1(22=-=-='βγτβγ. (15)Fig. 54) It is given the meson moves with velocity V =0.6 crelative to the Lab frame, its energy measured in the Lab frame is1751408.01122=⨯=-='βMc E MeV . Grading SchemePart 1 2 points, distributed as follows:0.4 point for the shape of x (t ) in Fig. 1; 0.3 point for 4 equal intervals in Fig. 1; (0.3 for correct derivation of the formula only)0.1 each for the coordinates of the turning points A and C , 0.4 point in total; 0.4 point for the shape of p (x ) in fig. 2; (0.2 for correct derivation only)0.1 each for specification of 0p , f c p L /0=, 0p -, L - and arrows, 0.5 pointin total.(0.05 each for correct calculations of coordinate of turning points only).Part 2 4 points, distributed as follows:0.6 each for the shape of )(1t x and )(2t x , 1.2 points in total;0.1 each for the coordinates of the turning points A, B, D and E in Fig. 3, 0.8 pointin total;0.3 each for the shape of )(11x p and )(22x p , 0.6 point in total;0.1 each for 2/0Mc p =, f Mc L 2/2=, 0p -, L - and arrows in Fig. 4a andFig. 4b, 1 point in total; 0.4 point for f Mc d /2=Part 3 3 point, distributed as follows:0.8 each for the shape of )(1t x '' and )(2t x '', 1.6 points in total; 0.1 each for the coordinates of the turning points A, B, D and E in Fig. 5, 0.8 pointin total; (0.05 each for correct calculations of coordinate of turning points only).0.6 point for f Mc d 2/2='.Part 4 1 point (0.5 point for the calculation formula; 0.5 point for the numerical valueand units)Theoretical Problem 2SUPERCONDUCTING MAGNETSuper conducting magnets are widely used in laboratories. The most common form of super conducting magnets is a solenoid made of super conducting wire. The wonderful thing about a superconducting magnet is that it produces high magnetic fields without any energy dissipation due to Joule heating, since the electrical resistance of the superconducting wire becomes zero when the magnet is immersed in liquid helium at a temperature of 4.2 K. Usually, the magnet is provided with a specially designed superconducting switch, as shown in Fig. 1. The resistance r of the switch can be controlled: either r =0 in the superconducting state, or n r r = in the normal state. When the persistent mode, with a current circulating through the magnet and superconducting switch indefinitely. The persistent mode allows a steady magnetic field to be maintained for long periods with the external source cut off.The details of the superconducting switch are not given in Fig. 1. It is usually a small length of superconducting wire wrapped with a heater wire and suitably thermally insulated from the liquid helium bath. On being heated, the temperature of the superconducting wire increases and it reverts to the resistive normal state. The typical value of n r is a few ohms. Here we assume it to be 5Ω. The inductance of a superconducting magnet depends on its size; assume it be 10 H for the magnet in Fig. 1. The total current I can be changed by adjusting the resistance R . This problem will be graded by the plots only!The arrows denote the positive direction of I , I 1 and I 2.Fig. 11) If the total current I and the resistance r of the superconducting switch are controlledto vary with time in the way shown in Figs, 2a and 2b respectively, and assuming the currents I 1 and I 2 flowing through the magnet and the switch respectively are equal at