2011年泛珠三角及中华名校物理奥林匹克邀请赛试题及答案

2011 年泛珠三角及中华名校物理奥林匹克邀请赛

Pan Pearl River Delta Physics Olympiad 2011

Pan Pearl River Delta Physics Olympiad 2011 2011 年泛珠三角及中华名校物理奥林匹克邀请赛 Part-1 (Total 6 Problems) 卷-1（共 6 题） (9:00 am – 12:00 pm, 02-10-2011) Math hints 数学提示: (1 + x)α ≈ 1 + α x for x << 1, ∫ x n dx =

1 n +1 x , n ≠ ?1 . n +1

Q1 (8 points) 题 1（8 分） (a) A compound pendulum consists of a uniform rigid rod of mass m and length L and a small ball of mass m attached to the end of the rod, as shown in the figure. The upper end of the rod is attached to the joint on the ceiling about which the rod can rotate freely. Find the simple harmonic oscillation frequency of the pendulum. (4 points) 如图，一均匀硬杆，质量为 m，长度为 L，上端以光滑铰链系在 天花板上，下端有一质量也为 m 的小球。求系统的简谐振动频率。 （4 分）

(b) Two point charges q and 2q are fixed on a smooth horizontal rail separated by a distance L. A small cart carrying charge q and with mass m can move freely on the rail, as shown in the figure. Find the q q 2q simple harmonic oscillation frequency of the cart. (4 points) 如图，两个点电荷 q 和 2q 分别固定在长为 L 的水平光滑导轨的两端。一质量为 m 的小车，带电 q，可在导轨上自由滑行。求小车的简谐振动频率。 （4 分）
Q2 (9 points) 题 2（9 分） The mass of an electron at rest, in the unit of energy using the mass-energy equivalence relation, is 0.511 × 106 eV, or 0.511 MeV, and eV is electron-Volt. Find the momentum of an electron, in the unit of MeV/c (c is the speed of light in vacuum) and keep only two digits, when its kinetic energy is (i) 1.0 × 10-6 MeV, (ii) 1.0 MeV, and (iii) 1.0 × 106 MeV. 一静止电子的质量，若以质量-能量的等价关系而用能量为单位，为 0.511 × 106 eV, 或 是 0.511 MeV。eV 是电子伏特的缩写。求电子有以下动能时的动量。（以 MeV/c 为单 位， c 是真空中的光速。保留 2 位有效数字。）(i) 1.0 × 10-6 MeV, (ii) 1.0 MeV, and (iii) 1.0 × 106 MeV。 Q3 (8 points) 题 3（8 分） (a) Find the capacitance per unit length between a pair of parallel cylindrical conductors with radius R and separated by a distance d (>> R), as shown in Fig. a. (b) A cylindrical conductor with radius R is placed at a distance d (>> R) above a grounded conductor plate, as shown in Fig. b. Find the capacitance per unit length between the two conductors.

d R (a)

R d (b)

(a) 如图a，两平行圆柱形导体半径为R，间距为d (>> R)。求单位长度两导体之间的电 容。 (b) 如图b，一圆柱形导体半径为R，离一接地导体板距离为d (>> R)。求单位长度 两导体之间的电容。
1

2011 年泛珠三角及中华名校物理奥林匹克邀请赛

Pan Pearl River Delta Physics Olympiad 2011

Q4 (10 points) 题 4（10 分） This problem demonstrates why the energy density of gravitational field is negative. 本题演示为何重力场的能量密度是负的。

(a)

First, consider two large parallel flat sheets separated by a distance D, one carrying uniform electric charge area density σ, and the other carrying –σ. 首先考虑两块平行大薄板，板之间的间距为 D，一板带均匀面电荷σ，另一板带 均匀面电荷–σ。 (i) Find the electric force from one sheet exerted on a unit area of the other sheet. (1 point) 求一板对另一板单位面积的作用力。（1 分） (ii) Find the electric field E near the sheets. (1 point) 求板附近的电场 E。（1 分） (iii) Assume the total area of a plate is A. Let the separation distance D decrease by a small amount δ D . Find the work done by the electric force. (1 point) 设板的面积为 A。令板的间距 D 减少一小量 δ D ，求电场作的功。（1 分） (iv) Using the answer in (iii), find the energy density of the electric field and express the energy density in terms of E. (2 point) 利用(iii)的答案， 求电场的能量密度，并以电场 E 来表达。（2 分）

