## What causes circular error? A search on Google provided many links to articles on the subject, but I could not find any that said "why." This page is designed to answer that question in a reader-friendly manner: if you want to, you can scroll down when you get to the maths, skip the maths, go to the graphs and continue reading. This page is also designed for readers with smartphones, which is why some of the images are presented smaller than original.

There are numerous forces acting upon a pendulum as it swings back and forth in a mechanical clock, such as gravity, elastic energy from the suspension spring, and air resistance. On this page, the subject is gravity. It is well known among clockmakers that when the angle of swing changes, the accuracy of the timekeeping changes in clocks. The effect of gravity upon timekeeping accuracy can be measured by finding how long it takes for the pendulum to go over and back. The time it takes to go over and back is known as the period.

The moment a pendulum is released, gravity pulls it straight down, and a portion of that pull acts to pull the pendulum towards its vertical position, depending on the angle, the length of the pendulum, and the force of gravity, given by the following equation, in which acceleration is theta with an umlaut (two dots) over it: In a computer spreadsheet, the acceleration acting upon the pendulum can therefore be calculated for each moment in time, a small fraction of a second. Then the speed (angular velocity) of the pendulum is found by multiplying the acceleration by the amount of time (a small fraction of a second). The distance traveled (arc) in that amount of time is found by multiplying the angular velocity by the amount of time. The angle in radians is found by dividing the distance by the length of the pendulum. Then the angle in degrees is found by multiplying the angle in radians by 180 and dividing by pi (3.14). The results come together in a chart like this one. The formula in each cell of the spreadsheet is written so that the angle can be changed and the rest of the chart will be re-calculated to find how long it takes for the pendulum to reach the other side. In this chart, the angle shown is 13° and it takes one second for the pendulum to reach the other side. That is expected because a one-second pendulum is 39.1 inches (0.994 metres) long. When the pendulum reaches the other side, it changes direction to swing back, and this is seen in the chart when the velocity becomes negative. You can click on the chart below to see it full size: make your own chart and experiment with it.

When the angle is changed to 45°, it takes 1.0367 seconds for the pendulum to swing from one side to the other, almost 4% longer. Since time taken becomes longer, a clock would be seen to be losing time. The position of the pendulum (its angle) affects how gravity acts upon it, and the result is that the acceleration changes continuously. You can click on each one of all the graphs below to see it full size.

For a 13° arc from vertical:

The effect becomes more obvious for large angles.

For a 90° arc from vertical:

At 180°, the period goes to infinity.
For a 179° arc from vertical:

Looking at several graphs below, we can see that, as the angle increases, the height (amplitude) of the acceleration curve increases, but at a declining rate: when the angle doubles, the acceleration increases by less than double.

Beyond 90°, the acceleration curve no longer reaches a higher high, and forms what looks like a wave within a wave.

And around and around we go:

Looking more closely at the graph, we can see that the period is 2 seconds (2.00664) when the arc is 13°.

However, graph shows us that the period is 2.3 seconds (2.3532) when the arc is 90°. It takes longer for the pendulum to swing over and back.

The Cause of Circular Error:

When the angle is doubled, the pendulum swings twice as far, but the acceleration does not double, and so the speed does not double either. If the pendulum swings twice as far and the speed does not double, then it takes longer to reach the other side: the period increases. The change in the period with changing angle is called circular error.

Note that I am referring to peak angular acceleration and peak angular velocity here.

The graphs below show how the period increases rapidly (exponentially) as the angle increases. The period is the time it takes to go back and forth, which is two seconds in this example. The curves are not perfectly smooth because of small rounding errors in the data.

The graph shows that the period reaches two seconds when the angle reaches 13°. This means that the period is less than two seconds for smaller angles, causing a clock to gain time, but greater than two seconds for larger angles, causing a clock to lose time as a result of circular error. Notice that, for small angles, of 3° or less, the curve becomes flat because of what is called Linearization (when sinθ is approximately equal to θ).

Changing the Length:

Performing similar calculations by changing the length of the pendulum, but keeping the amplitude unchanged at 13°, shows that the pendulum length has a stronger effect upon circular error. In the chart below, the left column shows the expected period (time taken to go back and forth) in seconds. The next column shows the pendulum length in metres for the corresponding period. The right column shows the calculated period, using the spreadsheet at the top of this page. The graph below shows the expected period on the horizontal line (X axis) and the calculated period on the vertical line (Y axis). The data compares the one-second pendulum, which has an expected period and a calculated period of 2 seconds, with the periods for a pendulum of other lengths. The blue line shows what the line would look like without circular error (Y=X).

Looking at the same one-second pendulum and adding a suspension spring, we get new graphs. The coefficient of elasticity of a spring deflected by bending remains constant, which is more or less true for small angles of 3° or less. In this example, I assume that the initial force applied by the suspension spring is equal to the initial force applied by gravity to bring the pendulum back to a vertical position, and the two forces are added together. Looking at a pendulum with an arc of only 3°, the graph for gravity looks like this one.

When a suspension spring is added in this simulation, the acceleration increases, the velocity remains the same, the angle decreases, and the period decreases.

When a stronger suspension spring is added, the acceleration increases further, the velocity remains the same, the angle decreases further, and the period decreases further. When an escapement is added to keep a pendulum going, as in a clock, the acceleration increases because there are now three forces acting upon the pendulum: the force of gravity, which is a function of sinθ, the elastic force from the suspension spring, which is a function of θ, and the force from the Graham escapement, as the escape wheel's tooth slides across the pallet's impulse face. In this example, the pallet has an arc of 6° and the pendulum has an arc of 3°, so the peak acceleration from the escapement that reaches the pendulum is multiplied by cos2θ, which has a range of 0.997 and 1 when the arc is 6°. The force of the escapement changes direction when the velocity of the pendulum changes direction. Acceleration gets out of control.

Therefore, an energy loss (resistance) needs to be introduced into the equation, such that the energy gains from the escapement are equal to the energy losses from air resistance, the bending of the suspension spring, and so on. The result makes for an interesting graph.

When the energy from the escapement is increased, the acceleration, the velocity, and the angle increase, until an angle is reached when the energy losses become equal to the energy gains from the escapement, and an equilibrium is reached.

The amplitudes of the curves are greater at equilibrium. The period remains unchanged.

However, when the energy losses are also increased in proportion to energy gains in this simulation, the amplitudes and the period remain unchanged. From the point of view of clock repair, the simulation offers insight into the forces that act upon a pendulum and affect timekeeping accuracy.
1. If you use a stronger suspension spring, the period will decrease significantly and the clock will gain time. The angle will also decrease, so a stronger mainspring or a heavier weight may be needed to keep the clock running.
2. The simulation suggests that increasing the energy from the escapement would not affect the period. In practice, I have found that using a stronger mainspring or a heavier weight will decrease the period slightly, so the clock will gain time.

I would like to thank Dr. Bernstein for his extraordinary patience, guidance and support.

Dennis S. Bernstein
ScB, MSE, PhD
Computer, Information and Control Engineering

James E. Knott Professor
Department of Aerospace Engineering
University of Michigan Ann Arbor

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