Formula Derivation in AS Physics Paper 1 (January 2018) | AS物理试卷1公式推导(2018年1月)

📚 Formula Derivation in AS Physics Paper 1 (January 2018) | AS物理试卷1公式推导(2018年1月)

In AS Physics Paper 1, especially in the January 2018 sitting, candidates often encounter questions that require a solid understanding of how fundamental equations are derived. Being able to reconstruct these derivations not only strengthens conceptual grasp but also helps tackle multiple-choice and structured questions with confidence. This article revisits the key derivations across mechanics, materials, waves and electricity that are central to the AS syllabus.

在AS物理试卷1中,尤其是2018年1月的考试,常会出现需要扎实理解基本方程如何推导的题目。能够自己推导这些公式不仅能加深概念理解,还能自信地应对选择题与结构化问题。本文重温了力学、材料、波和电学中核心公式的推导,这些都是AS阶段的学习重点。

1. Deriving the First Equation of Motion (v = u + at) | 推导第一个运动学方程 (v = u + at)

Acceleration is defined as the rate of change of velocity. For uniform acceleration, this can be written as a = (v − u) / t, where u is the initial velocity, v is the final velocity and t is the time taken.

加速度定义为速度的变化率。对于匀加速运动,这可以写成 a = (v − u) / t,其中 u 是初速度,v 是末速度,t 是所用时间。

Multiplying both sides by t gives at = v − u. Adding u to both sides yields the first equation of motion.

两边同乘以 t 得到 at = v − u。再在两边加上 u,就得到了第一个运动学方程。

v = u + at

This linear relationship shows that final velocity is simply initial velocity plus the velocity gained from acceleration over time.

这个线性关系表明,末速度等于初速度加上加速度在时间内增加的速度。


2. Deriving the Second Equation of Motion (s = ut + ½at²) | 推导第二个运动学方程 (s = ut + ½at²)

For uniform acceleration, displacement s equals average velocity multiplied by time. The average velocity is (u + v)/2. From the first equation, v = u + at, so substituting gives:

对于匀加速运动,位移 s 等于平均速度乘以时间。平均速度为 (u + v)/2。由第一个方程 v = u + at 代入得到:

Average velocity = (u + u + at)/2 = u + ½at. Multiplying by t gives the displacement.

平均速度 = (u + u + at)/2 = u + ½at。乘以时间 t 即得位移。

s = ut + ½at²

This derivation shows how displacement depends on initial velocity, time and acceleration. The term ½at² arises from the additional distance covered due to acceleration.

这个推导表明位移依赖于初速度、时间和加速度。项 ½at² 来自于因加速而多走的距离。


3. Deriving the Third Equation of Motion (v² = u² + 2as) | 推导第三个运动学方程 (v² = u² + 2as)

Start by squaring the first equation: v² = (u + at)² = u² + 2uat + a²t². Factor out 2a from the last two terms: v² = u² + 2a(ut + ½at²).

先将第一个方程平方:v² = (u + at)² = u² + 2uat + a²t²。将后两项提取公因子 2a:v² = u² + 2a(ut + ½at²)。

Notice that the bracket is precisely the expression for s. Hence, v² = u² + 2as.

注意到括号内正好是 s 的表达式。因此得到 v² = u² + 2as。

v² = u² + 2as

This equation is particularly useful when time is not involved, linking velocity, acceleration and displacement directly.

这个方程在不需要时间时尤其有用,直接关联了速度、加速度和位移。


4. Deriving Kinetic Energy (Eₖ = ½mv²) | 推导动能公式 (Eₖ = ½mv²)

Consider an object of mass m accelerated from rest to speed v over a displacement s by a constant force F. The work done by the force is W = F × s. From Newton’s second law, F = ma.

考虑质量为 m 的物体,在恒力 F 作用下由静止加速到速度 v,位移为 s。力做的功 W = F × s。由牛顿第二定律,F = ma。

Using v² = u² + 2as with u=0 gives v² = 2as, so s = v²/(2a). Substituting into the work equation:

利用 v² = u² + 2as,且 u=0,得 v² = 2as,所以 s = v²/(2a)。代入功的公式:

W = ma × (v²/(2a)) = ½mv². This work is stored as kinetic energy.

W = ma × (v²/(2a)) = ½mv²。这个功以动能的形式储存。

Eₖ = ½mv²


5. Deriving Gravitational Potential Energy (ΔEₚ = mgΔh) | 推导重力势能变化 (ΔEₚ = mgΔh)

To lift an object of mass m through a vertical height Δh at constant velocity, the upward force must equal the weight mg. The work done by this force is force × distance = mg × Δh.

将质量为 m 的物体匀速提升竖直高度 Δh,向上的力必须等于重力 mg。该力做的功为力 × 距离 = mg × Δh。

Work done against gravity is stored as gravitational potential energy, so the change in GPE is:

克服重力做的功储存为重力势能,因此重力势能的变化为:

ΔEₚ = mgΔh

This assumes a uniform gravitational field and no other energy transfers.