(b) Now, consider two neutral parallel flat sheets of uniform area mass density σ separated by a distance D. 现在考虑两块中性平行大薄板，板之间的间距为 D，质量面密度为σ。 (i) Find the gravitational force from one sheet exerted on a unit area of the other sheet. (1 point) 求一板对另一板单位面积的引力。（1 分） (ii) Find the gravitational field g near the sheets. (1 point) 求板附近的引力场 g。（1 分） (iii) Assume the total area of a plate is A. Let the separation distance D decrease by a small amount δ D . Find the work done by the gravitational force. (1 point) 设板的面积为 A。令板的间距 D 减少一小量 δ D ，求引力场作的功。 （1 分） (iv) Using the answer in (iii), find the energy density of the gravitational field and express the energy density in terms of g. (2 points) 利用(iii)的答案， 求引力场的能量密度，并以引力场 g 来表达。 （2 分）
Q5 (5 points) 题 5（5 分） A ‘magic’ transparent sheet can be placed onto the screen of a notebook computer to prevent peeping at large angles. Give a brief explanation of a possible working principle of such sheet. 将一‘神奇’透明膜贴在手提电脑的屏幕上，就可防止旁边的人 偷看。试给出一个‘神奇’透明膜的工作原理。

Please turn to the next page 请转下页 2

2011 年泛珠三角及中华名校物理奥林匹克邀请赛

Pan Pearl River Delta Physics Olympiad 2011

Q6 (10 points) 题 6（10 分） The operation of an internal combustion engine in automobiles can be modeled by the following four-stroke cycle in the pressure-volume (P-V) diagram as shown in the figure: A) Adiabatic compression from V1 to V2. B) Heating raising the temperature from T1 to T2 at constant volume. C) Adiabatic expansion from V2 to V1, producing mechanical work. D) Cooling at constant volume lowering the temperature from T3 to T4. Let n be the number of moles of gas operated in a cycle, CV and CP be the molar specific heat of the gas at constant volume and constant pressure, respectively. Also let γ = CP/CV. (a) Express the temperature ratios T2/T3 and T1/T4 in terms of the volume ratio V1/V2. (2 points) (b) Let Q be the heat absorbed by the gas in the heating stroke, and W1 and W3 be the work done by the gas in the compression and expansion strokes respectively. Calculate the ratios W1/Q and W3/Q. (6 points) (c) Find the efficiency of the engine in terms of V1, V2, and γ. (2 points)
P

B C

A V2 V1

D V

《THE END 完》

3

2011 年泛珠三角及中华名校物理奥林匹克邀请赛

Pan Pearl River Delta Physics Olympiad 2011

Pan Pearl River Delta Physics Olympiad 2011 2011 年泛珠三角及中华名校物理奥林匹克邀请赛 Part-2 (Total 3 Problems) 卷-2（共 3 题） (2:30 pm – 5:30 pm, 02-10-2011) Math hints 数学提示: Q1 (a)
α ∫ cos( x)dx = sin( x) ; (1 + x) ≈ 1 + α x for x << 1.

(b)

(c)

Neutrino Oscillation (15 points) 题 1 中微子振荡（15 分） Neutrinos are very light particles with masses below 10 eV. Estimate the speed of a neutrino with total energy of 108 eV in the unit of the speed of light in vacuum c. (3 points) 中微子是具有很小质量（10 电子伏以下）的粒子。估算一个总能量为 108 电子伏的中微 子的速度（以真空中光速 c 为单位）。（3 分） Neutrinos have one fascinating property that no other particles have, namely they keep changing continuously from one type to another and changing back as time goes by. For example, an electron neutrino (state-1) will change to a muon neutrino (state-2) and change back over a time period of T. Its mass will change from m1 in state-1 to m2 in state-2. This phenomenon is called neutrino oscillation. Quantum mechanics says that the period T is h determined by T = , where E1 and E2 are the total energy of the neutrino in state-1 and | E1 ? E2 | state-2, respectively, | E2 ? E1 | is the absolute value of the energy difference, and h is the Planck constant. For a neutrino of fixed momentum p, find T in terms of m1, m2, h, p, and c. (7 points) 中微子有个很有趣的独特性质。随着时间的流逝，它可以逐渐从一种中微子变成另一种 中微子，再逐渐变回原来的中微子，周而复始，永不停止。比如，电子中微子（状态1）可以逐渐变成渺子中微子（状态-2），再逐渐变回成电子中微子。这一现象称为中微 子振荡。一个循环所需的时间，即振荡周期，为 T。根据量子力学，振荡周期为 h ，其中 E1 和 E2 分别为中微子在状态-1 和状态-2 的总能量， | E2 ? E1 | 是两者 T= | E1 ? E2 | 之差的绝对值，h 为普郎克常数。若中微子的动量 p 为恒定值，m1、m2、h、p、c 为已 知，求振荡周期 T。（7 分） Suppose electron neutrinos with energy of 108 eV change to muon neutrinos after traveling through the Earth, (You need to recall roughly the order of magnitude of the Earth diameter.) 2 estimate the minimum value | m12 ? m2 | in the unit of (eV)2. You may find the constant

hc = 1.24 ×10?6 eV ? m useful. (5 points) 若能量为 108 电子伏的电子中微子在穿过地球的过程中变成了渺子中微子，估求 2 | m12 ? m2 | 的最小值（以(电子伏)2 为单位）。你需要自己给出地球直径的近似值，并可能

