Shenzhen Hong Kong Pui Kiu College Longhua Xinyi School
Grade 12 Physics | 21 Oct 2026 | Paper A (24 MCQs) + Paper B (3 structured questions)
Understand where the marks were lost first, then read the item-by-item solutions — that is the fastest route.先看清分数丢在哪里,再逐题看解析,效率最高。
| Part | Questions | Max | Score | Rate |
|---|---|---|---|---|
| Section A — Multiple choice | 1 – 24 | 30 | 20 | 66.7% |
| Section B — Q1 (Photoelectric effect) | 1(a)–(c) | 10 | 7 | 70% |
| Section B — Q2 (Hydrogen-like ion) | 2(a)–(b) | 10 | 5 | 50% |
| Section B — Q3 (STM) | 3(a)–(e) | 10 | 5 | 50% |
| Total合计 | — | 60 | 37 | 61.7% |
| Topic | Items | Core requirement |
|---|---|---|
| Photoelectric effect & photons | A1–A8, B1 | hf = φ + Kmax; eVs = Kmax; I–V and Vs–f graphs; the three failures of the wave model光电方程、遏止电压、两类图像、波动说失效的三点理由 |
| Evolution of atomic models | A9–A11, A14 | Thomson plum-pudding → Rutherford nuclear → Bohr quantisation: what each can and cannot explain汤姆孙 → 卢瑟福 → 玻尔,各自能解释什么 |
| Hydrogen spectrum | A12, A13, A15, A16, B2 | En = −13.6/n² eV; series limits and excited-state numbering; emission vs absorption arrows; derivation of R能级公式、谱系编号、发射/吸收箭头方向、R 的推导 |
| Matter waves & electron diffraction | A17, A18, A21 | λ = h/p; higher kinetic energy → shorter λ → narrower fringes德布罗意波长与条纹间距 |
| Resolving power & microscopes | A20, A22, A23, B3 | Rayleigh criterion θ = 1.22λ/D; TEM vs STM principles and limits瑞利判据;TEM 与 STM 的原理与限制 |
| Nanomaterials & allotropes | A19, A24 | Same atoms, different arrangement; surface and quantum effects同素异形体;表面效应与量子效应 |
Read the stem carefully: the statement must be both an implication of the wave theory and in conflict with the photoelectric effect.
First identify the applied voltage: the battery's positive terminal is on the metal plate, so the voltage is retarding.
Observations and inferences:
Rutherford's nuclear model (1911) contains exactly these three elements.
Rutherford's model is a classical picture: the electron orbits the nucleus and the Coulomb attraction supplies the centripetal force. Bohr kept that picture and added quantisation.
A shorter λ needs a larger momentum. Because the electron is far lighter, at the same speed it has much less momentum, so it must travel much faster to beat the neutron.
Both are made of carbon atoms; they are allotropes and differ only in how the atoms are arranged — diamond is a three-dimensional network (each C bonded to four others, sp³) while graphite is layered hexagonal sheets (sp²).
| Microscope | Aperture D / μm | λ / nm | θmin ≈ 1.22λ/D |
|---|---|---|---|
| P | 40 | 0.0040 | 1.22×10−7 rad |
| Q | 35 | 0.0050 | 1.74×10−7 rad |
| R | 14 | 0.0055 | 4.79×10−7 rad |
| S | 12 | 0.0065 | 6.61×10−7 rad |
A TEM forms its image from electrons that have passed through the specimen, so the specimen must be extremely thin (typically < 100 nm). A conducting specimen is also preferable to avoid charging.
Structured answers are marked on key terms + a complete logical chain + full working. Each item below gives the model answer first, then the marking points and a diagnosis of the marks you actually lost.结构题得分点是"关键词 + 逻辑链 + 完整运算"。每题先给范文,再给采分点与实际失分诊断。
Given: green light λ = 495 nm (weak), threshold frequency f0 = 5.10×1014 Hz (corresponding to yellow light)已知:绿光波长 495 nm,金属截止频率 5.10×10¹⁴ Hz(对应黄光)
Under the wave model the energy of the incident light is spread out continuously over the wavefront, so an electron at the surface can absorb energy gradually and accumulate it until the work function is exceeded. The wave model therefore predicts that radiation of any frequency would eventually eject electrons, provided the intensity is high enough or the illumination lasts long enough — that is, emission would depend on intensity and there should be no sharp cut-off frequency.
Experimentally, however, no electrons are emitted at all when f < f0, however intense the light. This strong dependence on frequency rather than intensity is exactly what the wave model cannot explain.
波模型下光能连续分布在整个波前,表面电子可以逐渐吸收并累积能量,直到超过逸出功。因此波模型预言:只要强度足够大或照射时间足够长,任何频率的光最终都能打出电子,即发射只取决于强度,不应存在尖锐的截止频率。但实验中当 f < f₀ 时无论光多强都完全没有电子逸出——这一"只认频率、不认强度"的现象正是波模型无法解释的。| Condition | Stopping potential Vs | Maximum photocurrent | Reasoning |
|---|---|---|---|
| (i) Blue light, same intensity蓝光,强度相同 | Increases增大 | Decreases减小 | Blue has a shorter wavelength and therefore a higher frequency, so each photon carries more energy and Kmax = hf − φ is larger; hence Vs = Kmax/e increases. The same intensity means the same total energy per second, but each photon is more energetic, so the number of photons per second falls, fewer photoelectrons are released per second and the maximum photocurrent is smaller. 蓝光波长更短、频率更高,单光子能量更大,最大动能更大,故遏止电压增大。强度相同意味着每秒总能量相同,而单光子能量更大,因此每秒光子数减少,光电子数减少,最大光电流减小。 |
| (ii) Green light, same wavelength, higher intensity绿光,波长相同,强度更高 | Unchanged不变 | Increases增大 | Same wavelength means the same photon energy, so Kmax and therefore Vs are unchanged. Higher intensity means more photons per second, so more photoelectrons per second and a larger current. 波长(频率)不变,单光子能量不变,最大动能与遏止电压不变;强度增大使每秒光子数增多,光电子数增多,电流增大。 |
Given: En = Z²(−13.6/n²) eV for a hydrogen-like ion, where EG is the ground-state energy of hydrogen题给:类氢离子能级 En = Z²(−13.6/n²) eV
Hydrogen has the smaller ionisation energy.
