📚 Radian Measure: Angular Measurement in Circular Motion | 弧度制:圆周运动中的角度度量
When studying circular motion in A-Level Physics, the choice of angle unit is not arbitrary — it is deliberately made to simplify the mathematics of motion along a curved path. The radian is the SI unit of angular measure, and it forms the foundation of every equation you will encounter in rotational dynamics, from angular velocity to centripetal acceleration.
在 A-Level 物理学习圆周运动时,角度单位的选择并非随意——它是经过精心设计,用以简化曲线路径上运动的数学表达。弧度是角度的国际单位制(SI)单位,它构成了从角速度到向心加速度等旋转动力学中一切方程的基础。
1. What is a Radian? | 什么是弧度?
A radian is defined as the angle subtended at the centre of a circle by an arc whose length is exactly equal to the radius of the circle. In other words, if you take a length of string equal to the radius r and lay it along the circumference of the circle, the angle spanned at the centre is 1 radian — approximately 57.3°.
弧度的定义是:圆上长度恰好等于半径的弧所对应的圆心角。换言之,若取一段长度等于半径 r 的细绳,将其沿圆周铺设,则圆心处所张的角度即为 1 弧度——约等于 57.3°。
This definition leads directly to the fundamental relationship between arc length s, radius r, and angle θ (in radians):
这一定义直接引出了弧长 s、半径 r 与角度 θ(以弧度为单位)之间的基本关系:
θ = s / r or s = rθ
Because θ is defined as a ratio of two lengths, it is dimensionless. However, the radian is still treated as a unit to indicate that angular measure is being used, just as the mole counts dimensionless entities.
由于 θ 被定义为两个长度的比值,因此它是无量纲的。然而,弧度仍然被视为一个单位,以表明此处使用的是角度的度量,正如摩尔用于计数无量纲的粒子数目一样。
2. Converting between Degrees and Radians | 度与弧度的转换
A full revolution around a circle corresponds to an arc length equal to the circumference, 2πr. Substituting into θ = s / r gives θ = 2πr / r = 2π rad. Since a full revolution is also 360°, we obtain the key conversion: 360° = 2π rad, or equivalently 180° = π rad.
绕圆一整圈对应的弧长等于周长 2πr。代入 θ = s / r 得到 θ = 2πr / r = 2π rad。由于一整圈也等于 360°,我们得到关键换算关系:360° = 2π rad,即 180° = π rad。
| Degrees 度 | Radians 弧度 |
| 0° | 0 |
| 30° | π/6 |
| 45° | π/4 |
| 60° | π/3 |
| 90° | π/2 |
| 180° | π |
| 360° | 2π |
To convert from degrees to radians, multiply by π/180. To convert from radians to degrees, multiply by 180/π. In CIE examinations, answers involving angular quantities are almost always expected in radians unless the question explicitly requests degrees.
将度转换为弧度需乘以 π/180;将弧度转换为度需乘以 180/π。在 CIE 考试中,涉及角度的答案几乎总是要求以弧度给出,除非题目明确要求使用度。
3. Angular Displacement | 角位移
Angular displacement θ describes the change in angle of an object moving along a circular path. Unlike linear displacement, which is measured in metres, angular displacement is measured in radians. For one complete revolution, θ = 2π rad; for half a revolution, θ = π rad.
角位移 θ 描述物体沿圆周路径运动时的角度变化量。与以米为单位的线位移不同,角位移以弧度为单位。一整圈的角位移为 θ = 2π rad;半圈则为 π rad。
Angular displacement is a vector quantity in the sense that it has both magnitude and a direction of rotation (clockwise or anticlockwise). In CIE A-Level problems, we typically assign positive values to anticlockwise motion and negative values to clockwise motion, following the standard mathematical convention.
角位移在某种意义上是一个矢量,因为它既有大小又有旋转方向(顺时针或逆时针)。在 CIE A-Level 题目中,我们通常按照标准数学惯例,将逆时针运动取正值,顺时针运动取负值。
It is crucial to remember that the arc length and the angular displacement are related by s = rθ only when θ is expressed in radians. If θ were given in degrees, this simple relationship would fail, as the ratio s/r is dimensionless and independent of degree divisions.