(a) The path of light bent by gravitational field is an effect of General Relativity. However, one can analysis such phenomenon and obtain an approximate answer using Newtonian mechanics by assuming that a light beam is made of photons traveling at speed c, with the effective mass of each photon being equal to m = E / c 2 , where E is the energy of the photon. Let us first consider the case of a classical particle flying by a fixed point mass M at high initial speed v. The trajectory of the particle

1

2011 年泛珠三角及中华名校物理奥林匹克邀请赛

Pan Pearl River Delta Physics Olympiad 2011

will be bent due to the gravity of the point mass. Because of the high speed of the particle, the bending angle is very small and can be approximately calculated in the following way. 根据广义相对论，光线在引力场里会弯曲。若把光束看作是以光速 c 运动的具有能量 E 的光子，并赋予光子有效质量 m = E / c 2 ，则此现象也可以用牛顿力学来解释，并得到近似的答 案。首先，我们考虑一初始速度 v 很高的经典粒子，飞过一质量为 M 的固定质点。由于引力作 用，粒子的轨迹会弯曲。但由于粒子的初速度很高，弯曲的角度很小，因此可用以下的近似方 法求得。 (i) Assume that the trajectory of the particle remains straight, as if the point mass was not there. The distance from the trajectory to the fixed point mass is b, as shown in the figure. Calculate the total impulse the particle receives from the point mass as it travels from the far left to the far right in terms of M, b, G the universal gravity constant, and m the mass of the particle. You may find it easier to use the angle θ as the integration variable. (4 points)

θ

M

(ii)

(b) The angular distance of two stars in the sky happens to be the same as the sun’s angular diameter. 天空中有两颗星的角距离刚好和太阳的角直径一样。 (i) The sun-earth distance is 1.5 × 1011 m, and the sun’s diameter is 1.4 × 109 m. Calculate the sun’s angular diameter in the sky. (1 point) 已知日-地距离为 1.5 × 1011 米，太阳的直径为 1.4 × 109 米。求太阳的角直径。（1 分） (ii) When the sun happens to be right between the two stars in the sky, the Apparent Position stars appear to be ‘pushed outwards’ by the sun, as shown in the figure. Draw a diagram to briefly explain the phenomenon. (2 points) 当太阳刚好位于这两颗星的中间时，两颗星好象从它们原来的位置 (Original Position) 被推到现在观察到的视觉位置(Apparent Position)。 作简图解释此现象。（2 分） (iii) Calculate the apparent angular distance between the two stars in (ii). The Original Position mass of the sun is 2.0 × 1030 kg. The speed of light in vacuum is c = 3.0 ×108 m / s . The universal gravity constant is G = 6.67 ×10?11 N ? m 2 / kg 2 . (5 points) 求(ii)中观察到的两星之间的视觉角距离。已知太阳质量为 2.0 × 1030 kg，真空光速为 c = 3.0 ×108 m / s ，引力常数为 G = 6.67 ×10?11 N ? m 2 / kg 2 。（5 分） (iv) With the present technology, why the phenomenon in (ii) can only be observed during a total solar eclipse? (1 point) 为何上述现象用现有的技术只有在日全食时才能观察到？（1 分） (v) If the moon’s orbit size were doubled, could we still observe total solar eclipse? (1 point) 若月球的轨道半径为现在的两倍，还会有日全食现象吗？（1 分）

2

2011 年泛珠三角及中华名校物理奥林匹克邀请赛

Pan Pearl River Delta Physics Olympiad 2011

Q3

Magnetic monopoles (20 points)