the beginning (Fig. 2c and Fig. 2d), how do they vary with time from t 1 to t 4? Plot your answer in Fig. 2c and Fig. 2d2) Suppose the power switch K is turned on at time t =0 when r =0, I 1=0 and R =7.5Ω, and the total current I is 0.5A. With K kept closed, the resistance r of the superconducting switch is varied in he way shown in Fig. 3b. Plot the corresponding time dependences of I , I 1 and I 2in Figs. 3a, 3c and 3d respectively.3) Only small currents, less than 0.5A, are allowed to flow through theFig.2a2b 2c 2dFig. 3a3b 3c 3dsuperconducting switch when it is in the normal state, with larger currents the switch will be burnt out. Suppose the superconducting magnet is operated in a persistent mode, i. e. I =0, and I 1=i 1(e. g. 20A), I 2=-i 1, as shown in Fig. 4, from t =0 to t =3min. If the experiment is to be stopped by reducting the current through the magnet to zero, how would you do it? This has to be done in several operation steps. Plot the corresponding changes of I , r , I 1 and I 2in Fig. 44) Suppose the magnet is operated in a persistent mode with a persistent current of 20A (t =0 to t =3min. See Fig. 5). How would you change it to a persistent mode with acurrent of 30a? plot your answer in Fig. 5.Fig. 4a4b 4c 4dFig. 5a5b 5cTheoretical Problem 2—Solution 1) For t =t 1 to t 3Since 0=r , the voltage across the magnet dt LdI V M /1==0, therefore,011121)(I t I I ==; 01221I I I I I -=-=.For t =t 3 to t 4Since I 2=0 at t =t 3, and I is kept at 021I after3t t =, 02==n M r I V , therefore, 1I and 2I will not change.0121I I =; 02=IThese results are shown in Fig. 6.5dFig. 6a6b 6c 6d2) For 0=t to 1=t min: Since 0=r , 0/1==dt LdI V M0)0(11==I I5.012=-=I I I A.At 1=t min, r suddenly jumps from O to n r , I will drop from R E / to)/(n r R E + instantaneously, because 1I can not change abruptly due to the inductance of the magnet coil. For R E /=0.5A, Ω=5.7R and Ω=5n R . I will drop to 0.3A. For 1=t min to 2 min:I , 1I and 2I gradually approach their steady values:5.0==REI A, 5.01==I I A 02=I .The time constantnn Rr r R L )(+=τ. When 10=L H, Ω=5.7R and Ω=5n r , 3=τsec. For 2=t min to 3 min:Since 0=r , 1I and 2I will not change, that is5.01=I A and 02=IFig. 7a7b3) The operation steps are: First stepTurn on power switch K , and increase the total current I to 20 A, i. e. equal to 1I .Since the superconducting switch is in the state 0=r , so that L V M = 0/1=dt dI , that is, 1I can not change and 2I increases by 20A, in other words, 2I changes from 20- A to zero. Second stepSwitch r from 0 to n r . Third stepGradually reduce I to zero while keeping 5.02<I A: since n M r V I /2= anddt dI L V m /1=, when 10=L H, Ω=5n r , the requirement 5.02<I A corresponds to 25.0/1<dt dI A/sec, that is, a drop of <15A in 1 min. In Fig. 8 dt dI /～0.1A/sec and dt dI /1 is around this value too, so the requirement has been fulfilled. Final stepSwitch r to zero when 0=M V and turn off the power switch K . These resultsare shown in Fig. 8.7c 7dFig. 8a8b 8c4) First step and second step are the same as that in part 3, resulting in 02=I .Third step Increase I by 10 A to 30 A with a rate subject to the requirement5.02<I A. Fourth step Switch r to zero when 0=M V .Fifth step Reduce I to zero, 301=I A will not change because M V is zero.12I I I -= will change to 30- A. The current flowing through the magnet is thus closed by the superconducting