务必牢记:只有当 θ 以弧度表示时,弧长与角位移的关系 s = rθ 才成立。若 θ 以度为单位,这一简单关系将失效,因为 s/r 是无量纲比值,与度的划分无关。
4. Angular Velocity | 角速度
Angular velocity ω is defined as the rate of change of angular displacement with respect to time:
角速度 ω 定义为角位移随时间的变化率:
ω = Δθ / Δt
The SI unit of angular velocity is radians per second (rad s⁻¹). For uniform circular motion — motion at constant speed along a circle — the angular velocity is constant, and the linear speed v of the particle is related to ω by v = rω.
角速度的国际单位是弧度每秒(rad s⁻¹)。对于匀速圆周运动——即物体沿圆以恒定速率运动——角速度恒定,质点的线速率 v 与 ω 的关系为 v = rω。
For an object completing n revolutions per unit time, the angular velocity can also be written as ω = 2πn. Since one full revolution corresponds to 2π radians, if an object makes f revolutions per second, then ω = 2πf = 2π/T, where T is the period (time for one revolution).
对于单位时间内完成 n 圈的物体,角速度可写为 ω = 2πn。由于一整圈对应 2π 弧度,若物体每秒完成 f 圈,则 ω = 2πf = 2π/T,其中 T 为周期(完成一圈所需时间)。
In exam questions, you will often be given the number of revolutions per minute (rpm). Convert this to revolutions per second first, then multiply by 2π to obtain ω in rad s⁻¹.
在考试题目中,常会给出每分钟转数(rpm)。应先将 rpm 转换为每秒转数,再乘以 2π 得到以 rad s⁻¹ 为单位的角速度。
5. Relationship between Linear and Angular Quantities | 线量与角量的关系
The connection between linear and angular quantities is one of the most important ideas in circular motion. For a particle at distance r from the axis of rotation, the linear speed is given by:
线量与角量之间的联系是圆周运动中最核心的概念之一。对于距转轴距离为 r 的质点,其线速率由下式给出:
v = rω
This equation tells us that for a fixed angular velocity, points farther from the centre move faster. For example, on a rotating turntable, a point near the rim travels a greater distance per revolution than a point near the centre, so it must have a higher linear speed.
该方程表明:在角速度固定的情况下,距圆心越远的点运动越快。例如,在旋转的转盘上,靠近边缘的点每圈走过的距离比靠近中心的点更大,因此其线速率必然更高。
The direction of the linear velocity at any instant is always tangent to the circular path — that is, perpendicular to the radius at that point. This is why linear velocity is sometimes called tangential velocity. While the speed is constant in uniform circular motion, the velocity is not constant because its direction changes continuously.
任意时刻线速度的方向始终与圆周路径相切——即在该点处垂直于半径。这就是为什么线速度有时也被称为切向速度。在匀速圆周运动中,虽然速率恒定,但速度并不恒定,因为其方向在持续改变。
Similarly, the linear distance travelled along the arc, s, relates to the total angular displacement by s = rθ, and the tangential acceleration (when angular velocity is changing) is aₜ = rα, where α is the angular acceleration.
同理,沿弧线走过的线距离 s 与总角位移的关系为 s = rθ;当角速度变化时,切向加速度为 aₜ = rα,其中 α 为角加速度。
6. Centripetal Acceleration | 向心加速度
Even when a particle moves at constant speed around a circle, it is accelerating because its velocity vector continuously changes direction. This acceleration is directed towards the centre of the circle and is therefore called centripetal acceleration.
即使质点以恒定速率绕圆运动,它依然在加速,因为其速度矢量方向在持续改变。该加速度指向圆心方向,因此被称为向心加速度。
Using the geometry of similar triangles in a velocity vector diagram, one can show that the magnitude of centripetal acceleration is:
利用速度矢量图中的相似三角形几何关系,可以证明向心加速度的大小为:
a = v² / r or a = rω²
The two forms are equivalent through v = rω: substituting v = rω into a = v²/r gives a = (rω)²/r = rω². Both forms appear regularly in CIE examination papers, and you should be comfortable using whichever is more convenient given the data provided.