The uniqueness theorem of the theory of electric and magnetic fields ensures that virtual (image) charges could be placed outside the closed space in which the fields are to be determined to mimic the original boundary conditions. The fields in the closed space are then the same as the ones generated by the real charges inside the space and the virtual charges outside the space. For an interface without G free charge and free electric current, the boundary conditions for electric field E , electric G G G G G G G ⊥ G ⊥ G ⊥ G // G // displacement D , magnetic field B , and auxiliary field H are E1/ / = E2/ / , D1⊥ = D2 , B1 = B2 , H1 = H 2 . Here ‘ ⊥ ’means the components perpendicular to the interface, and ‘//’ means the components parallel to the interface. 利用电、磁场理论的唯一性定理，我们可在一闭合空间外用虚拟电荷分布来产生和原来相同的 边界条件，并用这些虚拟电荷分布和空间内原来的电荷分布求出闭合空间内的电、磁场。在一 G G G G 个无自由电荷、自由电流的界面，电场 E 、电位移矢量 D 、磁场 B 、磁辅助场 H 的边界条件 G G G G ⊥ G ⊥ G ⊥ G // G // , B1 = B2 , H1 = H 2 。这里‘ ⊥ ’、‘//’分别代表垂直、平行于界面的分 分别为 E1/ / = E2/ / , D1⊥ = D2 量。 (a) Consider the case of a point charge q inside medium-1 at a distance d from the x 2 1 interface between two ordinary dielectric media with dielectric constants ε1 and ε 2 , respectively. The Z-axis is perpendicular to the interface, the point charge q is on the Zaxis, and the interface is at z = 0. Two image charges q1 and q2 are used to solve this problem. In medium-2, the electric field is equal to what is generated by a point charge of ( q1 + q / ε1 ) at position (0, 0, d). The field in medium-1 is equal to the total field by a point charge q / ε1 at position (0, 0, d) and a point charge q2 at position (0, 0, –d). 已知介质-1、介质-2 为介电常数分别为 ε1 、 ε 2 的普通绝缘体。一点电荷 q 在介质-1 内， 离两介质之间的界面的距离为 d。坐标 Z 轴与界面垂直，点电荷 q 在 Z 轴上，界面位置为 z = 0。求解本题需要用到两个虚拟电荷 q1 、q2。在介质-2 内的电场由在(0, 0, d)的点电荷 q1 + q / ε1 产生；在介质-1 内的电场由在(0, 0, d)的点电荷 q / ε1 和在(0, 0, –d)的点电荷 q2 共同产生。 (i) Apply the above boundary conditions to determine q1 and q2. (3 points) 利用上述边界条件，求 q1、q2。（3 分） (ii) Determine the total surface charge density at the interface. (1 point) 求界面上的总电荷面密度。（1 分） (iii) Verify your answer with the special condition ε1 = ε 2 . (1 point) 用特殊情况 ε1 = ε 2 来验证你的答案。（1 分） (iv) Verify your answer with the special condition ε1 << ε 2 . (1 point) 用特殊情况 ε1 << ε 2 来验证你的答案。（1 分） (b) A magnetic dipole is made of a south pole and a north pole. Interestingly, so far no magnetic monopoles, namely the objects carrying only a south pole or a north pole, have ever been discovered. If a magnetic monopole of ‘magnetic charge’ g ever exists, it will generate a magnetic field in the same way as an electric point charge generates an electric field. Recently, pseudo particles behaving like magnetic monopoles generated by the collective motions of electrons in a particular type of materials, called the ‘topological insulators’, was theoretically predicted. Such particle can be induced by an external electric point charge. Similar to part-a, a point electric charge q is placed at a distance d from the interface between an ordinary dielectric medium (medium-1) with dielectric constant ε1 and

z

3

2011 年泛珠三角及中华名校物理奥林匹克邀请赛

Pan Pearl River Delta Physics Olympiad 2011

magnetic permeability μ1 , and a topological insulator (medium-2) with dielectric constant ε 2 , magnetic permeability μ2 , and a magneto-electric coupling constant β . The relations between various fields in G G G G G G G G G G B1 B2 + β E2 . medium-1 are D1 = ε1 E1 , and H1 = .Those in medium-2 are D2 = ε 2 E2 ? β B2 , and H 2 =

μ1

μ2

The electric field and the magnetic field in both media can again be found by using image charges as in part-a. For simplicity, let us use a set of specially chosen units such that the electric field at position G G G G r ? r0 G G r generated by a point electric charge q at position r0 is E (r ) = q G G 3 , and the magnetic field | r ? r0 | G G G G r ? r0 produced by a magnetic monopole of magnetic charge g in a similar spatial setting is B (r ) = g G G 3 . | r ? r0 | In medium-2, the electric field is generated by a point electric charge of ( q1 + q / ε1 ) at position (0, 0, d), and the magnetic field is generated by a magnetic monopole with charge g1 at position (0, 0, d). In medium-1, the electric field is generated by a point electric charge of q / ε1 at position (0, 0, d) and a point charge q2 at position (0, 0, –d), and the magnetic field is generated by a magnetic monopole with charge g2 at position (0, 0, –d). 磁偶极子由一对南、北极组成。有趣的是，到现在为止我们还没能找到只带南极或北极 的所谓磁单极子。一个带‘磁荷’ g 的磁单极子产生的磁场和一个点电荷产生的电场的表达式 是一样的。最近，有理论预言，在一种叫拓扑绝缘体（topological insulator）的物质里，电子 的运动可以产生象磁单极子这样的准粒子。这种粒子可由点电荷感应产生。与(a)部分类似，一 点电荷 q 在普通的介质-1 内，离介质-1 与拓扑绝缘体（介质-2）的界面的距离为 d。介质-1 的 介电常数为 ε1 ，磁化率为 μ1 。介质-2 的介电常数为 ε 2 ，磁化率为 μ2 ，电磁偶合系数为 β 。介 G G G G G G G B1 质-1 内各个场之间的关系为 D1 = ε1 E1 ， H1 = 。介质-2 内各个场之间的关系为 D2 = ε 2 E2 ? β B2 ,
G H2 =

