Tide-Predicting Machine No. 2

Last updated

Tide-Predicting Machine No. 2, also known as Old Brass Brains, [1] was a special-purpose mechanical computer that uses gears, pulleys, chains, and other mechanical components to compute the height and time of high and low tides for specific locations. The machine can perform tide calculations much faster than a person could do with pencil and paper. The United States Coast and Geodetic Survey put the machine into operation in 1910. It was used until 1965, when it was replaced by an electronic computer. [2]

Contents

Tide-Predicting Machine No. 2
Tide Predicting Machine No. 2 ("Old Brass Brains").jpg
Tide Predicting Machine No. 2
Date invented1895
ManufacturerUnited States Coast and Geodetic Survey
Introduced1910
Discontinued1965
Weight2,500 pounds (1,134 kg)
Dimensions10.8 feet (3.3 m) long, 6.2 feet (1.9 m) high, 2 feet (0.6 m) wide

Early U.S. tide-prediction efforts

Tides are the rise and fall of sea levels caused by the combined effects of gravitational forces exerted by the Moon, Sun, and rotation of the Earth. In 1867 the United States Coast Survey started printing annual tide tables to support safe and effective maritime, coastal, and defense activities. [2] [3] Before long, these tables showed the times and heights of high and low tides to the nearest minute and tenth of a foot, respectively. Tables were printed for a year at a time and distributed prior to the start of the year. [3] [4]

The prediction of tides is very challenging as it depends on multiple factors–including the alignment of the Sun and Moon, the shape of the coastline, and near-shore bathymetry. Tide theories attempt to account for these factors but lead to complex calculations. Originally, calculations were performed by hand, which was very labor-intensive and error-prone. [5] The burden became even larger when the United States Coast and Geodetic Survey (as the U.S. Coast Survey was renamed in 1878) started using the more accurate harmonic method for predictions of tides in 1884. [3]

To significantly reduce the work required to predict tides, in 1881 William Ferrel of the Coast and Geodetic Survey designed a tide-predicting machine. Fauth & Co. Instrument Makers built Tide-Predicting Machine No. 1 and delivered it in 1882. The Survey started using the machine routinely in 1883. [6]

History and mechanism

In 1895 the Coast and Geodetic Survey grew concerned because Tide-Predicting Machine No. 1 had developed considerable wear from almost constant use over 12 years. The office decided to construct a new machine that was faster, more accurate, and more reliable. This became Tide-Predicting Machine No. 2. [4]

Rolin Harris and E. G. Fischer of the Coast and Geodetic Survey led the effort. [5] The design team studied previous British and U.S. tide-predicting machines and incorporated their best attributes in the design of the new machine. [6] The machine, also known as “Old Brass Brains”, used an intricate arrangement of gears, pulleys, slides, and other components. The design of the new machine was approved in 1895, and construction began in 1896. [4]

Tide-Predicting Machine No. 2 was the first tide-predicting machine to incorporate both a paper graph of the tides–the approach used by earlier British machines–and dials and scales that showed the tide height and corresponding date and time–used by Tide-Predicting Machine No. 1. The dials and scales made it much easier for an operator to precisely determine the height and time of high and low tides. The paper graph, referred to as a tide curve, was very useful as a record of the computation that could be checked later to confirm the calculations were performed correctly. [6]

A hand crank turned by the operator provides the power for the machine’s mechanical calculations. Battery-powered electrical circuits are used to mark the start of hours and days on the paper graph and to stop the machine when high and low tides were reached so the operator can note the height and time. [6]

This photo shows the largest of the three sections of Tide-Predicting Machine No. 2. The gears on the left transmit power from the hand crank. The components on the right contribute to the computation of the time of high and low tides. NOAA's Tide Predicting Machine No. 2.jpg
This photo shows the largest of the three sections of Tide-Predicting Machine No. 2. The gears on the left transmit power from the hand crank. The components on the right contribute to the computation of the time of high and low tides.

