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Page 469: Lesson Check
The period of a pendulum oscillating due to gravity can be found using the length of the pendulum $L$ as follows:
$$
begin{equation}
T = 2 , pi sqrt{frac{L}{g}}
end{equation}
$$
By looking at formula (1) we can see that the period $T$ of the pendulum is proportional to the square root of the length of the pendulum $L$, that is:
$$
begin{align*}
T sim sqrt{L}
end{align*}
$$
From this it is obvious that an increase in the length of the pendulum $L$ will lead to an increase in the pendulum’s period $T$.
We know that the maximal potential energy the pendulum has during its motion is when it is in the amplitude position.
So we conclude that pendulum A has larger maximal potential energy than pendulum B.
This means that pendulum A has larger total energy than pendulum B, since energy is conserved during the motion.
When expired as kinetic energy, we see that pendulum A has larger speed than pendulum B.
The same conclusion could have been reached simply by stating that pendulum A, in average, has to have greater speed than pendulum B because it has to move a larger distance in the same period of time.
The period of a pendulum oscillating due to gravity can be found using the length of the pendulum $L$ as follows:
$$
begin{equation}
T = 2 , pi sqrt{frac{L}{g}}
end{equation}
$$
We need to find the period of a swing of length $L = 3text{ m}$ at a location where the gravitational acceleration is $g = 9.81 ; frac{text{m}}{text{s}^2}$. We do this using formula (1):
$$
begin{align*}
T = 2 , pi sqrt{frac{L}{g}}
end{align*}
$$
Plugging in the numbers we get:
$$
begin{align*}
T &= 2 , pi sqrt{frac{3text{ m}}{9.81 ; frac{text{m}}{text{s}^2}}} \
T &= 3.47text{ s}
end{align*}
$$
The period of a pendulum oscillating due to gravity can be found using the length of the pendulum $L$ as follows:
$$
begin{equation}
T = 2 , pi sqrt{frac{L}{g}}
end{equation}
$$
We know that the period of the pendulum is $T = 1text{ s}$
We will use formula (1) to find the length of the pendulum.
First we need to rearrange it for $L$ as follows:
$$
begin{align*}
T &= 2 , pi sqrt{frac{L}{g}} \
T^2 &= 4 , pi^2 left(frac{L}{g} right) \
L &= left(frac{T}{2 , pi} right)^2 cdot g
end{align*}
$$
Plugging in the values we get:
$$
begin{align*}
L &= left(frac{1text{ s}}{2 , pi} right)^2 cdot 9.81 ; frac{text{m}}{text{s}^2} \
L &= 0.248text{ m} approx 0.25text{ m}
end{align*}
$$
The period of a pendulum oscillating due to gravity can be found using the length of the pendulum $L$ as follows:
$$
begin{equation}
T = 2 , pi sqrt{frac{L}{g}}
end{equation}
$$
Firstly we find the period since we know that the pendulum performs 5 oscillations in 16s. This is done as follows:
$$
begin{align*}
T = frac{t}{n} = frac{16text{ s}}{5} = 3.2text{ s}
end{align*}
$$
Now to find the intensity of the gravitational acceleration at the location of the pendulum. This can be done using formula (1), since we know the length $L = 2.5text{ m}$ and the period $T = 3.2text{ s}$, as follows:
$$
begin{align*}
T = 2 , pi sqrt{frac{L}{g}}
end{align*}
$$
$$
begin{align*}
T &= 2 , pi sqrt{frac{L}{g}} \
T^2 &= 4 , pi^2 left(frac{L}{g} right) \
g &= frac{4 , pi^2 , L}{T^2}
end{align*}
$$
Plugging in the numbers we get:
$$
begin{align*}
g = frac{4 , pi^2 cdot 2.5text{ m}}{(3.2text{ s})^2} = 9.63 ; frac{text{m}}{text{s}^2}
end{align*}
$$
g = 9.63 ; frac{text{m}}{text{s}^2}
$$