### тИ КщМЕ ОИ ВЯчСТЕР -сЩМТАНГ ЙЯИТИЙчР

дЕМ ЕМТОПъСАЛЕ ЙЯИТИЙщР СТИР СУМчХЕИР ТОПОХЕСъЕР.

### пЕЯИЕВЭЛЕМА

 Part 1 EXAMPLES 33 CHAPTER III 41 EXAMPLES 51 EXAMPLES 72 EXAMPLES 85 EXAMPLES 96 EXAMPLES 109
 EXAMPLES 203 EXAMPLES 211 EXAMPLES 224 EXAMPLES 234 EXAMPLES 215 245 EXAMPLES 255 MISCELLANEOUS EXAMPLES 266 ON THE THEORY OF COUPLES 273

 EXAMPLES 122 EXAMPLES 129 EXAMPLES 146 EXAMPLES 156 EXAMPLES 167 EXAMPLES 182 EXAMPLES 193
 ON THE GENERAL EQUATIONS OF EQUILIBRIUM 284 CHAPTER III 290 CHAPTER IV 302 EXAMPLES 315 EXAMPLES 328 MISCELLANEOUS EXAMPLES 312 342

### дГЛОЖИКч АПОСПэСЛАТА

сЕКъДА 16 - If any number of forces, acting at a point, can be represented in magnitude and direction by the sides of a polygon taken in order, they will be in equilibrium.
сЕКъДА 12 - If three forces, represented in magnitude and direction by the sides of a triangle, act on a point, they will keep it at rest.
сЕКъДА 4 - As the body on , which the forces act is in equilibrium, the supporting force / ' must be equal in magnitude and opposite in direction to the resultant of the loads L.
сЕКъДА 215 - ... altitude equal to the depth of the centre of gravity of the surface below the surface of the fluid.
сЕКъДА 29 - Prove that the algebraic sum of the moments of two concurrent forces about any point in their plane is equal to the moment of their resultant about the same point.