switch. Final step Turn off the power switch K . The magnet is operating in the persistent mode.These results are shown in Fig. 9.Grading SchemePart 1,2 points:0.5 point for each of 1I , 2I from 1t t = to 3t and 1I , 2I from 3t t = to 4t .Part 2,3 points:0.3 point for each of 1I , 2I from 0=t to 1 min, I , 1I , 2I at 1=t min,8dFig. 9a9b 9c 9dand 0I , 1I , 2I from 1=t to 2 min;0.2 point for each of I , 1I , and 2I from 2=t to 3 min. Part 3, 2 points: 0.25 point for each section in Fig. 8 from 3=t to 9 min, 8 sections in total. Part 4,3 points:0.25 point for each section in Fig. 9 from 3=t to 12 min, 12 sections in total.Theoretical Problem 3COLLISION OF DISCS WITH SURFACE FRICTIONA homogeneous disc A of mass m and radius R A moves translationally on a smoothhorizontal x -y plane in the x direction with a velocity V (see the figure on the next page). The center of the disk is at a distance b from the x-axis. It collides with a stationary homogeneous disc B whose center is initially located at the origin of the coordinate system. The disc B has the same mass and the same thickness as A, but its radius is R B . It is assumed that the velocities of the discs at their point of contact, in the direction perpendicular to the line joining their centers, are equal after the collision. It is also assumed that the magnitudes of the relative velocities of the discs along the line joining their centers are the same before and after the collision.1) For such a collision determine the X and Y components of the velocities of the twodiscs after the collision, i. e. AXV ', AY V ', BX V ' and BY V ' in terms of m , A R , B R , V and b .2) Determine the kinetic energies A E ' for disc A and B E ' for disc B after the collision in terms of m , A R , B R , V and b .Theoretical Problem 3—Solution1) When disc A collides with disc B, let n be the unit vector along the normal to the surfaces at the point of contact and t be the tangential unit vector as shown in the figure. Let ϕ be the angle between n and the x axis. Then we haveϕsin )(B A R R b +=The momentum components of A and B along n and t before collision are:0,cos ==Bn An mV mV mV ϕ,0,sin ==Bt At mV mV mV ϕ.Denote the corresponding momentum components of A and B after collision byAnV m ', Bn V m ', At V m ', and Bt V m '. Let A ω and B ω be the angular velocities of A and B about the axes through their centers after collision, and A I and B I be their corresponding moments of intertia. Then,221A A mR I =,221B B mR I =The conservation of momentum givesBn AnV m V m mV '+'=ϕcos , (1) tn AtV m V m mV '+'=ϕsin ,(2)The conservation of angular momentum about the axis through O givesB B A A B A AtI I R R V m mVb ωω+++'=)( (3)The impulse of the friction force exerted on B during collision will cause amomentum change of AtV m ' along t and produces an angular momentum B B I ω simultaneously. They are related by.B B b BtI R V m ω=' (4)During the collision at the point of contact A and B acquires the same tangential velocities, so we haveB B Bt A A AtR V R V ωω-'=-' (5)It is given that the magnitudes of the relative velocities along the normal directionof the two discs before and after collision are equal, i. e.An BnV V V '-'=ϕcos . (6)From Eqs. 1 and 6 we get0='AnV , ϕcos V V Bn='. From Eqs. 2 to 5, we get ϕsin 65V V At=', ϕsin 61V V Bt=',A A R V 3sin ϕω=,BB R V 3sin ϕω=.The x and y