A simple pendulum is a fundamental concept in physics used to study oscillatory motion. It consists of a point mass, often called a bob, suspended by a light, inextensible string from a fixed support. When the bob is pulled to one side and released, it swings back and forth due to gravity, exhibiting periodic motion.
The time period of a simple pendulum is defined as the time taken for one complete oscillation (a swing from one extreme position to the other and back to the starting extreme position).
The time period ($T$) of a simple pendulum for small angular displacements is determined by its length ($L$) and the acceleration due to gravity ($g$) at the location. The formula that describes this relationship is:
$T = 2\pi \sqrt{\frac{L}{g}}$
Where:
We are given that the length of the pendulum is $L = 1 \, m$. We will use the standard value for the acceleration due to gravity, $g \approx 9.8 \, m/s^2$.
Substitute these values into the formula for the time period:
$T = 2\pi \sqrt{\frac{1 \, m}{9.8 \, m/s^2}}$
First, calculate the value inside the square root:
$\frac{1}{9.8} \approx 0.10204 \, s^2$
Now, take the square root:
$\sqrt{0.10204 \, s^2} \approx 0.3194 \, s$
Finally, multiply by $2\pi$ (using $\pi \approx 3.14159$):
$T \approx 2 \times 3.14159 \times 0.3194 \, s$
$T \approx 6.28318 \times 0.3194 \, s$
$T \approx 2.006 \, s$
The calculated time period for a 1 m long pendulum is approximately 2.006 seconds. Let's look at the provided options:
The calculated value $2.006 \, s$ is extremely close to 2 seconds. Therefore, the time period of a 1 m long pendulum approximates to 2 seconds.
| Parameter | Value Used |
|---|---|
| Pendulum Length ($L$) | 1 m |
| Acceleration due to Gravity ($g$) | $\approx 9.8 \, m/s^2$ |
| Calculated Time Period ($T$) | $\approx 2.006 \, s$ |
| Factor | Effect on Time Period ($T$) | Relationship |
|---|---|---|
| Length ($L$) | $T$ increases with increasing $L$ | $T \propto \sqrt{L}$ |
| Acceleration due to Gravity ($g$) | $T$ decreases with increasing $g$ | $T \propto \frac{1}{\sqrt{g}}$ |
| Mass of the Bob | $T$ is independent of mass (for simple pendulum idealization) | N/A |
| Amplitude (small angles) | $T$ is independent of amplitude (for angles < approx. 15°) | N/A |
The formula used for the time period of a simple pendulum assumes that the oscillations are small (amplitude is small). When the amplitude is large, the motion is not perfectly simple harmonic, and the actual time period is slightly longer than that given by the formula.
The value of $g$ is not constant across the Earth's surface. It varies slightly with latitude, altitude, and local geological structure. This means that a pendulum clock would run at a slightly different rate if moved from one location to another with a different value of $g$.
For practical pendulums (physical pendulums) which have distributed mass rather than a point mass bob, the time period calculation involves the moment of inertia about the pivot point and the distance to the center of mass.
Which one of the following statements regarding simple pendulum is correct?
Simple pendulum has a time period independent of amplitude:
The bob of a simple pendulum is displaced from its mean position and then released from rest 0.20 m above its mean position. What is the speed of the bob as it passes through the mean position? (Take \(g = 10 \, m/s^2\))
What will be the time period of oscillation, if the length of a second pendulum is one third?
Two pendulums oscillate with a constant phase difference of 90°. If time period of one of them is 2 sec., then period of the other is
The period (T) for the pendulum with length (l) and placed at the gravitational acceleration (g) is given by:
Two pendulums of length $169$ cm and $144$ cm start vibrating in phase. At some instant, the two are at their mean position in the same phase. The minimum number of vibrations of the shorter pendulum after which the two are again in phase at the mean position is:
Which one of the following statements regarding simple pendulum is correct?
Simple pendulum has a time period independent of amplitude: