Table of Contents
Period ($T$) Of Circular Motion
The period $T$ of an object in circular motion is the time taken for the object to make one complete revolution.
- Unit: $s$ (seconds)
Frequency ($f$) Of Circular Motion
The frequency $f$ of an object in circular motion is the number of complete revolutions made by the object per unit time.
- Unit: $s^{-1}$ or Hz (hertz)
The relationship between period $T$ and frequency $f$ is given by the simple, yet fundamental equation:
$$T = \frac{1}{f}$$
Connection To Angular Velocity ($\omega$)
The time period $T$ and the frequency $f$ are intimately connected to the concept of angular velocity ($\omega$), which is the rate of change of angular displacement over time. After completing one full rotation (360 degrees or $2\pi$ radians), the angular displacement gives rise to the angular velocity equation:
$$\omega = \frac{2 \pi}{T}$$
Alternatively, this can be expressed in terms of frequency as:
$$\omega = 2 \pi f$$
Here, $f$ represents the frequency of rotation, providing a direct link between the rotational rate and angular velocity. Angular velocity is measured in radians per second ($\text{rad s}^{-1}$), underscoring the angular distance covered per unit of time.
From Angular to Linear: The Rotational Velocity Equation
A crucial equation bridges the gap between angular velocity ($\omega$) and linear or rotational velocity ($v$). Given that the arc length $s$ is equal to the product of the radius $r$ and the angular displacement $\theta$, and that velocity is the change in displacement over time, we can derive:
$$v = r \omega$$
This equation demonstrates that an object’s linear speed ($v$) during circular motion is a function of its distance from the center of rotation ($r$) and its angular velocity ($\omega$).
This principle is vividly illustrated in everyday examples, such as a playground merry-go-round, where individuals positioned further from the center travel faster than those near the center, despite sharing the same angular velocity. This is because their linear velocity is amplified by a greater radius.
[Optional] Derivation Of Rotational Velocity Equation
Linear velocity, denoted as $v$, is defined by the equation:
$$v = \frac{\Delta s}{\Delta t}$$
where $\Delta s$ represents the change in displacement over the time interval $\Delta t$. In the scenario of circular motion, the displacement in question corresponds to the length of the arc traversed, symbolized by $s$, which can be calculated using the formula $s = \theta r$, where $\theta$ is the angular displacement in radians and $r$ is the radius of the circular path.
Substituting the expression for $s$ into the formula for linear velocity, we obtain:
$$v = \frac{r \Delta \theta}{\Delta t}$$
In the realm of rotational dynamics, angular velocity, represented by $\omega$, is defined as the rate of change of angular displacement over time, which is mathematically expressed as $\omega = \frac{\Delta \theta}{\Delta t}$. By substituting this relationship into the previous equation, we derive the formula for linear velocity in terms of angular velocity:
$$v = r \omega$$
This equation succinctly relates linear velocity to angular velocity ($\omega$) and the radius ($r$) of the circular path, highlighting a fundamental connection between linear and rotational motion metrics.
Worked Examples
Example 1
The Earth’s radius is 6400 km, and the Shetland Isles are situated at a latitude of 60°.
a) Determine the Earth’s angular velocity.
b) Compute the rotational velocity of a point located on the equator.
c) Calculate the rotational velocity of the Shetland Isles.
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a) The formula for angular velocity $\omega$ is given by:
$$\omega = \frac{2\pi}{T}$$
Where $T$ is the time period for one complete rotation. For earth rotation, the time period of one complete rotation is 24 hours or 86400 seconds.
$$\begin{aligned} \omega &= \frac{2\pi}{T} \\ &= \frac{2 \pi}{86400} \\ &= 7.27 \times 10^{-5} \text{ rad s}^{-1}\end{aligned}$$
b) The rotational velocity $v$ of a point on the equator is given by:
$$v = \omega \times r$$
Where: $r$ is the radius of the Earth.
$$\begin{aligned} v &= \omega \times r \\ &= (7.27 \times 10^{-5}) \times (6400 \times 1000) \\ &= 465 \text{ m s}^{-1} \end{aligned}$$
c) To calculate the rotational velocity of the Shetland Isles at a latitude $\lambda$, the formula is:
$$v = \omega \times r \times \cos(\lambda)$$
Where:
$\omega$ is the angular velocity,
$r$ is the radius of the Earth, and
$\cos(\lambda)$ is the cosine of the latitude.
$$\begin{aligned} v &= \omega \times r \times \cos(\lambda) \\ &= (7.27 \times 10^{-5}) \times (6400 \times 1000) \times \cos(60^{\circ}) \\ &= 465.42 \times \cos(60^{\circ}) \\ &= 233 \text{ m s}^{-1} \end{aligned}$$
Example 2: Converting Angular Velocity to Linear Velocity
A bicycle wheel of radius 0.5 meters is spinning at an angular velocity of $4 \text{ rad/s}$. Calculate the linear velocity of a point on the rim of the wheel.
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The linear velocity ($v$) can be found using the relationship $v = r\omega$, where $r$ is the radius and $\omega$ is the angular velocity.
$$v = 0.5 \text{ m} \times 4 \text{ rad/s} = 2 \text{ m/s}$$
The linear velocity of a point on the rim of the bicycle wheel is 2 m/s.
Example 3: Understanding Period and Frequency
A Ferris wheel completes 3 full rotations in 90 seconds. What are the period and frequency of the Ferris wheel’s rotation?
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- Period, $T$: The period is the time taken for one complete rotation. Since the Ferris wheel completes 3 rotations in 90 seconds, the time for one rotation is $90 \div 3 = 30$ seconds. So, $T = 30$ seconds.
- Frequency, $f$: The frequency is the number of rotations per second, which can be calculated as $f = \frac{1}{T} = \frac{1}{30} = 0.0333 \text{ Hz}$.
Example 4: Calculating Angular Velocity
If a record player spins at a frequency of 45 revolutions per minute (RPM), what is its angular velocity in radians per second?
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- First, convert the frequency to Hz: $45 \, \text{RPM} = \frac{45}{60} = 0.75 \, \text{Hz}$.
- Angular velocity $\omega = 2\pi f = 2\pi \times 0.75 \approx 4.71 \, \text{rad/s}$.
Example 5: From Angular to Linear Velocity
A bicycle’s wheel has a radius of 0.5 meters, and it rotates at an angular velocity of 2 radians per second. What is the linear velocity of a point on the rim of the wheel?
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$$v = r\omega = 0.5 \times 2 = 1 \, \text{m/s}$$
Example 6: Frequency from Period
A satellite completes an orbit around Earth in 2 hours. Determine its frequency in revolutions per hour (RPH) and Hertz (Hz).
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- RPH: Since it completes 1 orbit in 2 hours, its frequency is $0.5 \, \text{RPH}$.
- Hz: To convert RPH to Hz, $0.5 \, \text{RPH} = \frac{0.5}{3600} \approx 1.39 \times 10^{-4} \, \text{Hz}$ (since there are 3600 seconds in an hour).
Example 7: Relating Period, Frequency, and Angular Velocity
A merry-go-round makes one complete turn in 8 seconds. Calculate its period, frequency, and angular velocity.
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- Period (T): $T = 8$ seconds.
- Frequency (f): $f = \frac{1}{T} = \frac{1}{8} = 0.125 \text{ Hz}$.
- Angular Velocity ($\omega$): $\omega = 2\pi f = 2\pi \times 0.125 = \pi / 4 \approx 0.785 \, \text{rad/s}$.
Example 8: Comparing Linear Velocities
Two points are located on a spinning disc, one at a radius of 0.2 meters and the other at 0.4 meters. If the disc spins at a frequency of 10 Hz, what are the linear velocities of these two points?
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- Angular Velocity ($\omega$): $\omega = 2\pi f = 2\pi \times 10 = 20\pi \, \text{rad/s}$.
- Linear Velocity of Point 1 ($v_1$): $v_1 = r_1\omega = 0.2 \times 20\pi = 4\pi \, \text{m/s}$.
- Linear Velocity of Point 2 ($v_2$): $v_2 = r_2\omega = 0.4 \times 20\pi = 8\pi \, \text{m/s}$.