components of the velocities after collision are:,)(65sin cos 22B A At An Ax R R Vb V V V +='+'='ϕϕ (7)222)(6)(5cos sin B A B A At An AyR R b R R Vb V V V +-+='+'-='ϕϕ, (8)⎥⎦⎤⎢⎣⎡+-='+'='22)(651sin cos B A Bt Bn Bx R R b V V V ϕϕ, (9)222)(6)(5cos sin B A B A Bt Bn By R R b R R Vb V V V +-+-='+'-='ϕϕ,(10)2) After the collision, the kinetic energy of disc A is222222)(8321)(21B A A A Ay Ax A R R b mV I V V m E +=+'+'='ω(11)while the kinetic energy of disc B is⎥⎦⎤⎢⎣⎡+-=+'+'='222222)(121112121)(21B A B B By Bx BR R b mV I V V m E ω (12)Grading Scheme1. After the collision, the velocity components of discs A and B are shown in Eq. 7, 8, 9 and 10 of the solution respectively. The total points of this part is 8. 0. If the result in which all four velocity components are correct has not been obtained, the point is marked according to the following rules.0.8 point for each correct velocity component;0.8 point for the correct description of that the magnitudes of the relative velocities of the discs along the line joining their centers are the same before and after the collision.0.8 point for the correct description of the conservation for angular momentum;0.8 point for the correct description of the equal tangential velocity at the touching point;0.8 point for the correct description of the relation between the impulse and the moment of the impulse.2. After the collision, the kinetic energies of disc A and disc B are shown in Eqs. 11 and 12 of the solution respectively.1.0 point for the correct kinetic energies of disc A;1.0 point for the correct kinetic energies of disc B;The total points of this part is 2.0XXV INTERNATIONAL PHYSICS OLYMPIADBEIJING, PEOPLE’S REPUBLIC OF CHINAPRACTICAL COMPETITIONJuly 15, 1994Time available: 2.5 hoursREAD THIS FIRST!INSTRUCTIONS:1. Use only the ball pen provided.2. Your graphs should be drawn on the answer sheets attached to the problem.3. Write your solution on the marked side of the paper only.4. The draft papers are provided for doing numerical calculations and draft drawings.5. Write at the top of every page:●The number of the problem●The number of the page of your report in each problem●The total number of pages in your report to the problem●Your name and code numberEXPERIMENTAL PROBLEM 1Determination of light reflectivity of a transparent dielectric surface.Experimental Apparatus1. He-Ne Laser(～1.5mW).The light from this laser is not linearly polarized.2. Two polarizers (P1, P2) with degree scale disk (Fig. 1), one (P1) has been mounted in front of the laser output window as a polarizer, and another one can be fixed in a proper place of the drawing board by push-pins when it is necessary.3. Two light intensity detectors (D1, D2) which consisted of a photocell and a microammeter (Fig. 2).4. Glass beam splitter(B).5. Transparent dielectric plate, whose reflectivity and refractive index are to be determined.6. Sample table mounted on a semicircular degree scale plate with a coaxial swivel arm(Fig. 3).7. Several push-.pins for fixing the sample table on the drawing board and as its rotation axis.8. Slit aperture and viewing screen for adjusting the laser beam in the horizontal direction and for alignment of optical elements.9. Lute for adhere of optical elements in a fixed place.10. Wooden drawing board.11. Plotting papersExperiment Requirement1. Determine the reflectivity of the p-component as a function of the incident angle(the electric field component, parallel to the plane of incidence is called the p-component).