G G G G r ?r G G 见，我们选用一套特殊的单位，使一位于 r0 的点电荷 q 在 r 处的电场为 E (r ) = q G G0 3 ，而磁 | r ? r0 | G G G G r ?r 荷 g 产生的磁场为 B (r ) = g G G0 3 。在介质-2 内的电场由位于(0, 0, d)的电荷 q1 + q / ε1 产生， | r ? r0 | 磁场由位于(0, 0, d)的磁荷 g1 产生。在介质-1 内的电场由位于(0, 0, d)的电荷 q / ε1 和位于(0, 0, –d)

μ2

G B2

μ1

G + β E2 。与(a)部分类似，介质里的电、磁场也能用虚拟电、磁荷来求解。为方便起

4

Note; The 扭缸汩的g sch臼ηc is mtended for grading when the final answer is wrong. If the final answ时 is conect, full m盯k should be given 自然rd less of the proc时飞ire.
PART! QI (8 points) In a g叫叫le

q，川抑制al 叫yU, -}aq' 时也同时ic en前衍毛才问＇ ,

(a)

i 、川 1 当

3 co呐 ＝ 2mgL(l .? .
I

I 3 cos<9J=2 气 mgL）庐， (I point)

iζa … mL〓i 令一 f8＇ 小一（… mL')8磊、 here ［ 照… ml＇ 。 point)

2

3 4 !a3{g 绍叶，，gL, andb = -m匠， then甜需！…＝：－！＂＇，I→仪 points)

2

4 2 3
I

Vb

2Ji\/L

Alternative solution. , l , 4 f 百 ml＇＋ … mL' ＝句， ml' (I pomt) 3 3
το
ω 飞二于皿 ι」卫工工出一芹叫一（2

IK

13 公 3呻ιL

}

\/ l

\/ 2·4mL1

3 I 2,/2'1 L

"

pomts)

u :-'l二（＿！＿书一＿！：＿1
p

to find the balance p恻岛，三

1 2 I ., (24+ 11 如β2 u. =-1I －：－一十？→ γ一→…－－，， lox 黑…一→ι2-ox'

L才阳Jx'. (l poi哗
1、hen a ，工…一一一句二二ι←
4,,L＇马

Alter双层ive
]

Force F …一一i 叮一一－；－，
4班。 ＼＿ x·

Balance pmnt at F ＝告， x， 二（J'i-l泣。（］ point)
l

4万句飞 x I Jx

q' 1 1

r

L 寸 － ox)

2 '1

r1

2

1

r1

2

1

I (l r

poin啡

。＇

{1

2

)

and making 制fficicnt of ox zero

c，土…二一刊0 万 Xe =(Ji －队叫树

x;

（主 ω 守。）＇

'

’问 l ,Ii

( ? r 1:

IL 一（ Ji － 巾 r J

8L'1e乌

(1 poi咐

(24{ l7ψ7)q'

AU’O

LT

?-d QA … lb

-Z w

-

l

E心

A吨吵

1.96~. (I point)

solution

l(t

2 1 I (1 pomt) (L-x)')

2

M础C叫1tK ＝－~I，，，＝去（二百多已到＝ 3.82兰以报〉
’ CCC

IK

「…？一

Q2{9po面也｝

Rel咄咄主ic total energy is E = ~τ （1

point)

point)

So the momentum 叩」~汗~＝均可~.（1 point)

c

c

(i) K 《 me＇ ，主旧

P 忽 ！. .fi, 阳宝宝 ！.／2x 自51 lxlO"" = I.Ox ］在＿， MeV le. (2 抖。3喇
c c
(ii) p (iii)

＝！.岳可E平王二~万J = l .4}\4"eV I c. (2 points)
c c

c Q3 (8 points) 问） L时 one cable c町咛 line charge densityλ 句 and 由e other 盹盯y …，＜， α1oose the line joining the cable centers as 由c X-axis and choosex 需 O at the middle point b咄咄阳 the ca七Jes哩也S ;i I 1 l 1 时时 clectnc field on the X-axis ,s E ＝……；一一←一十一.....：：.＿＿ 1- (1 pol就｝ 2,r，，气 d/2 ÷x d/2-x)

K 异 mc2. p 二 ！！＿ l.Oxl扩1,feV I c. (2 points)

Tue volta草e diff，自由国 between the 仰。 eabl聪 is d年aλr rd ., rd 1l＇＂－＇ λ （ d …H飞 λ （ d 飞 但 i E dx I Inl 一今x 仆!nl … x I I z 一－ Inl~ 阳县， 1τI (2 4立刻 2Jl"电 L 飞 2 ) \,2 Jj (JO 刻 π马飞 k j 剂。 ＼ 1<) points) 。
（d飞 C 寸口 zνInl I· (I point)

