They Were Gradually Working Her Up

 

We know from the testimony of J. Bruce Ismay that the Titanic started out running at 70 revolutions per minute after leaving Queenstown. We also know that 70 rpm corresponds to about 20.7 knots through the water.[1] The distance between Daunt’s Rock Lightvessel, the starting point of the transatlantic part of the voyage just outside of  Queenstown, and Fastnet light, a lighthouse situated on a small isolated rock off the southwest coast of Ireland, is a run  of about 55 nautical miles.[2] At 20.7 knots, it would take 2 hours and 40 minutes to make that distance. Since departure at Daunt’s Rock was noted at 2:20 p.m., an arrival time at Fastnet of 5:00 p.m. would therefore be expected. It is interesting to note that Sir James Bisset, Second Officer on the rescue ship Carpathia in 1912, wrote in his 1959 book Tramps and Ladies that the Titanic “had Fastnet rock abeam at 5 p.m.” which is something he may have heard in conversations with Titanic’s surviving officers on the way back to New York.[3]

 

According to Ismay’s recollection, the revolutions carried on Friday, the second day out, were increased to about 72 rpm. At 72 rpm the ship would be making 21.2 knots through the water. If that increase in revolutions began on Thursday evening at the beginning of the First Watch (the 8 p.m. to 12 a.m. watch), then the average speed through the water between 2:20 p.m. GMT Thursday, April 11, and local apparent noon Friday, April 12, averages out to 21.1 knots,[4] just slightly better than the derived 20.98 knots average speed over ground for the 484 mile run from Daunt’s Rock to her April 12 noon position.

 

Friday evening, April 12, Captain Smith sent a position report from the Titanic to the La Touraine for 7 p.m. GMT.  It read:

 

Titanic 'To Captain La Touraine,’ Thanks for your message and information my position. 7 p.m. G.M.T. Lat. 49.45; long. 23.38. W. Greenwich; had fine weather; compliments. - Smith

 

The difference between the time given in the La Touraine message (7 p.m. GMT) and the time for local apparent noon (1:24 p.m. GMT) was 5 hours 36 minutes. The distance from our noon position for April 12 (50° 06’ N, 20° 43’ W) to the position in the La Touraine message (49° 45’ N, 23° 38’ W) is 114.6 miles. The speed over ground calculates out to 20.5 knots for that period of time. But if Ismay was correct, and the Titanic was carrying 72 revolutions per minute, then the ship should have been making about 21.2 knots through the water all that afternoon. The difference between 21.2 knots through the water and 20.5 knots over ground suggests that the ship was under the influence of a relatively strong easterly component of the North Atlantic drift at that time, something that is quite reasonable and not at all unexpected during a westbound voyage.

 

We also have from the testimony of Fireman Frederick Barrett that another double-ended boiler was lit up some time on Friday. What time that boiler was connected on line is not known, but we know from Barrett that it takes close to 12 hours to bring a boiler on line after it is lit. Adding just one more boiler to the 20 double-ended boilers they already had connected up on Friday increases the overall steam supply by 5%. Thus the power delivered by the boilers for the same firing rate would go up by about 5% which would result in an increase in revolutions from 72 rpm to about 73 rpm keeping the same firing rate.[5] This means that the speed of the ship would have gone up from 21.2 to 21.5 knots. If we assume, as they would later do on Sunday, that this extra boiler was lit about 8 a.m. Friday morning and then connected up around 8 p.m. that Friday night, then we get a weighted average speed through the water for the second day out from Queenstown of 21.4 knots. With an overall average speed over ground of 20.91 knots from noon Friday to noon Saturday, we find that the Titanic was still under the influence of an easterly current drift of about a ˝ knot on its second day out. Clearly, the North Atlantic Drift was having a noticeable affect on the progress of the ship this particular day. It is little wonder that the purser told second class passenger Lawrence Beesley that the 519 mile run for the second day was somewhat disappointing.[6]

 