(a) Specify the transmission axis of the polarizer (A) by the position of the markedline on the degree scale disk in the p-componet measurement(the transmission axis is the direction of vibration of the electric field vector of the transmitted light).(b) Choose any one of the light intensity detector and set its micro-ammeter at therange of "×5". Verify the linear relation ship between the light intensity and the micro-ammeter reading. Draw the optical schematic diagram. Show your measured data and calculated results(including the calculation formula)in the farm of a table. Plot the linear relationship curve.(c) Determine the reflectivity of the p -component as a function of the incident angle. Draw the optical schematic diagram. Show your measured data and calculated reflectivity(including the calculation formula)in the form of a table. Plot the reflectivity as a function of the incident angle.2. Determine the refractive index of the sample as accurate as possible. Explanation and Suggestion1. Laser radiation avoid direct eye exposure.2. Since the output power of the laser beam may fluctuate from time to time, the fluctuation of light output has to be monitored during the performance of the experiment and a correction of the experimental results has to be made.3. The laser should be lighting all the time, even when you finish your experiment and leave the examination hall, the laser should be keeping in work.4. The reflected light is totally plane polarized at an incident angle B θ while tg B θn = (refractive index).Fig. 1 polarizers with degree scale diskFig. 2 Light intensity detector(1) Insert the plug of photocell into the “INPUT” socket of microammeter (2) Switching on the microammeter.(3) Blocd off the light entrance hole in front of the photocell and adjust the scale reading of micro ammeter to “0”.(4) Set the “Multiple” knob to a proper range.Fig.3 Sample table mounted on a semicircular degree scale plateExperimental Problem 1——Solution1. (a) Determine the transmission axis of the polarizer and the Brewster angle B θ ofthe sample by using the fact that the rerlectivity of the p -component 0=p R at the Brewster angle.Change the orientation of the transmission axis of 1P , specified by the position of the marked line on the degree scale disk (ψ) and the incident angle (i θ) successively until the related intensity 0=r I .Now the incident light consists of p -component only and the incident angle is B θ, thecorresponding values 1ψ and B θ are shown below:︒±︒=5.05.1401ψ or 322.3°±0.1°The Brewster angle B θ is 56.3°±0.1° 1. (b) Verification of the linear relationship between the light intensity and themicroammenter reading.The intensity the transmitted light passing through two polarized 1P and 2Pobeys Malus ’ lawθθ20cos )(I I =where 0I is the intensity of the light polarized by 1p and incident, I is the intensity of the transmitted light, and θ is the angle between the transmission axes of1P and 2p . Thus we can obtain light with various intensities for the verification by using two polarizers. The experimental arrangement is shown in the figure.The light intensity detector 1D serves to monitor the intensity fluctuation of theincident beam (the ratio of 1I to 2I remain unchanged), and 2D measures 2I . Let)(1θi and )(2θi be the readings of 1D and 2D respectively, and )(2θψ be the reading of the marked line position. 