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Center-of-momentum frame

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2136: 2669: 1423: 38: 1861: 2402: 1156: 676: 2131:{\displaystyle {\begin{aligned}\mathbf {p} _{1}^{\prime }&=m_{1}\mathbf {u} _{1}^{\prime }\\&=m_{1}\left(\mathbf {u} _{1}-\mathbf {V} \right)={\frac {m_{1}m_{2}}{m_{1}+m_{2}}}\left(\mathbf {u} _{1}-\mathbf {u} _{2}\right)\\&=-m_{2}\mathbf {u} _{2}^{\prime }=-\mathbf {p} _{2}^{\prime }\\\end{aligned}}} 2367:
This is a substantially simpler calculation of the momenta of both particles; the reduced mass and relative velocity can be calculated from the initial velocities in the lab frame and the masses, and the momentum of one particle is simply the negative of the other. The calculation can be repeated for
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returns the lab frame equation above, demonstrating any frame (including the COM frame) may be used to calculate the momenta of the particles. It has been established that the velocity of the COM frame can be removed from the calculation using the above frame, so the momenta of the particles in the
2664:{\displaystyle {\begin{aligned}{\frac {{\rm {d}}\mathbf {R} }{{\rm {d}}t}}&={\frac {\rm {d}}{{\rm {d}}t}}\left({\frac {m_{1}\mathbf {r} _{1}+m_{2}\mathbf {r} _{2}}{m_{1}+m_{2}}}\right)\\&={\frac {m_{1}\mathbf {v} _{1}+m_{2}\mathbf {v} _{2}}{m_{1}+m_{2}}}\\&=\mathbf {V} \\\end{aligned}}} 1418:{\displaystyle {\begin{aligned}{\frac {{\rm {d}}\mathbf {R} }{{\rm {d}}t}}&={\frac {\rm {d}}{{\rm {d}}t}}\left({\frac {m_{1}\mathbf {r} _{1}+m_{2}\mathbf {r} _{2}}{m_{1}+m_{2}}}\right)\\&={\frac {m_{1}\mathbf {u} _{1}+m_{2}\mathbf {u} _{2}}{m_{1}+m_{2}}}\\&=\mathbf {V} \\\end{aligned}}} 1703: 3227: 1845: 3083: 1133: 367: 2922: 3318: 2765: 1519: 905: 2362: 3397: 1544: 3106: 1728: 2937: 2201: 356: 1037: 671:{\displaystyle \sum _{i}p'_{i}=\sum _{i}m_{i}v'_{i}=\sum _{i}m_{i}(v_{i}-V_{c})=\sum _{i}m_{i}v_{i}-\sum _{i}m_{i}{\frac {\sum _{j}m_{j}v_{j}}{\sum _{j}m_{j}}}=\sum _{i}m_{i}v_{i}-\sum _{j}m_{j}v_{j}=0.} 944:
system must travel at the speed of light in any frame, and always possesses a net momentum. Its energy is—for each reference frame—equal to the magnitude of momentum multiplied by the speed of light:
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respectively. The transformations are applied to take the velocity of the frame from the velocity of each particle from the lab frame (unprimed quantities) to the COM frame (primed quantities):
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of a system is not a location, but a collection of relative momenta/velocities: a reference frame. Thus "center of momentum" is a short for "center-of-momentum