R

(b) Employ the method of image charge, the electric field is?= －一l 一…～… i The 2m 乌 （ d+x d x) voltage 郁的rence 犯（ 1 point)

(

1

I

l …

V=

d.,,

f Edx ＝＿！［记（d叫 －ln(d 司，d…r去总（子）＝~ln（去） (2 2万马
(2d 飞 -;;- i. (I

poin时 c-1 风 llnl poin吗

'

Q4(10 伊1ln相｝

(a) (i) The force of plate伺l on plate-2 is determined by the field gene方斟ed 如y plate-I only. Apply

Ga附 law to th叫到d川ngpl毗＂＂th a p姐！box boon必价r去E·d.'i ＝ 车
Since we a,e only consid由ng the field 悦。ne plate, which 指出C 描me on both side oft如c

'

",

pl班， the field is thcu.E ＝乒主任抖出）
“巾。

2

<;lnc can also use integration to cal即late the field dirα；tly.
E － …一；一…一－－…一一……一飞…牛 4矿石， ,(L'+r7 ）川 2，。（L' +t1 ）闪＇＇ 2c0

The 如cc 阳 unit 附a isF 坦 f-=,· (1 川口。

}

LC.0

(it) The total electric 丑eld 格由e

supe串osi衍。n

of the f如Id generated by 市e two plates. The

field between the pl阳 is? －三毛加tsi曲曲e plates the field is z棋。（ 1 point)

(iii) The work done on an area A of the plate is
Z 忍

(1 point) 2e0 (iv）双c volume of the space where the 在eld is non zero ts decreased by A8D . Let the en挝gy density of the 丑eld by H. Then the e在ergy storel 阳也c 丑。Id is decre斟时 byHAiiD By
8W-AF·iiD 二二←二 8D

o-' A 二 阳配gy cons哥va岳阳，肌48D 巳丁一δD
2&0 which is positive (2 p创n恼）

So the 四町gy density is given by H - c:- - 民·， F品’ 2e0 2

o-'

(i) Gauss law
iηthe

s

same way as part 归）哩 we 沁飞·e g - 2,rGo-z, (I point)
-4,rGσ

T.1e forιa per 到削t area isF 二 21rG<r0"i0. (1 poi刻。 (ii）我掉 field in the spacεbetween the plat目 lS z配O Outside the field is g (1 poi时） 。v）古le VO；明白 of space where the field is non-zero is mer邮sedby AoD.
-AF 、 8D 饵 2πGσ＂ A5D.

(1ii)8W

The 剧时且y s即时

in the field is de臼叫树…HAb"D. So H - -2:tG<r

－巾G~ －－.！＿_i_ （栩如ts) 飞4，机，）＇ 2 4irG

Q5 (5 poin拍） A homogenous sh，由全 withn> I 自由correct Possible solutions are given below. Any other 011es 吐时盯ccoπ·ect m principle should al甜 be g刊η full 黠arlc

Q6(10 poi极盼 (a) PV＇ 主 C ＝令 NKTV＇＇ 忽 C, (1 point) Th四只 IT,= 1飞／乙叫只 IV,Y' (l poi呻 (h) Internal en旺gyof ideal gas 1sl' - N,0 + Nc,T 型（ 1 point) Then

…川杰
y
I (1

Q 三四口 N叫几句） , ? ,

and Cv ,

- ~.

pot州

Wor呈阳

' ' i… y For path A‘ c-c， 口 P,V[ - Nk卖V{ ',andforpathC: C-Cc 凶 乓乓＇ - NkT,V｛＇ τbenwe
』 ave

W-

jPdV 坦 I cv' av － 二＇..－ V''

(I

poi时）

3

4

C

Nk!

I

iV.'i

J

、 1一ν 飞

! JT,~f-'r(T,

T，） 阳叫

W，＝ …芒 v (v,>-? －忖＝
(c)

……[ l → l 」 t
l … rl 飞 v,)

Nk(

(v.Y汁
[

) '

1'.

Z 叩……亿一叶，（ I point) 1… y

Nk

Then 去v,1Q 蒜 叹一乙） I (T2 年 Ii ），朋d 呈几 IQ=(T,-T,)l(T， …工；） , (I E警。由导
w 中审 (1：十 T,)-(T, 十 T 飞

9

, (1

po血。

(

(v,1 ＇＇飞 f

(v.1' '1

J·忡皿t)

PART ll Question I (IO poin如｝ Solution: (a) 1乳c tοtal m时阜y 碍 z玄Z飞tel范 larger t如an the 矿est 臼E吾y So 曲c answ轩 is 乓 I m 阳阳口o 始 movio革 atspe窑d V挝ye！οsetο 咀，at oflight (3 pomt§ ) (b)
E,

2pc 2pc
l m'c' 1 （旷…m;)c也 I arr汽4 ＿.：，：：一）恐？…～…冉一＝寸一一一位 pot附｝

m.＇ ♂ 局 pc(l …立立工－）－ p<(l

2

T z 一一一ω …＝……，－，，. (2 poi在毡｝ IE，：：?二 I l:vn'c' If 出e expansion is done m （咛 2础忧ad in （沟，悦l mark should still be given to (b).