02=i when 90=θ°, the corresponding 2ψ is 2ψ(90°), and the value of θ corresponding to 2ψ is|90)90(|22︒±︒-=ψψθData and results;︒=︒4)90(2ψFrom the above data we can obtain the values of )(/)(2θθI I from the formula)0()0()()()(21120i i i i I I ⋅=θθθ and compare them with θ2cos for examining the linear relationship. The results obtained are:1. (c) Reflectivity measurementThe experimental arrangement shown below is used to determine the ratio of 0Ito 1I which is proportional to the ratio of the reading )(20i of 2D to the corresponding reading )(10i of 1D .Then used the experimental arrangement shown below to measure the relativityp R of the sample at various incident angle )(θ while the incident light consists of p -component only. Let )(1θi and )(2θi be the readings of 1D and 2Drespectively.Then the reflectivity is2010120)()()()(i i i i I I R p ⋅==θθθθ Data and results:Ai A i μμψ3.1358.195.14010201=⨯=︒=。
奥林匹克物理竞赛试题及答案
奥林匹克物理竞赛试题及答案国际奥林匹克物理竞赛是国际中学生的物理大赛，高中同学可以用来提升物理解题能力。
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奥林匹克物理竞赛试题国际物理奥林匹克竞赛简介竞赛设立由参赛成员国组成的国际物理奥林匹克委员会。
竞赛章程规定：目的是为增进中学物理教学的国际交流，通过竞赛促进开展物理学科的课外活动，以加强不同国家青年之间的友好关系和人民间的相互了解合作。
同时帮助参赛者发展物理方面的创造力，把从学校学到的知识用于解决实际问题的能力。
国际物理奥林匹克竞赛每年举办一次。
由各会员国轮流主办，并由各代表团团长和一名主办国指定的主席组成国际委员会。
国际委员会的任务是公平合理地评卷，监督章程规定的执行情况，决定竞赛结果。
每一会员国可选派5名高中学生或技术学校学生参加竞赛。
参加者的年龄到竞赛开始的那一天不能超过20岁。
参赛代表队要有2名团长，2名团长是国际委员会的成员，条件是能胜任解答赛题，能参加竞赛试卷的讨论和评分工作，并能通晓一种国际物理奥林匹克的工作语言。
国际物理奥林匹克的工作语言是英文、法文、德文和俄文。
代表团到达主办国时，团长要将参加学生及团长的情况告诉主办国家组织人员。
竞赛于每年6月底举行。
竞赛分两天进行。
第一天进行3道理论计算题竞赛，另一天的竞赛内容是1—2道实验题。
中间有一天的休息。
参赛者可使用计算尺、不带程序编制的计算器和对数表、物理常数表和制图工具，但不能使用数学和物理公式一览表。
竞赛题由参加国提供题目，主办国命题。
在竞赛前，赛题要保密。
竞赛题内容包括中学物理的4个部分(力学、热力学和分子物理学、光学及原子和核物理学、电磁学) ，解题要求用标准的中等数学而不要用高等数学。
主办国提出评卷标准并指定评卷人。
每题满分为10分。
各代表团团长同时对自己团员竞赛卷的复制品进行评定，最后协商决定成绩。
评奖标准是以参赛者前三名的平均分数计为100%，参赛者达90% 以上者为一等奖，78—90%者为二等奖，65—78%者为三等奖，同时发给证书。
国际物理奥林匹克竞赛试题.doc
国际物理奥林匹克竞赛试题理论试题题1A 某蹦迪运动员系在一根长弹性绳子的一端，绳的另一端固定在一座高桥上，他自静止高桥向下面的河流下落，末与水面相触，他的质量为m，绳子的自然长度为L，绳子的力常数（使绳子伸长lm所需的力）为k，重力场强度为g。
求出下面各量的表达式。
（a）运动员在第一次达到瞬时静止前所落下的距离y。
（b）他在下落过程中所达到的最大速率v。
（c）他在第一次达到瞬时静止前的下落过程所经历的时间t。
设运动员可以视为系于绳子一端的质点，与m相比绳子的质量可忽略不计，当绳子在伸长时服从胡克定律，在整个下落过程中空气的阻力可忽略不计。
B 一热机工作于两个相同材料的物体之间，两物体的温度分别为T A和T B（T A＞T B），每个物体的质量均为m，比热恒定，均为s。
设两个物体的压强保持不变，且不发生相变。
（a）假定热机能从系统获得理论上允许的最大机械能，求出两物体A和B最终达到的温度T?的表达式，给出解题全部过程。
（b）由此得出允许获得的最大功的表达式。
（c）假定热机工作于两箱水之间，每箱水的体积为2.50m3，一箱水的温度为350K，另一箱水的温度为300K。
计算可获得的最大机械能。
已知水的比热容= 4.19×103kg-1K-1，水的密度=1.00 x 103kgm.-3C 假定地球形成时同位素238U和235U已经存在，但不存在它们的衰变产物。
238U和235U的衰变被用来确定地球的年龄T。
（a）同位素238U以4.50×109年为半衰期衰变，衰变过程中其余放射性衰变产物的半衰期比这都短得多，作为一级近似，可忽略这些衰变产物的存在，衰变过程终止于铅的同位素206Ph。
用238U的半衰期、现在238U的数目238N表示出由放射衰变产生的206Pb原子的数目206n。
（运算中以109年为单位为宜）（b）类似地，235U在通过一系列较短半衰期产物后，以0.710×109年为半衰期衰变，终止于稳定的同位素207Pb。
物理奥赛初赛试题及答案
物理奥赛初赛试题及答案一、选择题（每题5分，共20分）1. 光在真空中的传播速度是：A. 3×10^8 m/sB. 3×10^5 m/sC. 3×10^6 m/sD. 3×10^7 m/s答案：A2. 根据牛顿第二定律，力和加速度的关系是：A. F = maB. F = ma^2C. F = m/aD. F = a/m答案：A3. 以下哪个选项是正确的能量守恒定律表述？A. 能量可以被创造B. 能量可以被消灭C. 能量既不能被创造也不能被消灭D. 能量可以在不同形式之间转换答案：C4. 根据库仑定律，两个点电荷之间的力与它们之间的距离的关系是：A. 与距离成正比B. 与距离成反比C. 与距离的平方成正比D. 与距离的平方成反比答案：D二、填空题（每题5分，共20分）5. 一个物体在水平面上以初速度v0开始滑行，摩擦系数为μ，滑行距离为s，则物体滑行时间t为______。
答案：t = v0 / (μg)6. 一个质量为m的物体从高度h自由落下，忽略空气阻力，其落地时的速度v为______。
答案：v = √(2gh)7. 一个电路中，电阻R、电流I和电压V之间的关系是______。
答案：V = IR8. 根据欧姆定律，电阻R、电流I和电压V之间的关系是______。
