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Frequency and Period of SHM

Lesson ~10 min read 8 MCQs

In simple terms: In simple terms, this topic is about the timing of back-and-forth motion, like a swing or a bouncing spring. We'll learn how to calculate how long one cycle takes (period) and how many cycles happen per second (frequency).

Why this matters

Imagine you’re at a park in Boston, pushing your younger cousin, Leo, on a swing. You give him a small push, and he swings back and forth, back and forth. You notice that whether you give him a tiny push or a slightly bigger one, the time it takes for him to swing out and come back to you seems to be the same. It's like the swing has its own natural rhythm.

Now, what if an adult, who is much heavier than Leo, gets on the same swing? Or what if you could magically shorten the swing's chains? Would the rhythm change? This timing—the steady beat of an oscillation—is what physicists call the period and frequency. Understanding it is key to describing everything from a swaying skyscraper in the wind to the vibrations of a guitar string. In this lesson, we'll get the formulas to predict this rhythm perfectly.

Concept overview

flowchart TD
    A[Start: Analyze the oscillating system] --> B{Is it a mass on a spring?};
    B -- Yes --> C[Use Spring Period Formula];
    C --> D[T = 2π * sqrt(m/k)];
    D --> E[Period depends on Mass (m) and Spring Constant (k)];
    E --> F[Period does NOT depend on Amplitude (A)];

    B -- No --> G{Is it a mass on a string (pendulum)?};
    G -- Yes --> H[Use Pendulum Period Formula];
    H --> I[T = 2π * sqrt(L/g)];
    I --> J[Period depends on Length (L) and Gravity (g)];
    J --> K[Period does NOT depend on Mass (m) or Amplitude (A)];

    F --> L[End];
    K --> L[End];
    G -- No --> M[Not simple harmonic motion covered in this topic];
    M --> L;
A flowchart that guides students in choosing the correct formula for calculating the period of an oscillating system. It branches based on whether the system is a mass-on-a-spring or a pendulum, showing the respective formulas and listing what variables the period does and does not depend on for each case.

Core explanation

When an object is in Simple Harmonic Motion, it follows a predictable, repeating pattern. The two most fundamental ways we measure this pattern are with period and frequency.

Period vs. Frequency: Two Sides of the Same Coin

Let's get our definitions straight first.

  • Period (T)
    This is the time it takes to complete one full cycle of motion. The unit for period is seconds (s). If a pendulum takes 3 seconds to swing from its starting point, all the way to the other side, and back to the start, its period is T = 3 s.
  • Frequency (f)
    This is the number of cycles completed in one second. The unit for frequency is Hertz (Hz), where 1 Hz = 1 cycle/second. If a spring bobs up and down 4 times every second, its frequency is f = 4 Hz.

They measure the same underlying rhythm, just from different perspectives. This leads to a beautifully simple relationship:

T = 1 / f

Think about it: if the period is long (it takes a lot of time for one cycle), the frequency must be low (you complete very few cycles per second). If the period is short (a cycle is super fast), the frequency must be high (you can fit many cycles into one second).

The Period of a Mass-Spring System

Now, let's look at our first classic SHM example: a mass attached to an ideal spring, sliding on a frictionless surface. What determines its period? It comes down to two things: the mass (m) and the spring's stiffness, represented by the spring constant (k).

The formula for the period of a mass-spring oscillator is:

T_s = 2π * √(m / k)

Let's break this down so it feels intuitive.

  • Mass (m)
    The mass is in the numerator, under the square root. This means if you increase the mass, you increase the period. This makes sense! A heavier block has more inertia, making it harder for the spring to pull and push. It will oscillate more slowly.
  • Spring Constant (k)
    The spring constant is in the denominator. A higher k means a stiffer spring. If you increase the spring constant, you decrease the period. This also makes sense. A stiffer spring exerts a stronger restoring force, snapping the mass back and forth more quickly.

The Period of a Simple Pendulum

Our second classic example is a simple pendulum: a mass (called a bob) hanging from a string of length l. For a pendulum, the restoring force is a component of gravity.