For the third day’s run of 546 miles, from noon Saturday to noon Sunday, we have information from both Ismay and Barrett that the revolutions were increased to 75 rpm. This was the minimum revolutions that was called for on Saturday, and Barrett said that he heard of no complaints afterward. It is therefore reasonable to assume that they were making 75 revolutions or better most of the time. We really don’t know what time this increase in revolutions took place, but what we do know is that from noon Saturday to noon Sunday the ship averaged about 22.06 knots over the ground. Carrying just 75 revolutions, the ship would have been making about 22.0 knots through the water. But we also know from Fireman Hendrickson that at 4 p.m. Sunday afternoon the ship was making 76 revolutions, and Fireman Thompson said that they had actually posted 77 revolutions down in the stokehold at 3 p.m., just an hour earlier. And all of this was before two or three more double-ended boilers were connected up that night at 7 p.m.  At 76 rpm the ship  would be making about 22.2 knots through the water, and at 77 rpm she would be making about 22.5 knots through the water. So an average of 22.06 knots over ground for the third day out, from noon Saturday to noon Sunday, certainly looks quite reasonable.

 

Finally, an increase in revolutions of about 2 rpm had taken place on Sunday night after additional double-ended boilers that were first lit up Sunday morning at 8 a.m. were put on line at 7 p.m. that evening.[7] Taking an average between 75 and 76 rpm from 12 noon until 7 p.m., and then allowing an increase to an average between 77 and 78 rpm from 7 p.m. until the collision at 11:40 p.m.,[8] we get a weighted average of 22.3 knots through the water from noon to the time of the collision. This result happens to match very well with the taffrail log reading of 260 nautical miles through the water observed by QM George Rowe at the time the accident happened, the distance run in 11 hours and 40 minutes since noon.  The distance over ground from noon the collision point was 258 nautical mile which works out to a speed made good of 22.11 knots.

 



[1] See http://www.encyclopedia-titanica.org/item/5661/.

 

[2] See http://www.encyclopedia-titanica.org/keeping_track.html.

 

[3] Sir James Bisset (in collaboration with P. R. Stephensen), Tramps and Ladies, first published in the United kingdom by Angus & Robertson, 1959.

 

[4] Assuming they increased the revolutions from 70 to 72 at 8 p.m. on Thursday, then the ship’s average speed through the water for the first day out from Queenstown becomes 20.7 knots times 5 hours 40 minutes, plus 21.2 knots times 17 hours 24 minutes, all divided by 23 hours 4 minutes (the total elapsed time from departure at Daunt’s Rock on April 11 to LAN on April 12). This results in an average speed through the water of 21.1 knots.

 

[5] The required power goes up approximately as the cube of the speed. Thus the speed goes as the cube-root of the power.

 

[6] Lawrence Beesley, The Loss of the S.S. Titanic – Its Story and Its Lessons, Houghton Mifflin Co., 1912, Chapter II.

 

[7] The connect time came from Fireman Alfred Shiers. The additional boilers being lit came from Firemen Frederick Barrett and John Thompson. Several passengers (Lawrence Beesley, Mahala Douglas, George Rheims, and Henry Stengel)  noted the increase in revolutions of the engines late that night. There was other supporting evidence of this as well including the increase in pressure shown on the boiler gauges.

 

[8] Adding additional boilers on line does not necessarily mean an instantaneous increase in boiler pressure or speed. These boilers would be connected up at the same pressure as the other boilers that were already on line. Because of the increased number of boilers connected up, the flow rate of steam from any given boiler would drop allowing for the pressure to build up to a new steady-state value assuming the furnace firing rates remained the same. On these Olympic class ships the furnaces could be fired every 8, 9, 10, 12, 15, 20, 25, or 30 minutes as set by the engineers. For the same furnace firing rate, the boiler pressure would have to increase until a new steady-state is achieved, at which point the engines would be running faster and boiler pressure would level off at the new increased value.

 

<< BACK                                                   HOME