Much consideration was given to the mechanical characteristics of the components to ensure reliability and accuracy. For instance, some components that were hard to replace were designed with a 50-year lifetime. Also, the summation chains were moved across gears under tension for a year of work days before being installed in the machine to ensure they were sufficiently flexible and their length would remain constant. [5]

Other work in the Coast and Geodetic Surevy took precedence over construction of the new machine, and a reduction in staff levels precluded all work on the new machine for three years. As a result, Tide-Predicting Machine No. 2 was not functional until 1910. [6] It was first applied to predicting values for the 1912 and 1913 tide tables. Then the machine was disassembled, polished, plated, lacquered, and reassembled in time to provide predictions for the 1914 tide tables. [5] Comparisons of the accuracy of the mechanical predictions of tides compared to hand calculations for two challenging locations demonstrated errors in heights of 0.72 inches (1.83 cm) or less. [4] [6]

Old Brass Brains is 10.8 feet (3.3 m) long, 6.2 feet (1.9 m) high, 2 feet (0.6 m) wide [5] and weighs approximately 2,500 pounds (1,134 kg). [7]

Use

To compute tides for a coastal location, the operator has to configure the machine for that location. This is done by adjusting physical settings on the machine based on up to 37 factors. Those factors are determined empirically by harmonic analysis of a time series of tides at the location, [6] and represent the influence of the moon, sun, depth of bay, offshore islands, etc. [2] Once computed the factors for a location can be applied to past and future years. [3] and are shared widely so anyone can perform tide calculations. [6]

A tide formula component crank on Tide-Predicting Machine No. 2. The mechanical arrangement (a slotted crank yoke) converts circular motion to a vertical motion that traces a sinusoid. The operator adjusts the position of the pin on the crank to represent a component of the tide formula at a specific coastal port before starting computations. The pin position affects the amplitude and phase of the sinusoid. A Tide Formula Component Crank on Tide Predicting Machine No. 2.jpg
A tide formula component crank on Tide-Predicting Machine No. 2. The mechanical arrangement (a slotted crank yoke) converts circular motion to a vertical motion that traces a sinusoid. The operator adjusts the position of the pin on the crank to represent a component of the tide formula at a specific coastal port before starting computations. The pin position affects the amplitude and phase of the sinusoid.

Assuming the factors for a location are known, configuring the machine to compute tides for the location requires 2.5–4 hours. Predictions for a year’s tides at that location can then be produced in 8–15 hours. [6] The calculations Tide-Predicting Machine No. 2 can perform in 1 day would require a person 125 days to perform by hand. [2]

Around 1915, the machine was used to produce annual tide tables for 70 major ports worldwide. [4] Additional ports were added in later years.

During World War II the Coast and Geodetic Survey produced annual tide tables for major ports four years in advance in case Old Brass Brains broke down or was sabotaged. [8] The Coast and Geodetic Survey also provided tide predictions for a number of additional locations in the Pacific, including potential locations for amphibious invasions. Obtaining tide observations for those locations to support computation of the factors required for predictions was often a significant challenge. [3]

Around 1960 Old Brass Brains was modified to replace the hand crank with an electric motor and to add an automatic readout of heights and times. [3] In 1965, the Coast and Geodetic Survey retired the Tide-Predicting Machine No. 2, 55 years after it entered service, and started performing its tide calculations with an electronic computer. [2]

Current status

The National Oceanic and Atmospheric Administration (NOAA) maintains Tide-Predicting Machine No. 2 in working condition. The machine is at NOAA’s facility in Silver Spring, Maryland. The public can occasionally view the machine during events such as the NOAA Open House. [9]

Mathematical basis

Tide Predicting Machine No. 2 is based on the first accurate mathematical approach for predicting tides, which was developed around 1867 by Sir William Thomson (who later became Lord Kelvin) and later refined by Sir George Darwin. This approach, called “harmonic analysis,” approximates tide heights by a summation of cosine terms, each of which has a different frequency. The formula for sea height is represented as

containing 10, 20 or even more trigonometric terms. is the height of mean sea level. For each term , is the amplitude of the term’s contribution to tide height above mean sea level, determines the frequency of the term, is the time, and is the relative phase of the term. This is the equation computed by most tide-predicting machines, including Old Brass Brains which handles 37 such terms. [6]