这里假设均匀重力场且无其他能量转化。


6. Deriving Conservation of Momentum from Newton’s Third Law | 从牛顿第三定律推导动量守恒

Consider two bodies A and B colliding. During collision, A exerts force F on B for time Δt. By Newton’s third law, B exerts force −F on A for the same duration.

考虑两个物体 A 和 B 碰撞。碰撞期间,A 对 B 施加力 F 持续 Δt 时间。根据牛顿第三定律,B 施加力 −F 于 A,时间相同。

Impulse on B = FΔt = mBvB − mBuB. Impulse on A = −FΔt = mAvA − mAuA. Adding these gives:

对 B 的冲量 = FΔt = mBvB − mBuB。对 A 的冲量 = −FΔt = mAvA − mAuA。两式相加:

0 = mAvA + mBvB − (mAuA + mBuB). Hence total momentum before equals total momentum after:

0 = mAvA + mBvB − (mAuA + mBuB)。因此碰撞前总动量等于碰撞后总动量:

mAuA + mBuB = mAvA + mBvB

This derivation confirms that momentum is conserved in an isolated system where no external forces act.

这一推导确认,在无外力作用的孤立系统中,动量守恒。


7. Deriving Elastic Potential Energy (E = ½FΔx or ½k(Δx)²) | 推导弹性势能 (E = ½FΔx 或 ½k(Δx)²)

For a spring obeying Hooke’s law, the force F is proportional to extension x: F = kx, where k is the spring constant. The force is not constant; it increases linearly from 0 to kx.

对于遵循胡克定律的弹簧,力 F 与伸长量 x 成正比:F = kx,其中 k 是弹簧常数。这个力不是恒定的;它从 0 线性增加到 kx。

The work done in stretching the spring is the area under the force–extension graph, which is a triangle: W = ½ × base × height = ½ × x × kx = ½kx². Using F = kx, the same energy can be written as ½FΔx.

拉伸弹簧做的功等于力–伸长量图下的面积,这是一个三角形:W = ½ × 底 × 高 = ½ × x × kx = ½kx²。利用 F = kx,同样的能量可写成 ½FΔx。

E = ½FΔx = ½k(Δx)²

This stored energy is recoverable as long as the elastic limit is not exceeded.

只要不超过弹性极限,这部分储存的能量是可恢复的。


8. Deriving Total Resistance for Series Resistors (R = R₁ + R₂) | 推导串联电阻的总电阻 (R = R₁ + R₂)

In a series circuit, the same current I flows through each resistor. The total p.d. V is the sum of individual p.d.s: V = V₁ + V₂. Using Ohm’s law, V = IR, V₁ = IR₁, V₂ = IR₂.

在串联电路中,相同电流 I 流过每个电阻。总电势差 V 等于各电阻电势差之和:V = V₁ + V₂。利用欧姆定律,V = IR,V₁ = IR₁,V₂ = IR₂。

Substituting gives IR = IR₁ + IR₂. Dividing through by I yields the simple sum:

代入得 IR = IR₁ + IR₂。两边除以 I 得到简单的相加关系:

R = R₁ + R₂

This result can be extended to any number of resistors in series.

此结果可以推广到任意数量电阻串联的情形。


9. Deriving Total Resistance for Parallel Resistors (1/R = 1/R₁ + 1/R₂) | 推导并联电阻的总电阻 (1/R = 1/R₁ + 1/R₂)

In a parallel arrangement, the p.d. V across each resistor is the same. The total current I splits: I = I₁ + I₂. Using Ohm’s law, I = V/R, I₁ = V/R₁, I₂ = V/R₂.

在并联连接中,每个电阻两端电势差 V 相同。总电流 I 分流:I = I₁ + I₂。利用欧姆定律,I = V/R,I₁ = V/R₁,I₂ = V/R₂。

Therefore V/R = V/R₁ + V/R₂. Dividing by V gives the reciprocal formula:

因此 V/R = V/R₁ + V/R₂。除以 V 得到倒数公式:

1/R = 1/R₁ + 1/R₂

The combined resistance is always smaller than the smallest individual resistance.

并联后的总电阻总是小于最小的单个电阻。


10. Deriving the Wave Equation (v = fλ) | 推导波速方程 (v = fλ)

The frequency f of a wave is the number of complete oscillations per second. The period T is the time for one complete wave to pass a point, and f = 1/T.

波的频率 f 是每秒钟完整振动的次数。周期 T 是一个完整波通过某点的时间,且 f = 1/T。

In one period, the wave travels exactly one wavelength λ. Therefore speed v = distance/time = λ/T. Substituting T = 1/f gives:

在一个周期内,波恰好传播一个波长 λ。因此速度 v = 距离/时间 = λ/T。代入 T = 1/f 得到:

v = fλ

This fundamental relationship applies to all types of waves, from sound to electromagnetic waves.

这个基本关系适用于所有类型的波,从声波到电磁波。

Published by TutorHao | Physics Revision Series | aleveler.com

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