1698:{\displaystyle \mathbf {V} ={\frac {\mathbf {p} _{1}+\mathbf {p} _{2}}{m_{1}+m_{2}}}={\frac {m_{1}\mathbf {u} _{1}+m_{2}\mathbf {u} _{2}}{m_{1}+m_{2}}}} 3222:{\displaystyle {\begin{aligned}\mathbf {P} &=\mathbf {p} _{1}+\mathbf {p} _{2}\\&=(m_{1}+m_{2})\mathbf {V} \\&=M\mathbf {V} \end{aligned}}} 1840:{\displaystyle \mathbf {p} _{1}^{\prime }+\mathbf {p} _{2}^{\prime }=m_{1}\mathbf {u} _{1}^{\prime }+m_{2}\mathbf {u} _{2}^{\prime }={\boldsymbol {0}}} 3078:{\displaystyle m_{1}\mathbf {u} _{1}=m_{1}\mathbf {v} _{1}=m_{1}\mathbf {V} ,\quad m_{2}\mathbf {u} _{2}=m_{2}\mathbf {v} _{2}=m_{2}\mathbf {V} } 2151: 706: 273: 198:
The center of momentum frame is defined as the inertial frame in which the sum of the linear momenta of all particles is equal to 0. Let
1128:{\displaystyle \mathbf {u} _{1}^{\prime }=\mathbf {u} _{1}-\mathbf {V} ,\quad \mathbf {u} _{2}^{\prime }=\mathbf {u} _{2}-\mathbf {V} } 102: 74: 55: 2917:{\displaystyle m_{1}\mathbf {u} _{1}+m_{2}\mathbf {u} _{2}=m_{1}\mathbf {v} _{1}+m_{2}\mathbf {v} _{2}=(m_{1}+m_{2})\mathbf {V} } 81: 3475: 3440: 2216: 88: 936:) do not have COM frames, because there is no frame in which they have zero net momentum. Due to the invariance of the 17: 3313:{\displaystyle \mathbf {p} _{1}^{\prime }=-\mathbf {p} _{2}^{\prime }=\mu \Delta \mathbf {v} =\mu \Delta \mathbf {u} } 3456: 121: 70: 741: 987:
An example of the usage of this frame is given below – in a two-body collision, not necessarily elastic (where
59: 3408: 177:(which is a single point) remains at the origin. In all center-of-momentum frames, the center of mass is at 3503: 3493: 1524:
The same results can be obtained by applying momentum conservation in the lab frame, where the momenta are
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COM frame can be expressed in terms of the quantities in the lab frame (i.e. the given initial values):
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is the velocity of the mass center. The total momentum in the center-of-momentum system then vanishes:
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is conserved). The COM frame can be used to find the momentum of the particles much easier than in a
1000: 996: 690: 2760:{\displaystyle m_{1}\mathbf {v} _{1}^{\prime }+m_{2}\mathbf {v} _{2}^{\prime }={\boldsymbol {0}}} 1708:
and in the COM frame, where it is asserted definitively that the total momenta of the particles,
1514:{\displaystyle m_{1}\mathbf {u} _{1}^{\prime }+m_{2}\mathbf {u} _{2}^{\prime }={\boldsymbol {0}}} 220: 207: 48: 900:{\displaystyle m_{0}{}^{2}=\left({\frac {E}{c^{2}}}\right)^{2}-\left({\frac {p}{c}}\right)^{2},} 2357:{\displaystyle \mathbf {p} _{1}^{\prime }=-\mathbf {p} _{2}^{\prime }=\mu \Delta \mathbf {u} } 950: 933: 3392:{\displaystyle \Delta \mathbf {v} =\mathbf {v} _{1}-\mathbf {v} _{2}=\Delta \mathbf {u} .} 995:: the frame where the measurement or calculation is done. The situation is analyzed using 8: 3513: 702: 182: 155: 3518: 3471: 3452: 3436: 3324: 2142: 941: 802:
of the system is given in any inertial frame by the relativistic invariant relation
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Unique inertial frame in which the total momentum of a physical system vanishes
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is the velocity of the COM, i.e. the time derivative of the COM location
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of the system vanishes. It is unique up to velocity, but not origin. The
185:, the COM frame is necessarily unique only when the system is isolated. 930: 181:, but it is not necessarily at the origin of the coordinate system. In 2196:{\displaystyle \Delta \mathbf {u} =\mathbf {u} _{1}-\mathbf {u} _{2}} 992: 922: 918:) vanishes and thus the total energy coincides with the rest energy. 728: 37: 3451:
Classical Mechanics, T.W.B. Kibble, European Physics Series, 1973,
351:{\displaystyle V_{c}={\frac {\sum _{i}m_{i}v_{i}}{\sum _{i}m_{i}}}} 926: 135: 3470:, D. Kleppner, R.J. Kolenkow, Cambridge University Press, 2010, 3435:
Dynamics and Relativity, J.R. Forshaw, A.G. Smith, Wiley, 2009,
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In the lab frame, the conservation of momentum fully reads:
709:. In the COM frame the total energy of the system is the 206:′ denote the center-of-momentum reference frame. Using a 2280:{\displaystyle \mu ={\frac {m_{1}m_{2}}{m_{1}+m_{2}}}} 169:
A special case of the center-of-momentum frame is the
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so the momenta of the particles compactly reduce to
3431: 3429: 62:. Unsourced material may be challenged and removed. 3391: 3312: 3221: 3077: 2916: 2759: 2663: 2356: 2279: 2195: 2130: 1839: 1697: 1513: 1417: 1127: 1017:, moving at initial velocities (before collision) 971: 899: 787: 670: 350: 256: 3092:multiplied by the velocity of the centre of mass 3485: 3426: 1150:(position of the center of mass of the system): 929:moving in a single direction, or, equivalently, 715:, and this quantity (when divided by the factor 788:{\displaystyle m_{0}={\frac {E_{0}}{c^{2}}}.} 3088:instead, it simply indicates the total mass 202:denote the laboratory reference system and 1850:Using the COM frame equation to solve for 921:Systems that have nonzero energy but zero 910:but for zero momentum the momentum term ( 122:Learn how and when to remove this message 1142:is the velocity of the COM frame. Since 3327:in the lab frame of particle 1 to 2 is 2145:in the lab frame of particle 1 to 2 is 14: 3486: 3232:Similar analysis to the above obtains 696: 60:adding citations to reliable sources 31: 2682:, this implies after the collision 2674:so at the origin of the COM frame, 2382:in place of the initial velocities 1428:so at the origin of the COM frame, 982: 24: 3378: 3337: 3302: 3288: 3277: 3254: 2744: 2714: 2457: 2450: 2429: 2415: 2346: 2335: 2312: 2155: 2119: 2096: 1915: 1881: 1824: 1794: 1764: 1744: 1498: 1468: 1211: 1204: 1183: 1169: 1097: 1053: 25: 3530: 173:: an inertial frame in which the 3382: 3365: 3350: 3341: 3306: 3292: 3267: 3244: 3211: 3193: 3143: 3128: 3115: 3071: 3047: 3022: 3002: 2978: 2953: 2910: 2867: 2842: 2817: 2792: 2753: 2734: 2704: 2653: 2604: 2579: 2512: 2487: 2421: 2350: 2325: 2302: 2183: 2168: 2159: 2109: 2086: 2046: 2031: 1961: 1947: 1905: 1871: 1833: 1814: 1784: 1754: 1734: 1657: 1632: 1576: 1561: 1549: 1507: 1488: 1458: 1407: 1358: 1333: 1266: 1241: 1175: 1121: 1107: 1087: 1077: 1063: 1043: 36: 3009: 1084: 47:needs additional citations for 3461: 3445: 3189: 3163: 2906: 2880: 479: 453: 13: 1: 3419: 3409:Laboratory frame of reference 188: 3468:An Introduction to Mechanics 7: 3402: 257:{\displaystyle v'=v-V_{c},} 210:, the particle velocity in 10: 3535: 193: 71:"Center-of-momentum frame" 691:inertial reference frames 1001:conservation of momentum 997:Galilean transformations 140:center-of-momentum frame 208:Galilean transformation 3393: 3314: 3223: 3096:is the total momentum 3079: 2918: 2761: 2665: 2358: 2281: 2197: 2132: 1841: 1699: 1515: 1419: 1129: 973: 901: 789: 672: 352: 258: 3394: 3315: 3224: 3080: 2919: 2762: 2666: 2359: 2282: 2198: 2133: 1842: 1700: 1516: 1420: 1130: 974: 972:{\displaystyle E=pc.} 934:electromagnetic waves 902: 790: 685:of the system is the 673: 353: 259: 3334: 3239: 3107: 2938: 2777: 2689: 2403: 2297: 2217: 2152: 1862: 1729: 1545: 1443: 1157: 1038: 951: 809: 742: 368: 274: 221: 171:center-of-mass frame 56:improve this article 3504:Frames of reference 3494:Classical mechanics 3281: 3258: 2927:This equation does 2748: 2718: 2339: 2316: 2123: 2100: 1919: 1885: 1828: 1798: 1768: 1748: 1502: 1472: 1101: 1057: 429: 393: 154:in which the total 148:zero-momentum frame 3499:Coordinate systems 3389: 3310: 3265: 3242: 3219: 3217: 3075: 2914: 2757: 2732: 2702: 2661: 2659: 2354: 2323: 2300: 2277: 2193: 2128: 2126: 2107: 2084: 1903: 1869: 1837: 1812: 1782: 1752: 1732: 1695: 1511: 1486: 1456: 1415: 1413: 1125: 1085: 1041: 969: 897: 785: 697:Special relativity 668: 641: 608: 582: 550: 527: 494: 442: 417: 406: 381: 380: 348: 334: 302: 254: 183:special relativity 160:center of momentum 18:Center of momentum 3509:Geometric centers 3476:978-0-521-19821-9 3441:978-0-470-01460-8 3325:relative velocity 2640: 2548: 2466: 2438: 2368:final velocities 2275: 2143:relative velocity 2022: 1693: 1612: 1394: 1302: 1220: 1192: 882: 854: 780: 735:) of the system: 707:Noether's theorem 689:as seen from all 632: 599: 594: 573: 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1349: 1345: 1340: 1335: 1328: 1324: 1317: 1314: 1312: 1310: 1306: 1298: 1294: 1290: 1285: 1281: 1273: 1268: 1261: 1257: 1253: 1248: 1243: 1236: 1232: 1225: 1218: 1213: 1206: 1200: 1197: 1195: 1190: 1185: 1177: 1171: 1163: 1162: 1136: 1135: 1123: 1119: 1114: 1109: 1104: 1099: 1094: 1089: 1083: 1079: 1075: 1070: 1065: 1060: 1055: 1050: 1045: 1028: 1021: 1014: 1007: 989:kinetic energy 984: 981: 980: 979: 968: 965: 962: 959: 956: 938:speed of light 908: 907: 896: 891: 886: 881: 878: 873: 868: 863: 858: 851: 847: 843: 838: 833: 828: 819: 815: 800:invariant mass 796: 795: 784: 777: 773: 767: 763: 757: 752: 748: 733:invariant mass 725:speed of light 698: 695: 687:minimal energy 679: 678: 667: 664: 659: 655: 649: 645: 639: 635: 631: 626: 622: 616: 612: 606: 602: 598: 590: 586: 580: 576: 568: 564: 558: 554: 548: 544: 535: 531: 525: 521: 517: 512: 508: 502: 498: 492: 488: 484: 481: 476: 472: 468: 463: 459: 455: 450: 446: 440: 436: 432: 428: 424: 420: 414: 410: 404: 400: 396: 392: 388: 384: 378: 374: 359: 358: 342: 338: 332: 328: 320: 316: 310: 306: 300: 296: 289: 284: 280: 265: 264: 253: 248: 244: 240: 237: 234: 230: 227: 195: 192: 190: 187: 175:center of mass 165: 152:inertial frame 130: 129: 112:September 2024 44: 42: 35: 28: 9: 6: 4: 3: 2: 3531: 3520: 3517: 3515: 3512: 3510: 3507: 3505: 3502: 3500: 3497: 3495: 3492: 3491: 3489: 3477: 3473: 3469: 3464: 3458: 3457:0-07-084018-0 3454: 3448: 3442: 3438: 3432: 3430: 3425: 3415: 3412: 3410: 3407: 3406: 3386: 3375: 3370: 3360: 3355: 3345: 3330: 3329: 3328: 3326: 3299: 3296: 3285: 3282: 3272: 3262: 3259: 3249: 3235: 3234: 3233: 3207: 3204: 3202: 3184: 3180: 3176: 3171: 3167: 3160: 3158: 3148: 3138: 3133: 3123: 3121: 3103: 3102: 3101: 3099: 3095: 3091: 3065: 3061: 3057: 3052: 3040: 3036: 3032: 3027: 3015: 3011: 3006: 2996: 2992: 2988: 2983: 2971: 2967: 2963: 2958: 2946: 2942: 2934: 2933: 2932: 2930: 2901: 2897: 2893: 2888: 2884: 2877: 2872: 2860: 2856: 2852: 2847: 2835: 2831: 2827: 2822: 2810: 2806: 2802: 2797: 2785: 2781: 2773: 2772: 2771: 2749: 2739: 2727: 2723: 2719: 2709: 2697: 2693: 2685: 2684: 2683: 2681: 2677: 2649: 2647: 2634: 2630: 2626: 2621: 2617: 2609: 2597: 2593: 2589: 2584: 2572: 2568: 2561: 2559: 2550: 2542: 2538: 2534: 2529: 2525: 2517: 2505: 2501: 2497: 2492: 2480: 2476: 2469: 2462: 2444: 2442: 2434: 2399: 2398: 2397: 2392: 2385: 2378: 2371: 2343: 2340: 2330: 2320: 2317: 2307: 2293: 2292: 2291: 2269: 2265: 2261: 2256: 2252: 2244: 2240: 2234: 2230: 2223: 2220: 2213: 2212: 2211: 2209: 2188: 2178: 2173: 2163: 2148: 2147: 2146: 2144: 2114: 2104: 2101: 2091: 2079: 2075: 2071: 2068: 2066: 2057: 2051: 2041: 2036: 2025: 2016: 2012: 2008: 2003: 1999: 1991: 1987: 1981: 1977: 1970: 1966: 1957: 1952: 1941: 1935: 1931: 1927: 1925: 1910: 1898: 1894: 1890: 1888: 1876: 1858: 1857: 1856: 1853: 1829: 1819: 1807: 1803: 1799: 1789: 1777: 1773: 1769: 1759: 1749: 1739: 1725: 1724: 1723: 1722:', vanishes: 1718: 1711: 1687: 1683: 1679: 1674: 1670: 1662: 1650: 1646: 1642: 1637: 1625: 1621: 1614: 1606: 1602: 1598: 1593: 1589: 1581: 1571: 1566: 1553: 1541: 1540: 1539: 1534: 1527: 1503: 1493: 1481: 1477: 1473: 1463: 1451: 1447: 1439: 1438: 1437: 1435: 1431: 1403: 1401: 1388: 1384: 1380: 1375: 1371: 1363: 1351: 1347: 1343: 1338: 1326: 1322: 1315: 1313: 1304: 1296: 1292: 1288: 1283: 1279: 1271: 1259: 1255: 1251: 1246: 1234: 1230: 1223: 1216: 1198: 1196: 1188: 1153: 1152: 1151: 1149: 1145: 1141: 1117: 1112: 1102: 1092: 1081: 1073: 1068: 1058: 1048: 1034: 1033: 1032: 1027: 1020: 1013: 1006: 1002: 998: 994: 990: 966: 963: 960: 957: 954: 947: 946: 945: 943: 939: 935: 932: 928: 924: 919: 917: 913: 894: 889: 884: 879: 876: 871: 866: 861: 856: 849: 845: 841: 836: 831: 826: 817: 813: 805: 804: 803: 801: 782: 775: 771: 765: 761: 755: 750: 746: 738: 737: 736: 734: 730: 726: 722: 718: 714: 713: 708: 704: 694: 692: 688: 684: 665: 662: 657: 653: 647: 643: 637: 633: 629: 624: 620: 614: 610: 604: 600: 596: 588: 584: 578: 574: 566: 562: 556: 552: 546: 542: 533: 529: 523: 519: 515: 510: 506: 500: 496: 490: 486: 482: 474: 470: 466: 461: 457: 448: 444: 438: 434: 430: 426: 422: 418: 412: 408: 402: 398: 394: 390: 386: 382: 376: 372: 364: 363: 362: 340: 336: 330: 326: 318: 314: 308: 304: 298: 294: 287: 282: 278: 270: 269: 268: 251: 246: 242: 238: 235: 232: 228: 225: 217: 216: 215: 213: 209: 205: 201: 186: 184: 180: 176: 172: 167: 163: 161: 157: 153: 149: 145: 141: 137: 126: 123: 115: 104: 101: 97: 94: 90: 87: 83: 80: 76: 73: –  72: 68: 67:Find sources: 61: 57: 51: 50: 45:This article 43: 39: 34: 33: 27: 19: 3467: 3463: 3447: 3322: 3231: 3097: 3093: 3089: 3087: 2928: 2926: 2769: 2679: 2675: 2673: 2390: 2383: 2376: 2369: 2366: 2289: 2208:reduced mass 2205: 2140: 1851: 1849: 1716: 1709: 1707: 1532: 1525: 1523: 1433: 1429: 1427: 1147: 1143: 1139: 1137: 1025: 1018: 1011: 1004: 988: 986: 920: 915: 911: 909: 797: 727:) gives the 720: 716: 710: 700: 686: 680: 360: 266: 211: 203: 199: 197: 170: 168: 159: 147: 143: 139: 133: 118: 109: 99: 92: 85: 78: 66: 54:Please help 49:verification 46: 26: 3414:Breit frame 2931:imply that 2141:notice the 712:rest energy 3514:Kinematics 3488:Categories 3420:References 703:relativity 189:Properties 82:newspapers 3379:Δ 3361:− 3338:Δ 3303:Δ 3300:μ 3289:Δ 3286:μ 3278:′ 3263:− 3255:′ 2745:′ 2715:′ 2347:Δ 2344:μ 2336:′ 2321:− 2313:′ 2221:μ 2179:− 2156:Δ 2120:′ 2105:− 2097:′ 2072:− 2042:− 1958:− 1916:′ 1882:′ 1825:′ 1795:′ 1765:′ 1745:′ 1499:′ 1469:′ 1118:− 1098:′ 1074:− 1054:′ 993:lab frame 925:(such as 923:rest mass 867:− 729:rest mass 634:∑ 630:− 601:∑ 575:∑ 543:∑ 520:∑ 516:− 487:∑ 467:− 435:∑ 399:∑ 373:∑ 327:∑ 295:∑ 239:− 150:, is the 144:COM frame 3519:Momentum 3403:See also 942:massless 719:, where 427:′ 391:′ 229:′ 156:momentum 927:photons 723:is the 267:where 194:General 136:physics 96:scholar 3474:  3455:  3439:  1715:' and 1138:where 683:energy 138:, the 98:  91:  84:  77:  69:  931:plane 214:′ is 164:frame 103:JSTOR 89:books 3472:ISBN 3453:ISBN 3437:ISBN 2389:and 2375:and 1531:and 1024:and 1010:and 999:and 940:, a 798:The 179:rest 75:news 2929:not 2210:is 701:In 166:". 