The frequencies are determined from astronomical considerations, which were determined by Thomson and Darwin and have been almost universally used. For instance one speed represents the speed of a theoretical moon with a uniform speed in a circular orbit in the equatorial plane. Other components with their own speeds correct for the differences between the orbit of that theoretical moon and the real Moon. [5] The coefficients and are determined by Fourier analysis of a time series of tide heights. This analysis can be performed with a record as short as two weeks but a 369-day sample is standard. [10] The longer sample minimizes the errors introduced by wind storms, freshets, and other non-regular influences. [6]

mechanism for generating sinusoidal motion component 099-tmpshaft.jpg
mechanism for generating sinusoidal motion component

To compute those terms the Coast and Geodetic Survey designers incorporated the same "slotted yoke crank" approach for mechanically computing cosines as Thomson used, shown in the schematic (right). A rotating drive-wheel ("crank") is fitted with an off-center peg. A shaft with a horizontally-slotted section is free to move vertically up and down. The wheel's off-center peg is located in the slot. As a result, when the peg moves around with the wheel, it makes the shaft move up and down within limits. As a result of this arrangement when the drive-wheel rotates uniformly, say clockwise, the shaft moves sinusoidally up and down. The vertical position of the center of the slot, at any time , can then be expressed as , where is the radial distance from the wheel's center to the peg, is the rate at which the wheel turns (in radians per unit of time) and is determined by gears, and is the starting phase angle of the peg, measured in radians from the 12 o'clock position to the angular position where the peg was at time zero. An operator adjusted the location of each pin based on the empirically computed parameters for a port’s tides. This arrangement makes a physical analog of just one term in the tide equation. Old Brass Brains computes 37 such terms.

The slotted yoke cranks at the top and bottom (with the triangular pieces) move vertically in a sinusoidal pattern. The locations of their pins determine their amplitudes and phases, representing factors in the tide equation. The pulleys across the center move with the attached cranks. The summation chain above and below the pulleys sums their influences. Slotted Yoke Cranks.jpg
The slotted yoke cranks at the top and bottom (with the triangular pieces) move vertically in a sinusoidal pattern. The locations of their pins determine their amplitudes and phases, representing factors in the tide equation. The pulleys across the center move with the attached cranks. The summation chain above and below the pulleys sums their influences.

The Coast and Geodetic Survey designers also adopted from the earlier British machines the approach of summing terms by passing a chain over and under pulleys attached to the vertically oscillating yokes. The amount of chain remaining after passing over and under pulleys indicated the sum of the terms. For example, a large value for a term would move its pulley further from a neutral position, deflecting the chain, and reducing the amount of excess chain remaining in system. [5]

One side of Old Brass Brains is used to compute the height of the tide. A similar arrangement of components on the other side, but with cranks 90 degrees out of phase, represents the derivative with respect to time of the tide height formula. When the derivative is zero the time of high or low tide has been reached. An electrical circuit detects this condition and stops the machine so the operator can record the date, time, and tide height. [6]

Related Research Articles

Mechanical advantage is a measure of the force amplification achieved by using a tool, mechanical device or machine system. The device trades off input forces against movement to obtain a desired amplification in the output force. The model for this is the law of the lever. Machine components designed to manage forces and movement in this way are called mechanisms. An ideal mechanism transmits power without adding to or subtracting from it. This means the ideal machine does not include a power source, is frictionless, and is constructed from rigid bodies that do not deflect or wear. The performance of a real system relative to this ideal is expressed in terms of efficiency factors that take into account departures from the ideal.