The energy of a hydrogen-like ion is proportional to Z², so the electron in He+ feels an attractive Coulomb force from a +2e nucleus that is four times stronger. It is therefore bound far more tightly and four times as much energy is needed to remove it.
氢原子的电离能更小。类氢离子能量正比于 Z²,He⁺ 的电子受 +2e 核的库仑引力是氢的 4 倍,被束缚得更紧,需要 4 倍能量才能移出(13.6 eV 对比 54.4 eV)。No. The formula was derived for a nucleus of charge +e (Z = 1). For He+ the nuclear charge is +2e, so every energy level is multiplied by Z² = 4:
The modified formula is therefore
A probe scans across the sample surface at a constant height.探针在样品表面上方以恒定高度扫描。
The current is a tunnelling current, produced by the quantum tunnelling effect — electrons cross the vacuum gap between tip and sample even though they classically lack the energy to do so.
该电流是隧道电流,由量子隧穿效应产生:电子在经典上能量不足的情况下仍能穿过针尖与样品之间的真空势垒。A very sharp probe is scanned across the sample at a (nominally) constant height, with a small voltage applied between tip and sample so that electrons tunnel across the gap. The tunnelling current depends exponentially on the tip–sample separation d:
so a tiny change in separation produces a large change in current. By recording the current at every position (x, y) while scanning — or by using a feedback loop that moves the tip up and down to keep the current constant and recording that height — a three-dimensional topographical map of the surface is built up, ultimately to atomic resolution.
用极细的探针在样品上方以(近似)恒定高度扫描,并在针尖与样品间加小电压使电子隧穿。隧道电流随间距 d 指数变化,间距的极小改变会引起电流的显著变化。逐点记录扫描中各位置的隧道电流(或用反馈回路调节针尖高度以保持电流恒定并记录该高度),即可重建表面三维形貌,最高可达原子分辨。(i) It can probe only the surface (the outermost atomic layer) and reveals nothing about the interior. Another accepted limitation is that the sample must be electrically conducting.
(ii) No. The tunnelling current depends only on the gap between the tip and the topmost surface atoms, so information about the interior of the slice cannot be obtained.
(i) 只能探测表面(最外层原子),无法反映内部结构(另一可接受答案:样品必须导电)。(ii) 不合适:隧道电流只取决于针尖与最外层表面原子的间距。Atomic manipulation — the tip can pick up, drag or position individual atoms and molecules on a surface (for example building atomic-scale patterns or writing information), or it can measure the local electronic density of states.
原子操纵:用针尖搬运、移动或放置单个原子/分子,构建原子尺度的图案或写入信息;也可测量表面局域电子态密度。No. The Rayleigh criterion applies to instruments that form an image from waves passing through a lens or aperture, where the resolution is set by diffraction, θmin = 1.22λ/D.
An STM involves no lens and no wave-imaging process. Its resolution is determined by the sharpness of the tip and by the exponential dependence of the tunnelling current on the tip–sample distance, so an extremely small change in separation produces a measurable change in current. Atomic resolution is therefore achieved without any diffraction limit.
不受限。瑞利判据适用于以波经透镜/孔径成像、分辨率受衍射限制的仪器。STM 没有透镜成像过程,其分辨率由针尖尖锐程度以及隧道电流对间距的指数依赖决定,间距的极小变化即可引起可测的电流变化,故可在无衍射限制的情况下达到原子分辨。| Quantity / law | Formula or value |
|---|---|
| Planck constant | h = 6.63×10−34 J s (hc = 1240 eV nm)普朗克常数 |
| Speed of light · elementary charge · electron mass | c = 3.00×108 m s−1; e = 1.60×10−19 C; me = 9.11×10−31 kg光速、元电荷、电子质量 |
| Photon energy | E = hf = hc/λ光子能量 |
| Photoelectric equation | hf = φ + Kmax, with φ = hf0光电方程 |
| Stopping potential | eVs = Kmax ⇒ Vs = (h/e)f − φ/e遏止电压 |
| Hydrogen energy levels | En = −13.6/n² eV氢原子能级 |
| Hydrogen-like ion levels | En = Z²(−13.6/n²) eV类氢离子能级 |
| Rydberg formula | 1/λ = R(1/n1² − 1/n2²), R = 1.097×107 m−1 = EG/(hc); for hydrogen-like ions use Z²R里德伯公式 |
| Series limits | Lyman → n=1; Balmer → n=2; Paschen → n=3; Brackett → n=4; Pfund → n=5各谱系终点 |
| de Broglie wavelength | λ = h/p = h/√(2mK) = h/√(2meV)德布罗意波长 |
| Rayleigh criterion | θmin = 1.22 λ / D瑞利判据 |
| Double-slit fringe spacing | Δy = λD/a双缝条纹间距 |