两种形式通过 v = rω 等价:将 v = rω 代入 a = v²/r 即得 a = (rω)²/r = rω²。两种形式在 CIE 试卷中均频繁出现,你应当根据题目给出的已知量灵活选用更方便的形式。
Note that centripetal acceleration is measured in m s⁻², the same unit as linear acceleration. Despite its name, it represents a change in velocity direction, not necessarily a change in speed.
注意,向心加速度的单位是 m s⁻²,与线加速度相同。尽管名称中含有”加速度”,它代表的是速度方向的变化,而不一定是速率大小的变化。
7. Centripetal Force | 向心力
According to Newton’s second law, any acceleration requires a resultant force in the same direction. For circular motion, the resultant force that produces centripetal acceleration also points towards the centre of the circle. This force is called the centripetal force, and its magnitude is:
根据牛顿第二定律,任何加速度都需要同方向的合力。对于圆周运动,产生向心加速度的合力同样指向圆心方向。该力被称为向心力,其大小为:
F = mv² / r or F = mrω²
Centripetal force is not a new, independent force of nature. It is simply the name given to whatever real force — tension, gravity, friction, or the normal reaction — happens to be acting towards the centre. For a satellite in orbit, the centripetal force is gravity; for a car turning a corner, it is the friction between the tyres and the road; for a mass on a string, it is the tension in the string.
向心力并非自然界中一种新的独立力。它只是指向圆心的实际力——拉力、重力、摩擦力或法向反作用力——的名称。对于轨道上的卫星,向心力是重力;对于转弯的汽车,向心力是轮胎与路面之间的摩擦力;对于系在绳上的物体,向心力是绳中的张力。
On a banked track or a conical pendulum, components of existing forces combine to provide the centripetal force. In these cases, it is essential to resolve forces carefully and remember that the net force towards the centre equals mv²/r or mrω².
在倾斜轨道或圆锥摆情形中,现有各力的分量共同提供向心力。在这种情况下,务必仔细分解力,并牢记指向圆心的合力等于 mv²/r 或 mrω²。
8. Radians in Simple Harmonic Motion | 简谐运动中的弧度
The radian also plays a central role in simple harmonic motion (SHM), which is sometimes described as the projection of uniform circular motion onto a diameter. For a particle in SHM, the displacement x as a function of time is written as x = A sin(ωt) or x = A cos(ωt), where A is the amplitude and ω is the angular frequency in rad s⁻¹.
弧度在简谐运动(SHM)中也扮演核心角色,而简谐运动有时被描述为匀速圆周运动在直径上的投影。对于做简谐运动的质点,位移 x 随时间 t 的函数可写为 x = A sin(ωt) 或 x = A cos(ωt),其中 A 为振幅,ω 为角频率,单位为 rad s⁻¹。
In these equations, the argument of the sine or cosine function — ωt — is an angle measured in radians. When performing calculations, your calculator must be set to radian mode (RAD), not degree mode (DEG). A common student error is leaving the calculator in degree mode and obtaining incorrect phase angles.
在这些方程中,正弦或余弦函数的自变量——ωt——是以弧度量度的角度。进行数值计算时,计算器必须设为弧度模式(RAD),而非角度模式(DEG)。学生常犯的错误是忘记将计算器切换为弧度模式,从而导致相位角的计算结果错误。
The angular frequency ω in SHM is related to the period by ω = 2π/T = 2πf. In CIE formula booklets, this is often given alongside the definitions of centripetal acceleration, reinforcing the connection between circular motion and oscillatory motion.
简谐运动中的角频率 ω 与周期的关系为 ω = 2π/T = 2πf。在 CIE 公式手册中,此式通常与向心加速度的定义并列给出,强调了圆周运动与振荡运动之间的联系。
9. Worked Example | 例题解析
A particle moves in a horizontal circle of radius 0.50 m. It completes 40 revolutions in 20 seconds. Determine: (a) the angular velocity in rad s⁻¹, (b) the linear speed, (c) the centripetal acceleration, (d) the net force on the particle if its mass is 200 g.
