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Parliamentary video of the pendulum of the great clock |
The Great Clock of Parliament
(Big Ben) uses a pendulum to keep time. Fine adjustment of the pendulum is accomplished by adding old (pre-decimal) pennies to the pendulum. According to the website of Parliament, each 9.4 g penny used to adjust the clock is added to the pendulum in such a way that the clock mechanism speeds up enough to gain two fifths of one second in 24 hours of operation. Further, the website reports that the pendulum rod has a mass of 321 kg and a length of 4.48 m, and the bob attached to the rod has a mass of 203 kg.
Part A
Assuming that the rod is thin and uniform and that the bob can be treated as a point particle, what is the approximate period of Big Ben's pendulum?
System: Rod and pendulum bob together as a single rigid body.
Interactions: Both components of the system are subject to external influences from the earth ([gravity]). The rod is also subject to an external influence from the axle of the pendulum. We will consider [torques] about the axle of the pendulum. Because of this choice of axis, the external force exerted by the axle on the pendulum will produce no [torque], and so it is not relevant to the problem.
Model: Single-Axis Rotation of a Rigid Body and Simple Harmonic Motion.
Approach:
Diagrammatic Representation:
We begin with a force diagram:
Mathematical Representation
Looking at the force diagram, we can see that the total [torque] from [gravity] about the axis of rotation is given by:
\begin
[ \tau = -m_
g\frac
\sin\theta - m_
gL\sin\theta ]\end
The moment of inertia of the composite pendulum is the sum of the moment of inertia of the thin rod rotated about one end plus the moment of inertia of the bob treated as a point particle:
\begin
[ I_
= \frac
m_
L^
+ m_
L^
]\end
With these two pieces of information, we can write the rotational version of Newton's 2nd Law as:
\begin
[ \left(\frac
m_
L^
+ m_
L^
\right)\alpha = - \left(m_
g\frac
+ m_
gL\right)\sin\theta ]\end
We can now perform some algebra to isolate α:
\begin
[ \alpha = -\left(\frac{\frac
m_
+m_{\rm bob}}{\frac
m_
+m_{\rm bob}}\right)\frac
\sin\theta]\end
This equation is not yet of the form required by the Simple Harmonic Motion model, since α is not directly proportional to θ. To achieve the form required by the Simple Harmonic Motion model, we must make the standard small angle approximation which is generally applied to pendulums. In the small angle approximation, the sine of θ is approximately equal to θ. Thus, we have:
\begin
[ \alpha \approx -\left(\frac{\frac
m_
+m_{\rm bob}}{\frac
m_
+m_{\rm bob}}\right)\frac
\theta ] \end
which is of the proper form for Simple Harmonic Motion with the natural angular frequency given by:
\begin
[ \omega = \sqrt{\left(\frac{\frac
m_
+m_{\rm bob}}{\frac
m_
+m_{\rm bob}}\right)\frac
{L}} ]\end
We are asked for the period of the motion, which is related to the natural angular frequency by the relationship:
\begin
[ T = \frac
= 2\pi\sqrt{\left(\frac{\frac
m_
+m_{\rm bob}}{\frac
m_
+m_{\rm bob}}\frac
{g}} = 3.92 s]\end
The website of Parliament claims that the "duration of pendulum beat" is 2 seconds. This seems to contradict our calculation. Can you explain the discrepancy? Check your explanation using the video at the top of this page.