The formula for the period of a simple pendulum, for small angles (less than about 15°), is:

T_p = 2π * √(l / g)

Let's analyze this one too.

  • Length (l)
    The length of the string is in the numerator. If you increase the length, you increase the period. Think of the swing set at the park. A long swing has a slow, lazy rhythm. A short one swings back and forth much faster.
  • Gravitational Acceleration (g)
    The value of g (about 9.8 m/s² on Earth) is in the denominator. If you were to take your pendulum to the Moon, where g is much smaller, the period would increase. The weaker gravity would provide a weaker restoring force, making the pendulum swing more slowly.

Here's the other big trap: What does the period of a simple pendulum not depend on? Two things!

  1. 1
    Mass (m)
    Look at the formula—mass isn't in it! This is very counter-intuitive. A 1 kg bob and a 10 kg bob on identical strings will have the exact same period. On the AP exam, this is a very common conceptual question.
  2. 2
    Amplitude (for small angles)
    Just like the spring, as long as you don't pull the pendulum back too far, the angle of release doesn't affect the period.

These two formulas are your essential tools for calculating the timing of any SHM system you'll see in this course. Master them, and you've mastered this topic.

Worked examples

Example 1

Calculating the Rhythm of a Spring

Problem: A 0.5 kg block is attached to a horizontal spring with a spring constant of 50 N/m. The block is pulled 10 cm from its equilibrium position and released. What are the period and frequency of the oscillation?

Solution:

  1. 1
    Identify the system and your goal
    We have a mass-spring system. We need to find the period (T) and frequency (f).
  2. 2
    Choose the correct formula
    For a mass-spring system, the period is given by: T_s = 2π * √(m / k)
  3. 3
    Check the variables
    The problem gives us m = 0.5 kg and k = 50 N/m. What about the 10 cm displacement? Remember, for an ideal spring, the period does not depend on the amplitude. That 10 cm is extra information designed to see if you know this concept. We don't need it for this calculation.
  4. 4
    Plug in the values and solve for the period
    T_s = 2π * √(0.5 kg / 50 N/m) T_s = 2π * √(0.01 s²) T_s = 2π * (0.1 s) T_s ≈ 0.628 s

    So, it takes about 0.63 seconds for the block to complete one full back-and-forth cycle.

  5. 5
    Calculate the frequency
    Frequency is the inverse of the period. f = 1 / T f = 1 / 0.628 s f ≈ 1.59 Hz

    This means the block completes about 1.6 oscillations every second.

Example 2

Conceptual Pendulum Problem

Problem: Priya has a pendulum with a period of 2.0 seconds. She wants to create a new pendulum with a period of 4.0 seconds. How should she change the length of the pendulum's string?

Solution:

  1. 1
    Identify the relationship
    This is a proportional reasoning problem. We need to relate the period of a pendulum (T_p) to its length (l). The formula is: T_p = 2π * √(l / g)
  2. 2
    Analyze the proportion
    The period T_p is directly proportional to the square root of the length l. We can write this as T ∝ √l.
  3. 3
    Set up the ratio
    We want to find the new length (l_new) relative to the old length (l_old). We know the new period (T_new = 4.0 s) is double the old period (T_old = 2.0 s). T_new / T_old = √(l_new / l_old)
  4. 4
    Solve for the change in length
    4.0 s / 2.0 s = √(l_new / l_old) 2 = √(l_new / l_old)

    To get rid of the square root, we square both sides of the equation: 2² = l_new / l_old 4 = l_new / l_old l_new = 4 * l_old

Try it yourself

Problem 1

A car's suspension can be modeled as a 1200 kg mass sitting on four springs, each with a spring constant k = 25,000 N/m. If the car hits a bump and starts oscillating up and down, what is the approximate period of this oscillation? (Assume the mass is distributed evenly).

Problem 2

An astronaut on a new planet wants to measure the local acceleration due to gravity, g. She builds a simple pendulum with a string of length 0.80 m. She measures the time for 10 full swings to be 25.0 seconds. What is the value of g on this planet?