In mechanics and physics, simple harmonic motion is a special type of periodic motion an object experiences due to a restoring force whose magnitude is directly proportional to the distance of the object from an equilibrium position and acts towards the equilibrium position. It results in an oscillation that is described by a sinusoid which continues indefinitely.

<span class="mw-page-title-main">Angular velocity</span> Pseudovector representing an objects change in orientation with respect to time

In physics, angular velocity, also known as angular frequency vector, is a pseudovector representation of how the angular position or orientation of an object changes with time, i.e. how quickly an object rotates around an axis of rotation and how fast the axis itself changes direction.

In geometry, a solid angle is a measure of the amount of the field of view from some particular point that a given object covers. That is, it is a measure of how large the object appears to an observer looking from that point. The point from which the object is viewed is called the apex of the solid angle, and the object is said to subtend its solid angle at that point.

<span class="mw-page-title-main">Earth radius</span> Distance from the Earth surface to a point near its center

Earth radius is the distance from the center of Earth to a point on or near its surface. Approximating the figure of Earth by an Earth spheroid, the radius ranges from a maximum of nearly 6,378 km (3,963 mi) to a minimum of nearly 6,357 km (3,950 mi).

<span class="mw-page-title-main">Tautochrone curve</span> Concept in geometry

A tautochrone curve or isochrone curve is the curve for which the time taken by an object sliding without friction in uniform gravity to its lowest point is independent of its starting point on the curve. The curve is a cycloid, and the time is equal to π times the square root of the radius over the acceleration of gravity. The tautochrone curve is related to the brachistochrone curve, which is also a cycloid.

<span class="mw-page-title-main">Negative frequency</span>

In mathematics, signed frequency expands upon the concept of frequency, from just an absolute value representing how often some repeating event occurs, to also have a positive or negative sign representing one of two opposing orientations for occurrences of those events. The following examples help illustrate the concept:

In mathematics, a change of variables is a basic technique used to simplify problems in which the original variables are replaced with functions of other variables. The intent is that when expressed in new variables, the problem may become simpler, or equivalent to a better understood problem.

The Eötvös effect is the change in measured Earth's gravity caused by the change in centrifugal acceleration resulting from eastbound or westbound velocity. When moving eastbound, the object's angular velocity is increased, and thus the centrifugal force also increases, causing a perceived reduction in gravitational force.

<span class="mw-page-title-main">Sunrise equation</span> Equation to derive time of sunset and sunrise

The sunrise equation or sunset equation can be used to derive the time of sunrise or sunset for any solar declination and latitude in terms of local solar time when sunrise and sunset actually occur.

<span class="mw-page-title-main">Orbit determination</span>

Orbit determination is the estimation of orbits of objects such as moons, planets, and spacecraft. One major application is to allow tracking newly observed asteroids and verify that they have not been previously discovered. The basic methods were discovered in the 17th century and have been continuously refined.

Atmospheric tides are global-scale periodic oscillations of the atmosphere. In many ways they are analogous to ocean tides. Atmospheric tides can be excited by:

<span class="mw-page-title-main">Theory of tides</span> Scientific interpretation of tidal forces

The theory of tides is the application of continuum mechanics to interpret and predict the tidal deformations of planetary and satellite bodies and their atmospheres and oceans under the gravitational loading of another astronomical body or bodies.

<span class="mw-page-title-main">Least-squares spectral analysis</span> Periodicity computation method

Least-squares spectral analysis (LSSA) is a method of estimating a frequency spectrum based on a least-squares fit of sinusoids to data samples, similar to Fourier analysis. Fourier analysis, the most used spectral method in science, generally boosts long-periodic noise in the long and gapped records; LSSA mitigates such problems. Unlike in Fourier analysis, data need not be equally spaced to use LSSA.

<span class="mw-page-title-main">Tide-predicting machine</span> Mechanical analog computer

A tide-predicting machine was a special-purpose mechanical analog computer of the late 19th and early 20th centuries, constructed and set up to predict the ebb and flow of sea tides and the irregular variations in their heights – which change in mixtures of rhythms, that never repeat themselves exactly. Its purpose was to shorten the laborious and error-prone computations of tide-prediction. Such machines usually provided predictions valid from hour to hour and day to day for a year or more ahead.