一质点在半径 0.50 m 的水平圆上运动,20 秒内完成 40 圈。求:(a) 角速度(以 rad s⁻¹ 为单位);(b) 线速率;(c) 向心加速度;(d) 若质点的质量为 200 g,求其所受的合力。
Solution — Part (a): The frequency of revolution is f = 40 / 20 = 2.0 revolutions per second. Therefore the angular velocity is ω = 2πf = 2π × 2.0 = 4π ≈ 12.6 rad s⁻¹.
解答 — 第 (a) 部分:每秒转数为 f = 40 / 20 = 2.0 圈/秒。因此角速度为 ω = 2πf = 2π × 2.0 = 4π ≈ 12.6 rad s⁻¹。
Part (b): Using v = rω, we obtain v = 0.50 × 4π = 2π ≈ 6.28 m s⁻¹.
第 (b) 部分:由 v = rω,得 v = 0.50 × 4π = 2π ≈ 6.28 m s⁻¹。
Part (c): Using a = rω², we get a = 0.50 × (4π)² = 0.50 × 16π² = 8π² ≈ 78.96 m s⁻².
第 (c) 部分:由 a = rω²,得 a = 0.50 × (4π)² = 0.50 × 16π² = 8π² ≈ 78.96 m s⁻²。
Part (d): Converting mass to kilograms, m = 0.200 kg. The net force is F = mrω² = 0.200 × 0.50 × 16π² = 1.6π² ≈ 15.8 N, directed towards the centre of the circle.
第 (d) 部分:将质量换算为千克,m = 0.200 kg。合力 F = mrω² = 0.200 × 0.50 × 16π² = 1.6π² ≈ 15.8 N,方向指向圆心。
10. Common Exam Pitfalls | 常见考试易错点
One of the most frequent errors in CIE circular motion questions is using degrees instead of radians in the equation s = rθ or ω = 2πf. Always check whether the angle given in the problem is already in radians; if it is in degrees, convert it before substituting into any formula.
CIE 圆周运动题中最常见的错误之一,是在 s = rθ 或 ω = 2πf 等公式中误用度而非弧度。请始终检查题目给出的角是否已用弧度表示;若以度为单位,需先换算再代入任何公式。
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Forgetting that v = rω requires ω in rad s⁻¹ — mixing units (e.g., using rev min⁻¹ directly) will produce incorrect answers by a factor of 2π.
忘记 v = rω 中的 ω 必须为 rad s⁻¹——直接混用单位(如 rev min⁻¹)会使答案产生 2π 倍数的误差。
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Confusing angular velocity ω with frequency f. They are related by ω = 2πf, not ω = f. A particle spinning at 5 revolutions per second has ω = 10π rad s⁻¹, not 5 rad s⁻¹.
混淆角速度 ω 与频率 f。两者关系为 ω = 2πf,而非 ω = f。每秒转 5 圈的物体,其角速度为 ω = 10π rad s⁻¹,而非 5 rad s⁻¹。
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Using a = v²/r when the speed is changing (non-uniform circular motion). This formula gives only the centripetal component; a tangential component also exists, and the total acceleration is the vector sum.
在速率变化的(非匀速)圆周运动中误用 a = v²/r。该公式只给出向心分量;此时还存在切向分量,总加速度应为二者的矢量和。
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Neglecting that centripetal force is always a resultant force, not an additional force. In free-body diagrams, do not draw “centripetal force” as a separate arrow alongside tension or gravity.
忽视向心力永远是合力而非额外力。在受力分析图中,不要将”向心力”画作与拉力或重力并列的独立箭头。
Conclusion | 总结
The radian is far more than a convenient unit — it is the natural measure of angle for circular motion and oscillatory systems. Mastery of the definitions θ = s/r, ω = Δθ/Δt, and the derived relationships v = rω, a = rω² = v²/r, and F = mrω² is essential for success in CIE A-Level Physics. Consistent use of radians, careful unit conversion, and disciplined force analysis will carry you through even the most demanding rotation questions.
弧度远不止是一个方便的单位——它是圆周运动与振荡系统中角度的天然量度。熟练掌握 θ = s/r、ω = Δθ/Δt 的定义,以及派生关系 v = rω、a = rω² = v²/r 和 F = mrω²,是 CIE A-Level 物理取得成功的必要条件。坚持使用弧度、仔细进行单位换算、严谨进行受力分析,这些习惯将助你攻克最棘手的旋转类题目。
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