(c) From expr瑞si-On of T in （坊， wehaveam'

=Tc''(! pomt)
JC

2Pch

, ? 2hcE Substitute P 玛 EI c (1 point) into above: t,mγ 叫一士十
On the o也er hand, cT 12 = 2尺础，（ I point) and R，础二 6xl06m (I 萨’恤金｝

Th四 Ml与＇＝……－－……一一一一.....，，－ ι …叫：启立告匀× 10' eV' (I 衍，如斗
4R 制准 立× 6xl0''

2hcE

IOi主 x!O＇台 xl.24 × JO""'

Note: Any answer 帆船 m the given 四nge s如ould get full mark.
Quεstion

2 (15 points)

Solution: （的 (i) The impulse pc叩endicul盯 to the path is I 提 j FJt ），古工 jF怡陋 B（材（ I 仰nt)
t:ilJl (J =

xIb

andx 叫人附 then have

dt =

I ,

ax 黑… d（棚 fl)=

b

b

I ---,-;;dB (l point)
t歹

ννγcos

Then ／二 i

,,a GMmb
l>V

?-,,

－－－－－；－，一份s()d（）＝一－：－－· (I po峭

2GMm

τbe imp时se alon革命e pa位 is

j 斗 F;. (t)dt 斗 F(t)sinθ（t)dt 兰 气γ－
' ?

GMmb ,,.,

D νr “川

I "" sinθdB= 0
4

(1 point)

5
(ii)p 工 mv ， 白朗扣斗二－－－－－，－－，－ ? (] point)

l

20，号f

p

bv·

（』）

1.4 × i自6
e 、－－

(ii)

Correct 盘a刑ng

(2 point咛

(i1革 seζ ……＂：＇：＂＂＂ :c:: 一－一一－－－－－－，…一.，...，.←＝ 21 × 10

2GM

2x6 67xl 。什 1,2 ×i告知
1.4× 1苗。×（3 × 10丁－

Re'

'

φ

(4 poin 悟）

The 拥gul时 distan凶始出en8=2吭，. + 20吉＝ 2.280 x 10' (l point)

the snn is 缸。如往事ht (I po撒哈 (v) No, l ec阳sethe 扭扭1!ar diameter of the moon would only 革时比lf of the a旧（ I point)

Q3 (20 points)

Ix磊十 y' 丰（ z … d)'

(a)

I

e,

E, =A'-土乓业吨各（三十q,),z<O, (0,5 如回s)

Lx' ＋扩巾（卜 d)"J

&,

Full m磊rks should be given if 寸L

ap严部则he above answ削

ρ，

=c2E,, D, =?1?,

\”' /

1.:L

E; = E；＇ 之。毛 ＝ q,

I· (I point) Solving （！）聪d （匀， q， 耳熟＝ I= \. c， 斗争 ＆，），?，）

（匀。当 points) n 飞／ φ 飞 f
<

s,u1q, I q q d I 份。口材昕一?；－）叫矿I ：：－一一－ ·:;,;r以 ψ 争一＋ q,l I ＝川...:::.:2L.可芹，（ I point) Jlx＇今 y＇ 牛 d ＇ 「 &,&, llx'+y ＇十 d马一－ Full mark should be 在IV副主 if &0 instead of4万 is give口 (iii) e， 主马，记昂 q1 =0. No 前terface and no 盟,age ch自ge. (I point)

cha玄喜c f吁＝ 'l牛 and a rε,iJ ch盯喜e豆. (l po诅t)
81

E,

(b)

(i）

ρ2 工 e，孟.， - f3B.句， D, e;E，γ 豆i， 凶 ！！.，，＿ φ 卢'E,' if，＝ 主
?， 战

i， ”乒玛业羊毛，!L ＋异地旦旦~q， ，户。（I poi哗
x＇ ÷y＇＋（卜 d)' J L 『 Lx～ y＇ 叫z +d)'

J

5

6
?叫＇，－，＋ xv， 斗z

-

，二，…V

/_'

d)i.二

lx'+y＇ 叫z d）＇；…码
n 十｝夜＋ (z

< 0. (I point)

poin命

l …江以二＂－－＇－＇＂..斗斗品， z ＞ 在（ l

+ d)l,.