<span class="mw-page-title-main">Geodetic coordinates</span> Geographic coordinate system

Geodetic coordinates are a type of curvilinear orthogonal coordinate system used in geodesy based on a reference ellipsoid. They include geodetic latitude (north/south) ϕ, longitude (east/west) λ, and ellipsoidal heighth. The triad is also known as Earth ellipsoidal coordinates.

The Bowring series of the transverse mercator published in 1989 by Bernard Russel Bowring gave formulas for the Transverse Mercator that are simpler to program but retain millimeter accuracy.

In physics, and especially scattering theory, the momentum-transfer cross section is an effective scattering cross section useful for describing the average momentum transferred from a particle when it collides with a target. Essentially, it contains all the information about a scattering process necessary for calculating average momentum transfers but ignores other details about the scattering angle.

<span class="mw-page-title-main">Geodesics on an ellipsoid</span> Shortest paths on a bounded deformed sphere-like quadric surface

The study of geodesics on an ellipsoid arose in connection with geodesy specifically with the solution of triangulation networks. The figure of the Earth is well approximated by an oblate ellipsoid, a slightly flattened sphere. A geodesic is the shortest path between two points on a curved surface, analogous to a straight line on a plane surface. The solution of a triangulation network on an ellipsoid is therefore a set of exercises in spheroidal trigonometry.

Nonlinear tides are generated by hydrodynamic distortions of tides. A tidal wave is said to be nonlinear when its shape deviates from a pure sinusoidal wave. In mathematical terms, the wave owes its nonlinearity due to the nonlinear advection and frictional terms in the governing equations. These become more important in shallow-water regions such as in estuaries. Nonlinear tides are studied in the fields of coastal morphodynamics, coastal engineering and physical oceanography. The nonlinearity of tides has important implications for the transport of sediment.

References

  1. "The fall of 'Old Brass Brains'". Product Engineering. 41 (1–6): 98. 1970.
  2. 1 2 3 4 5 "Old Brass Brains" (PDF). National Oceanic and Atmospheric Administration. February 1989. Retrieved May 1, 2016.
  3. 1 2 3 4 5 6 Hicks, Steacy (1967). "The Tide Prediction Centenary of the United States Coast and Geodetic Survey". International Hydrographic Review. XLIV: 121–131. Retrieved May 1, 2016.
  4. 1 2 3 4 5 Claudy, C. H. (March 7, 1914). "A Great Brass Brain: A Unique Engine, on the Accuracy of Which Depend Millions of Dollars and Thousands of Lives". Scientific American. 110: 197–198. doi:10.1038/scientificamerican03071914-197 . Retrieved May 1, 2016.
  5. 1 2 3 4 5 6 7 Description of the U.S. Coast and geodetic survey tide-predicting machine, Issue 2. U.S. Coast and Geodetic Survey. 1915.
  6. 1 2 3 4 5 6 7 8 9 10 11 12 Fischer, E. G. (May 1912). "The Coast and Geodetic Survey Tide Predicting Machine No. 2". Popular Astronomy. 20 (5): 269–285. Bibcode:1912PA.....20..269F . Retrieved May 1, 2016.
  7. "Tide Predicting Machines - NOAA Tides & Currents". www.co-ops.nos.noaa.gov. Retrieved 2016-05-01.
  8. Parker, Bruce (2012). The Power of the Sea: Tsunamis, Storm Surges, Rogue Waves, and Our Quest to Predict Disasters. Macmillan. p. 39. ISBN   978-0-230-12074-7.
  9. "NOAA Open House" . Retrieved May 1, 2016.
  10. Phillips, Tony. "Fourier Analysis of Ocean Tides II". Feature Column: Monthly Essays on Mathematical Topics. American Mathematical Society . Retrieved May 8, 2016.