HKDSE · 試験対策

Physics 試験対策

Master the HKDSE Physics exam with crucial study strategies, evidence-based common mistakes analysis, and professional calculator program setups based on 2021-2025 past papers and official HKEAA examiner reports.

読了時間 3 分更新日: 2026年6月21日

試験の概要

試験数
2
満点
153
制限時間
3時間 30分
出題形式
4
試験時間配点問題数配点比率出題形式
Paper 1 (Core Curriculum)2時間 30分1174560%MCQ, Short Question, Long Question
Paper 2 (Elective Curriculum)1時間361820%MCQ, Structured Question
評価段階
5**5*54321U
電卓の規定

Use only calculators on the HKEAA Approved List, bearing the 'H.K.E.A.A. APPROVED' (or older 'H.K.E.A. APPROVED') label. Programmable scientific models (e.g. Casio fx-50FH II, fx-3650P II) are allowed, and you MAY keep your own formulas/programs stored in memory — HKDSE does not require you to clear it. Graphic-display (graphing) and CAS/symbolic calculators are not on the approved list and must not be used.

  • AO1: Knowledge and Understanding (35%)
  • AO2: Evaluation and Translation (45%)
  • AO3: Experimental Skills and Investigation (20%)

過去問と採点基準にもとづいて作成(2021–2025)。

電卓プログラム

Resistors in Parallel

Casio fx-50FH II / fx-3650P II (HKEAA-approved programmable)

目的: Two resistors: \(R=\dfrac{R_1R_2}{R_1+R_2}\).

使う場面: Combining two parallel resistors quickly.

手順
Prompt R1, R2; outputs the combined resistance.
プログラム
?→A:?→B:AB÷(A+B)

試験での注意: For 3+ resistors apply it pairwise.

Thin Lens / Mirror Equation

Casio fx-50FH II / fx-3650P II (HKEAA-approved programmable)

目的: \(\frac{1}{f}=\frac{1}{u}+\frac{1}{v}\Rightarrow f=\frac{uv}{u+v}\).

使う場面: Lens/mirror problems given two of f, u, v.

手順
Prompt u, v; outputs f.
プログラム
?→U:?→V:U V÷(U+V)

試験での注意: Keep the real-is-positive sign convention consistent.

Kinematics (v and s)

Casio fx-50FH II / fx-3650P II (HKEAA-approved programmable)

目的: Constant acceleration: \(v=u+at\), \(s=ut+\tfrac12at^2\).

使う場面: Uniformly accelerated motion given u, a, t.

手順
Prompt u, a, t; outputs v then s.
プログラム
?→U:?→A:?→T:U+A T◢U T+0.5A T²

試験での注意: Only valid for constant acceleration; use SI units.

よくあるミス

  1. 1high影響する配点: 2Change of state: melting, boiling, latent heat

    Arguing that using a copper cup is justified in heat transfer measurements because copper conducts heat faster.

    回避方法: State that copper is a good conductor of heat, which would significantly increase heat loss to the surroundings by conduction, making polystyrene (a good insulator) a much better choice to minimize errors.
  2. 2high影響する配点: 2Force and Newton’s laws

    Assuming the tension in the string is exactly equal to the weight of the hanging mass when the system is accelerating downwards.

    回避方法: Apply Newton's Second Law: because the hanging mass accelerates downwards, there must be a net downward force, meaning weight must be greater than tension (\( mg - T = ma \)). Therefore, tension \( T \) is smaller than weight.
  3. 3medium影響する配点: 2Gases: laws and kinetic theory

    Assuming a gas cylinder can completely empty its gas contents into external containers/balloons.

    回避方法: Remember that once the pressure inside the cylinder drops to equal the ambient pressure (e.g., seabed pressure or atmospheric pressure), no more gas can flow out. The volume of gas remaining in the cylinder is still \( V \) at that ambient pressure.
  4. 4medium影響する配点: 2Electromagnetism & electromagnetic induction

    Believing that eddy currents can only be induced in magnetic metals like iron, rather than any conductor.

    回避方法: Explain that eddy currents are induced in any metallic conductor (such as copper or aluminium sheets) experiencing a changing magnetic flux, in accordance with Faraday's Law and Lenz's Law.
  5. 5high影響する配点: 2Gases: laws and kinetic theory

    Using macroscopic arguments instead of kinetic theory to explain pressure changes in gases.

    回避方法: Always describe the microscopic behavior: state that pressure is due to molecules colliding with the walls, and link pressure changes to the average kinetic energy (speed) of molecules and their collision frequency per unit area.
  6. 6medium影響する配点: 1Uniform circular motion and gravitation

    Omitting the negative sign in potential energy calculations when solving kinematics via conservation of energy.

    回避方法: For gravitational potential energy in orbits, use \( U = -\frac{GMm}{r} \) and carefully evaluate the difference: \( \Delta U = U_f - U_i \). Keep track of double negatives.

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