[x＇ 旷＋（z 呻＇］川山

_ _

; x' + yι÷ （z dl'
A扫江 0,

I

,,,g,.z<O.(lpoint)
d 捕归JS.

apply t主 e bc·undary co1

(i）苟二益；

(ii)
;a

g,

(I)ι （ I poin之｝

i5/ ＝房
--qdi,

cq

d言

ix'+ l

+d'J'' ［户 y' +d'J"''

--,

_( !L+q， 呐户 \&, ! PR"?c (T;y'+d']'" [x＇ 令y' +d于
(2}- (I

4 丑 i) t；ρ ＝ E

;
q_
X裁。十 3

「飞户卢斗：rj-;;;T~习功齿，

。｝

,

So

q， 忑啦

(1 point)

｛叫 H;'

if,
V 忖叫’ r＇具

「《

so ＆＝豆川 β｛!L 斗 q,)

c,

Put协附（！）呵。）

'=q, -I

into （衔，＂ e finally get { (s, -s,)(1 ／间 ＋ JI?,) -f)' )(qi

,÷Ii ?2 ) ÷ f]' ）＼ 叫／

F二ι－－－＂；；－

II …!, (I po,时）

,= '

I β (!LI l(E，忖，）（lj 《＋ ll 抖抖 JJ'Ae,J

c1 po峰时｝

§

?
i拟出e unit sys剧烈时e<l
cha玄ge

here, the G税制’ s Law b臼泪。如eV·E 出如伊. wh町 ep

JS the 如tal

density. Tru:cl乙ctric charge sheet density is

I 滔，－：：－生鱼=r· (l pm呻 σ 叫时々→ E；：） 叫汁牛气拧（q，→旦 ＋ !L-qi1 I Ix·+ y' +d' J c,
! Ix ＇ ÷y二叫， J
,,
L1kew1脯， the Ampere ’ s Lawnow isV × B=4trf, wh时cl isthe el惧怕G C让rrent d在lSi秒 Do not d臼iuc1 any points if 片吕 use<l instead of4ll . Choose a point on the X-axt:弓，朋d take a loop 明您 length Land

nearly z町。 height. g, →矿 g， g, 『I ，＝车手 χ。川…τ 忌， s; ＝－τXo For a loop perpendic ular to 挂1eXx x x out of the p呼口 plat时， the pa也 (pointmg 也制is y the along axis and

...，争e

2 I 1

’霉事

''

For a loop parallel to the X币制is 踊 shown in the fi且旧c, Lg Lgh 平 ·L五e + B;' ·Lx， 三寸与「

；性生

' ,Z . I
>

.
I

'

pH H·dl-=-ff
I

X

X'

x'

X 丁

σ

I -

B e., poi往往Z稳 into the p呼er plane. In Using 出e right 』and rule, we have K = 一条…儿， 2;rx1

： (Ip叫 阳刚， we have ii: = .!1L毕芳 21' 飞儿 T)')
Any other ways 如拮ach the above expression 五or the current densi守翻飞， fine.

7

2007年泛珠三角及中华名校物理奥林匹克邀请赛试题_免费...

2007年泛珠三角及中华名校物理奥林匹克邀请赛试题 2007年泛珠三角及中华名校物理奥林匹克邀请赛2007年泛珠三角及中华名校物理奥林匹克邀请赛隐藏>> Pan Pearl River ...

2015年泛珠三角及中华名校物理奥林匹克邀请赛

2015 年泛珠三角及中华名校物理奥林匹克邀请赛 香港科技大学高等研究院赞助 卷.1(共 5 题) (9:00 am - 12:00 pm, 25 February, 2015) 1.火星的逆行运动...

2014年泛珠三角及中华名校物理奥林匹克邀请赛试题

2014年泛珠三角及中华名校物理奥林匹克邀请赛试题_学科竞赛_高中教育_教育专区。扫描版今日推荐 180份文档 CET四六级高分通关宝典 2014年6月大学英语六级考试真题...

2 014年泛珠三角及中华名校物理奥林匹克邀请赛试题

2 014年泛珠三角及中华名校物理奥林匹克邀请赛试题_高中教育_教育专区。2 014 年泛珠三角及中华名校物理奥林匹克邀请赛试题 香港科技大学高等研究院赞助 转载列表:...

2009年泛珠三角及中华名校物理奥林匹克邀请赛Solution_...

2009年泛珠三角及中华名校物理奥林匹克邀请赛Solution_09 第五届第五届隐藏>> Pan Pearl River Delta Physics Olympiad 2009 Part-I 第一卷 Q1 题 1 (8 point...

2007年泛珠三角及中华名校物理奥林匹克邀请1

Pan Pearl River Delta Physics Olympiad 2007 年泛珠三角及中华名校物理竞赛 2007 年泛珠三角及中华名校物理奥林匹克邀请赛 Pan Pearl River Delta Physics Olympiad...