答案：I = V / R三、计算题（每题10分，共40分）9. 一辆汽车以恒定加速度a从静止开始加速，经过时间t后，汽车的速度v和位移s分别为多少？答案：v = ats = 1/2 * a * t^210. 一个质量为m的物体从高度h自由落下，求物体落地时的动能。
答案：动能 = 1/2 * m * v^2 = 1/2 * m * (2gh) = mgh11. 一个电阻R与一个电容C串联后接在电压为V的直流电源上，求电路达到稳态时的电流I。
答案：I = V / (R + 1/(C * ω))12. 一个质量为m的物体在弹簧的弹力作用下做简谐振动，弹簧的劲度系数为k，求物体的最大速度。
奥林匹克物理竞赛题
选择题：
一个物体在自由落体过程中，其动能与势能之和如何变化？
A. 逐渐增加
B. 逐渐减少
C. 保持不变（正确答案）
D. 无法确定
在一个完全弹性碰撞中，两个物体的总动能会如何变化？
A. 增加
B. 减少
C. 保持不变（正确答案）
D. 可能增加也可能减少
当一束光从空气射入水中时，其速度会如何变化？
A. 增加
B. 减少（正确答案）
C. 保持不变
D. 变为零
在一个电路中，如果电阻增加，那么电流会如何变化？
A. 增加
B. 减少（正确答案）
C. 保持不变
D. 变为零
一个物体在真空中自由下落，其加速度会如何？
A. 逐渐增大
B. 逐渐减小
C. 保持不变（正确答案）
D. 变为零
当一个物体受到与其运动方向相反的恒力作用时，其速度会如何变化？
A. 逐渐增大
B. 逐渐减小（正确答案）
C. 保持不变
D. 变为零后反向加速
在一个闭合电路中，如果电源电压增加，那么电路中的电流会如何变化？
A. 增加（正确答案）
B. 减少
C. 保持不变
D. 无法确定
当一束光线从玻璃射入空气时，其临界角是多大？
A. 0度
B. 45度
C. 90度（正确答案）
D. 取决于玻璃和空气的折射率
在一个简谐振动中，物体的动能和势能之和如何变化？
A. 逐渐增加
B. 逐渐减少
C. 保持不变（正确答案）
D. 周期性变化。
历届奥林匹克物理竞赛试题及解答
历届国际物理奥林匹克竞赛试题与解答第１届（1967年于波兰的华沙）【题１】质量Ｍ＝0.2kg 的小球静置于垂直柱上，柱高ｈ＝5m 。
一粒质量ｍ＝0.01kg 、以速度0＝500m/s 飞行的子弹水平地穿过球心。
球落在距离柱s ＝20m 的地面上。
问子弹落在地面何处？子弹动能中有多少转换为热能？解：在所有碰撞情况下，系统的总动量均保持不变：MV mv mv +=0其中v 和V 分别是碰撞后子弹的速度和小球的速 度. 两者的飞行时间都是01.12==ght s 球在这段时间沿水平方向走过20m 的距离，故它在水平方向的速度为：8.1901.120==V （m/s ） 由方程0.01×500＝0.01v ＋0.2×19.8 可求出子弹在碰撞后的速度为：v ＝104m/s子弹也在1.01s 后落地，故它落在与柱的水平距离为S ＝vt ＝104×1.01＝105m 的地面上。
碰撞前子弹的初始动能为=2021mv 1250 J 球在刚碰撞后的动能为=221MV 39.2 J 子弹在刚碰撞后的动能为=221mv 54 J与初始动能相比，两者之差为1250 J －93.2 J ＝1156.8 J这表明原来动能的92.5%被系统吸收而变为热能。
这种碰撞不是完全非弹性碰撞。
在完全弹性碰撞的情形下，动能是守恒的。
而如果是完全非弹性碰撞，子弹将留在球内。
【题2】右图（甲）为无限的电阻网络，其中每个电阻均为r ，求Ａ、Ｂ两点间的总电阻。
解：如图（乙）所示Ａ、Ｂ两点间的总电阻应等于Ｃ、Ｄ两点间的总电阻与电阻ｒ的并联，再与ｒ串联 图（甲） 后的等效电阻。
如果网络是无限的，则Ａ、Ｂ两点间的总电阻应等于Ｃ、Ｄ 两点间的总电阻，设为Ｒx 。
根据它们的串并联关系有：m M h SsυABr r r r r r r rA B r r r r r r r r ＣＤrR rR r R x xx ++= 图（乙） 解上式可得： r R x 251+=【题3】给定两个同样的球，其一放在水平面上，另一个以细线悬挂。
物理竞赛初赛试题及答案
物理竞赛初赛试题及答案一、选择题（每题4分，共40分）1. 光在真空中的传播速度是（）。
A. 299,792,458 m/sB. 299,792,458 km/hC. 299,792,458 m/hD. 299,792,458 km/s答案：A2. 牛顿第二定律的表达式是（）。
A. F = maB. F = mvC. F = m/aD. F = ma^2答案：A3. 根据热力学第一定律，系统内能的增加量等于（）。
A. 系统吸收的热量B. 系统对外做的功C. 系统吸收的热量减去对外做的功D. 系统吸收的热量加上对外做的功答案：D4. 一个物体在水平面上受到一个恒定的力，使其做匀加速直线运动。
若力的大小为10N，物体的质量为2kg，那么物体的加速度是（）。
A. 5 m/s^2B. 10 m/s^2C. 20 m/s^2D. 4 m/s^2答案：A5. 电磁波的波速在真空中是（）。
A. 299,792,458 m/sB. 300,000,000 m/sC. 3.00 x 10^8 m/sD. 3.00 x 10^5 km/s答案：C6. 一个电阻为10Ω的电阻器，通过它的电流为2A，那么电阻两端的电压是（）。
A. 20VB. 10VC. 5VD. 4V答案：A7. 根据欧姆定律，电流I与电压V和电阻R之间的关系是（）。
A. I = V/RB. I = VRC. I = V + RD. I = V - R答案：A8. 一个物体从静止开始自由下落，忽略空气阻力，其下落的加速度是（）。
A. 9.8 m/s^2B. 10 m/s^2C. 9.7 m/s^2D. 10.1 m/s^2答案：A9. 根据能量守恒定律，一个物体的动能和势能之和在没有外力作用下是（）。
A. 增加B. 减少C. 保持不变D. 无法确定答案：C10. 一个物体在水平面上受到一个恒定的力，使其做匀速直线运动。
若力的大小为10N，物体的质量为2kg，那么物体的加速度是（）。
历届IPho试题-历届IPho试题-IPhO-37ThCovermand
第37届国际奥林匹克物理竞赛
理论考试
（2006年7月10日，星期一，新加坡）
考试须知:
1.本场考试时间为5小时。
共有3题，每题10分。
2.只能使用考场所提供的笔。
3.只能使用考场所提供的纸张的正面。
4.不同的题目不要在同一张演算纸(Writing Sheets)上解答。
5.请在答卷纸(Answer Script)上答题。
另外还提供演算纸(Writing Sheets)。
根据
题中给出的数据，数值答案请保留正确的有效位数。
不要忘记写物理单位。
6.在演算纸上，写下解题所必需的步骤、内容，并标明希望考官批改的部分。
书
写时，希望用尽可能少的文字，只需提供公式、数值、符号和图表等。
7.请务必在所使用的每张答卷纸和演算纸上指定的方框内，填上国家号和学生
号；在所使用的每张演算纸上，填上题号、演算纸页码号和每题所使用的演算纸总数，以便考官批改。
此外，你可将题号和小题号写在空白纸张的顶部。
如果你不希望某张演算纸上的草稿被批改，请在不要的纸上画一个大叉，且不要把它算在演算纸的总页数内，亦不要编写页码。
8.考试结束时，请将所有答卷纸和演算纸按顺序整理，即每题答卷纸在前，希望
批改的演算纸随后，不希望批改的演算纸其次，未使用的纸张和印刷的考题放在最后。
将所有纸张按题号顺序放置，用所提供的夹子把它们夹好，留在桌面上。
不得把所提供的任何纸张携带出考场。
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moves on the plane without slipping. The free fall acceleration is .
