000 04821cam a22002414a 4500
008 1970
020 _aB0007EU51S
040 _aGamadero
_bspa
_cGamadero
041 _aeng
050 0 0 _aQC32
_bS2
_c1961
100 _aDaniel schaum
_93759
245 0 0 _aTheory and Problems of College Physics
250 _a6ta. edición
260 3 _aUnited States Of America
_b Schaum's Outline Series
_c1970
300 _a270p
_bIlustración
_c22 x 28 cm
505 _aCHAPTER 1. INTRODUCTION TO VECTORS .. 2. EQUILIBRIUM OF A BODY: PARALLEL COPLANAR FORCES EQUILIBRIUM OF A BODY: NON-PARALLEL COPLANAR FORCES UNIFORMLY ACCELERATED MOTION FORCE ........ 6. WORK, ENERGY, POWER 7. SIMPLE MACHINES 8. IMPULSE AND MOMENTUM 9. ANGULAR VELOCITY AND ACCELERATION 10. CENTRIPETAL AND CENTRIFUGAL FORCE 11. ROTATION OF A BODY 12. SIMPLE HARMONIC MOTION 13. ELASTICITY 14. FLUIDS AT REST 15. FLUIDS IN MOTION 16. SURFACE TENSION 17. 18. 19. 20. 21. HEAT EXPANSION OF SOLIDS AND LIQUIDS .. EXPANSION OF GASES CALORIMETRY, FUSION, VAPORIZATION TRANSFER OF HEAT THERMODYNAMICS ELECTRICITY AND MAGNETISM 22. ELECTROSTATICS 23. 24. OHM's LAw 25. ELECTRICAL ENERGY, HEAT, POWER RESISTANCE AND CIRCUITS 26. ELECTROLYSIS 27. 28. MAGNETIC FIELDS OF CURRENTS 29. MAGNETS AND MAGNETIC CIRCUITS 30. GALVANOMETERS, AMMETERS, VOLTMETERS 31. ELECTROMAGNETIC INDUCTION . 32. SELF-INDUCTANCE AND MUTUAL INDUCTANCE 33. ELECTRIC GENERATORS AND MOTORS . ALTERNATING CURRENTS 35. 36. 37. ILLUMINATION AND PHOTOMETRY REFLECTION OF LIGHT .. REFRACTION OF LIGHT THIN LENSES 39. OPTICAL INSTRUMENTS 40. DISPERSION OF LICHT 41. INTERFERENCE AND DIFFRACTION OF LIGHT ATOMIC AND NUCLEAR PHYSICS 42. QUANTUM PHYSICS, RELATIVITY, WAVE MeCHANICS 43. NUcLEAR PHYSICS ... APPENDIX A. SIGNIFICANT FICURES B. C. TRIGONOMETRY NEEDED FOR COLLECE PHYSICS D. EXPONENTS LOGARITHMS E. UNITS AND CONVERSION FACTORS :. F. G. IMPORTANT PHYSICAL CONSTANTS, GREEK ALPHABET CONVERSION OF ELECTRICAL UNITS •*. H. I. FOUR-PLACE LOGARITHMS AND ANTILOGARITINS NATURAL TRIGONOMETRIC FUNCTIONS
520 _aA SCALAR QUANTITY has only magnitude, e.g. time, volume of a body, mass of a body, density of a body, amount of work, amount of money. Scalars are added by ordinary algebraic methods, e.g. 2 sec + 5 sec = 7 sec. A VECTOR QUANTITY has both magnitude and direction. For example: 1) Displacement - an airplane flies a distance of 160 mi in a southerly direction. 2) Velocity - a ship sails due east at 20 mi/hr. 3) Force - a force of 10lb acts on a body in a vertically upward direction. A vector quantity is represented by an arrow drawn to scale. The length of the arrow represents the magnitude of the displacement, velocity, force, etc. The direction of the arrow represents the direction of the displacement, etc. Vectors are added by geometric methods. THE RESULTANT of a number of force vectors is that single vector which would have the same ef- fect as all the original vectors together. THE EQUILIBRANT of a number of vectors is that vector which would balance all the original vectors taken together. It is equal in magnitude but opposite in direction to the resultant. PARALLELOGRAM METHOD OF VECTOR ADDITION. The resultant of two vectors acting at any angle may be represented by the diagonal of a parallelogram drawn with the two vectors as adjacent sides, and directed away from the origin of the two vectors. VECTOR POLYGON METHOD OF VECTOR ADDITION. This method of finding the resultant consists-in beginning at any convenient point and drawing (to scale) each vector in turn, taking them in any order of succession. The tail end of each vector is attached to the arrow end of the preced. The line drawn to complete the triangle or polygon is equal in magnitude to the result- ant or equilibrant. The resultant is represented by the straight line directed from the starting point to the ar- row end of the last vector added. The equilibrant is represented by the same line as the resultant but is oppositely directed, i.e. toward the starting point. SUBTRACTION OF VECTORS. To subtract vector B from vector A, reverse the direction of vector B and add it vectorially to vector A, i.e. A -B = A +(-B). A COMPONENT OF A VECTOR is its effective value in any given direction. For example, the hori- zontal component of a vector is its effective value in a horizontal direction. A vector may be considered as the resultant of two or more component vectors, the vector sum of the components being the original vector. It is customary and
526 _aIngeniería Industrial
650 0 _aALGEBRA LINEAL
_91142
700 _aCarel W.
_93760
942 _2lcc
_cLIB
_e6ta. edición
_n0
945 _a1260
_bNorma Gabriela Corona Arreguin
_c1260
_dNorma Gabriela Corona Arreguin
999 _c8816
_d8816