Books with author Major William Henry Lowe Watson

"The author of this classic account of early tank warfare, Major W. H. L. Watson, was already an experienced veteran whose early Great War exploits in the Cycle Corps he had recorded in his ‘Adventures of a Despatch-Rider'. Early in 1917, as this book records, damp, disillusioned and feeling that the tank might inject a touch of romance into the war, he volunteered and was accepted into the Heavy Branch of the Machine Gun Corps - which later became the Tank Corps. After a brief period of training Watson's X! company was flung into action in April 1917 in the ‘blood-tub' battle of Bullecourt. Thereafter, he also fought at Third Ypres (Passchendaele). But the core of the book is the author's description of the battle of Cambrai in November 1917, when tanks were used en masse for the first time. He describes the initially successful breakthrough, and the subsequent German counterattack which won back almost a much ground as had been lost in the initial tank thrust. A vivid writer, Watson well records he extreme discomfort - heat, fumes, noise, splinters and general disorientation - suffered by the early tank crews. The remainder of the book describes the part played by the tanks in the final Allied counter offensive in 1918 from the battle of Amiens to the breaching of the Hindenburg Line. This is a hitherto rare but extremely valuable and well written account of the early days of the tank which must not be missed by any student of armoured warfare." -www.naval-military-press.com

“Steel, mud, blood and courage on the Western FrontThis is a fine book because it is a superb first hand eye-witness account of British Tanks in action throughout the First World War. Without much preamble Watson launches the reader, in company with the author’s brother officers, men and machines into the heart of the field of conflict on the 11th Corps forward line on the Western Front in the Autumn and Winter of 1916. From that point to the end of the book and the war itself the narrative takes us inexorably into the dark heart of war the tankers knew. Battles and battlefield experiences in their various phases (sometimes the book includes descriptions as expansive as three chapters each) are covered in engrossing detail. We join the author and the men we come to know as personalities, at First and Second Bullecourt, in much detail at Third Ypres and Cambrai before Amiens, the breaking of the Hindenburg Line and Second Le Cateau. This is a primary source work within a finite resource and as such is beyond value. Nevertheless, it is also a highly absorbing read to be relished by students of the period-professional and amateur alike. Available in soft cover and hard back with dust jacket for collectors.”-Leonaur Print VersionAuthor — Major William Henry Lowe Watson, D.S.O., D.C.M. (1891-1931)Text taken, whole and complete, from the edition published in Edinburgh; William Blackwood, 1920.Original Page Count – vii and 296 pagesMaps — 8 sketch maps.

This work has been selected by scholars as being culturally important, and is part of the knowledge base of civilization as we know it. This work was reproduced from the original artifact, and remains as true to the original work as possible. Therefore, you will see the original copyright references, library stamps (as most of these works have been housed in our most important libraries around the world), and other notations in the work.This work is in the public domain in the United States of America, and possibly other nations. Within the United States, you may freely copy and distribute this work, as no entity (individual or corporate) has a copyright on the body of the work.As a reproduction of a historical artifact, this work may contain missing or blurred pages, poor pictures, errant marks, etc. Scholars believe, and we concur, that this work is important enough to be preserved, reproduced, and made generally available to the public. We appreciate your support of the preservation process, and thank you for being an important part of keeping this knowledge alive and relevant.

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This is a pre-1923 historical reproduction that was curated for quality. Quality assurance was conducted on each of these books in an attempt to remove books with imperfections introduced by the digitization process. Though we have made best efforts - the books may have occasional errors that do not impede the reading experience. We believe this work is culturally important and have elected to bring the book back into print as part of our continuing commitment to the preservation of printed works worldwide.

This is a pre-1923 historical reproduction that was curated for quality. Quality assurance was conducted on each of these books in an attempt to remove books with imperfections introduced by the digitization process. Though we have made best efforts - the books may have occasional errors that do not impede the reading experience. We believe this work is culturally important and have elected to bring the book back into print as part of our continuing commitment to the preservation of printed works worldwide. This text refers to the Bibliobazaar edition.

This work has been selected by scholars as being culturally important, and is part of the knowledge base of civilization as we know it. This work was reproduced from the original artifact, and remains as true to the original work as possible. Therefore, you will see the original copyright references, library stamps (as most of these works have been housed in our most important libraries around the world), and other notations in the work.This work is in the public domain in the United States of America, and possibly other nations. Within the United States, you may freely copy and distribute this work, as no entity (individual or corporate) has a copyright on the body of the work.As a reproduction of a historical artifact, this work may contain missing or blurred pages, poor pictures, errant marks, etc. Scholars believe, and we concur, that this work is important enough to be preserved, reproduced, and made generally available to the public. We appreciate your support of the preservation process, and thank you for being an important part of keeping this knowledge alive and relevant.

This is a pre-1923 historical reproduction that was curated for quality. Quality assurance was conducted on each of these books in an attempt to remove books with imperfections introduced by the digitization process. Though we have made best efforts - the books may have occasional errors that do not impede the reading experience. We believe this work is culturally important and have elected to bring the book back into print as part of our continuing commitment to the preservation of printed works worldwide.

This historic book may have numerous typos and missing text. Purchasers can download a free scanned copy of the original book (without typos) from the publisher. Not indexed. Not illustrated. 1889 Excerpt: ...we know that df dg dh dx dy dz and therefore--p =--V2. Whence it follows that y/r is the potential of the free electricity in the field. 403. Again, if there be material motion in the field we have proved, Art. 389, that „.dF.dG.dH... _ „ dF d+-F = xdx-+ + zdz--cy+bz+G-H+-dT + d' with similar expressions for Q and R. If the substance be of invariable form we know that o, o2, o3 have the same values throughout, and also that This proposition was first demonstrated by Professor Poynting, D.Sc, F.R.S., in a paper published in the Transactions of the Royal Society of London for 1884. It being proved, as above, that the time variation of the energy within a closed surface is expressible as a surface integral over that surface, Professor Poynting assumes that the flow of energy through each surface element is the argument of that surface integral. This theory, with many interesting consequences, has met with general acceptance. therefore _ d,.-.-,--... dG db whence, attending to the equations dz ay r-,in A dc da V2G =--4-itv =-5--ax dz 9 Tt-da db dy dx, dP dQ dR',, as before, and p is in this case also the potential of electrical distribution. If we adopt the shorter and more usual formulae p = c--bz----dt dx &c, where jr'=Fx+Gy+Hz. Since P, Q, i2 in the two expressions differ only by the.. djr db dlr......«,.. quantities----t1-)-51-respectively, it is indifferent which forms are employed in the case of closed currents, only it is important to remember that in the one case the yjr is the potential of free electricity, and in the other case that it differs from that potential by the quantity j/ or Fx + Gy+Hz. Note.--The field equations arriTed at in this Chapter are those principally in use, and which will be employed in subsequent pages. Many...

This is a pre-1923 historical reproduction that was curated for quality. Quality assurance was conducted on each of these books in an attempt to remove books with imperfections introduced by the digitization process. Though we have made best efforts - the books may have occasional errors that do not impede the reading experience. We believe this work is culturally important and have elected to bring the book back into print as part of our continuing commitment to the preservation of printed works worldwide.