Part B (3 points)
= ,
(A.10)
since it does not slide over the plane.
Solving (A.8)-(A.10) results in velocities at the lowest point of the puck trajectory written as
=2
the equations of motion. It is written for the puck as follows
= sin ,
(A.1)
where is the horizontal projection of the puck acceleration.
For the cylinder the equation of motion with the
Consider the forces acting on the puck and the cylinder and
depicted in the figure on the right. The puck is subject to the
gravity force and the reaction force from the cylinder . The
bubble is found as
= + ,
(B.1)
where the molar heat capacity at arbitrary process is as follows
1
= = + .
(B.2)
Here stands for the molar heat capacity of the gas at constant volume, designates its pressure, is the
(A.3)
Then the equation of rotational motion around the center of mass of the cylinder takes the form
= ,
(A.4)
where the inertia moment of the hollow cylinder is given by
capacitor of capacitance 2 carries the electric charge 0 , a capacitor of
capacitance is uncharged, and there are no electric currents in both coils of
2
surface, caused by surface tension of the interface between liquid and gas, so that ∆ = .
Part C (3 points)
Initially, a switch is unshorted in the circuit shown in the figure on the right, a
bubble. Assume that the thermal equilibrium inside the bubble is reached much faster than the period of
oscillations.
Hint: Laplace showed that there is pressure difference between inside and outside of a curved
total amount of moles of gas in the bubble, and denote the volume and temperature of the gas,
respectively.
Evaluate the derivative standing on the right hand side of (B.2). According to the Laplace formula,
= +
(A.14)
and the acceleration
2
rel = rel
.
(A.15)
At the lowest point of the puck trajectory the acceleration of the cylinder axis is equal to zero,
=
,
(A.12)
(2+ )
(2+ )
ቤተ መጻሕፍቲ ባይዱ
.
(A.13)
In the reference frame sliding progressively along with the cylinder axis, the puck moves in a circle
of radius and, at the lowest point of its trajectory, have the velocity
formula for the frequency of the small radial oscillations of the bubble and evaluate it under the
assumption that the heat capacity of the soap film is much greater than the heat capacity of the gas in the
the gas pressure inside the bubble is defined by
4
= ,
(B.3)
thus, the equation of any equilibrium process with the gas in the bubble is a polytrope of the form
the plane as shown in the figure on the left. Find the interaction force
between the puck and the cylinder at the moment when the puck passes
the lowest point of its trajectory. Assume that the friction between the
(A.7) after integrating that
= 2.
(A.8)
It is obvious that the conservation law for the system is written as
2
2
2
= 2 + 2 + 2 ,
(A.9)
where the angular velocity of the cylinder is found to be
inductance and 2, respectively. The capacitor starts to discharge and at the
moment when the current in the coils reaches its maximum value, the switch is
acceleration is found as
= sin − .
(A.2)
Since the cylinder moves along the plane without sliding its
angular acceleration is obtained as
= /
therefore, the puck acceleration in the laboratory reference frame is also given by (A.15).
2
− = .
then the interaction force between the puck and the cylinder is finally found as
cylinder is subject to the gravity force , the reaction force from
the plane 1 , the friction force and the pressure force from the
puck ′ = −. The idea is to write the horizontal projections of
g
= 1.10 3 . 1) Find formula for the molar heat capacity of the gas in the bubble for such a process when
cm
the gas is heated so slowly that the bubble remains in a mechanical equilibrium and evaluate it; 2) Find
= 3 1 + 3 .
(A.16)
(A.17)
Theoretical competition. Tuesday, 15 July 2014
2/4
Part B