134:In 58:by 3490:: 3428:^ 2678:= 1538:: 1432:= 1430:R' 693:. 666:0. 3387:. 3383:u 3376:= 3371:2 3366:v 3356:1 3351:v 3346:= 3342:v 3307:u 3297:= 3293:v 3283:= 3273:2 3268:p 3260:= 3250:1 3245:p 3212:V 3208:M 3205:= 3194:V 3190:) 3185:2 3181:m 3177:+ 3172:1 3168:m 3164:( 3161:= 3149:2 3144:p 3139:+ 3134:1 3129:p 3124:= 3116:P 3098:P 3094:V 3090:M 3072:V 3066:2 3062:m 3058:= 3053:2 3048:v 3041:2 3037:m 3033:= 3028:2 3023:u 3016:2 3012:m 3007:, 3003:V 2997:1 2993:m 2989:= 2984:1 2979:v 2972:1 2968:m 2964:= 2959:1 2954:u 2947:1 2943:m 2911:V 2907:) 2902:2 2898:m 2894:+ 2889:1 2885:m 2881:( 2878:= 2873:2 2868:v 2861:2 2857:m 2853:+ 2848:1 2843:v 2836:1 2832:m 2828:= 2823:2 2818:u 2811:2 2807:m 2803:+ 2798:1 2793:u 2786:1 2782:m 2754:0 2750:= 2740:2 2735:v 2728:2 2724:m 2720:+ 2710:1 2705:v 2698:1 2694:m 2680:0 2676:R 2654:V 2650:= 2635:2 2631:m 2627:+ 2622:1 2618:m 2610:2 2605:v 2598:2 2594:m 2590:+ 2585:1 2580:v 2573:1 2569:m 2562:= 2551:) 2543:2 2539:m 2535:+ 2530:1 2526:m 2518:2 2513:r 2506:2 2502:m 2498:+ 2493:1 2488:r 2481:1 2477:m 2470:( 2463:t 2458:d 2451:d 2445:= 2435:t 2430:d 2422:R 2416:d 2394:2 2391:u 2387:1 2384:u 2380:2 2377:v 2373:1 2370:v 2351:u 2341:= 2331:2 2326:p 2318:= 2308:1 2303:p 2270:2 2266:m 2262:+ 2257:1 2253:m 2245:2 2241:m 2235:1 2231:m 2224:= 2189:2 2184:u 2174:1 2169:u 2164:= 2160:u 2115:2 2110:p 2102:= 2092:2 2087:u 2080:2 2076:m 2069:= 2058:) 2052:2 2047:u 2037:1 2032:u 2026:( 2017:2 2013:m 2009:+ 2004:1 2000:m 1992:2 1988:m 1982:1 1978:m 1971:= 1967:) 1962:V 1953:1 1948:u 1942:( 1936:1 1932:m 1928:= 1911:1 1906:u 1899:1 1895:m 1891:= 1877:1 1872:p 1852:V 1834:0 1830:= 1820:2 1815:u 1808:2 1804:m 1800:+ 1790:1 1785:u 1778:1 1774:m 1770:= 1760:2 1755:p 1750:+ 1740:1 1735:p 1720:2 1717:p 1713:1 1710:p 1688:2 1684:m 1680:+ 1675:1 1671:m 1663:2 1658:u 1651:2 1647:m 1643:+ 1638:1 1633:u 1626:1 1622:m 1615:= 1607:2 1603:m 1599:+ 1594:1 1590:m 1582:2 1577:p 1572:+ 1567:1 1562:p 1554:= 1550:V 1536:2 1533:p 1529:1 1526:p 1508:0 1504:= 1494:2 1489:u 1482:2 1478:m 1474:+ 1464:1 1459:u 1452:1 1448:m 1434:0 1408:V 1404:= 1389:2 1385:m 1381:+ 1376:1 1372:m 1364:2 1359:u 1352:2 1348:m 1344:+ 1339:1 1334:u 1327:1 1323:m 1316:= 1305:) 1297:2 1293:m 1289:+ 1284:1 1280:m 1272:2 1267:r 1260:2 1256:m 1252:+ 1247:1 1242:r 1235:1 1231:m 1224:( 1217:t 1212:d 1205:d 1199:= 1189:t 1184:d 1176:R 1170:d 1148:R 1144:V 1140:V 1122:V 1113:2 1108:u 1103:= 1093:2 1088:u 1082:, 1078:V 1069:1 1064:u 1059:= 1049:1 1044:u 1029:2 1026:u 1022:1 1019:u 1015:2 1012:m 1008:1 1005:m 967:. 964:c 961:p 958:= 955:E 916:c 914:/ 912:p 895:, 890:2 885:) 880:c 877:p 872:( 862:2 857:) 850:2 846:c 842:E 837:( 832:= 827:2 818:0 814:m 783:. 776:2 772:c 766:0 762:E 756:= 751:0 747:m 731:( 721:c 717:c 663:= 658:j 654:v 648:j 644:m 638:j 625:i 621:v 615:i 611:m 605:i 597:= 589:j 585:m 579:j 567:j 563:v 557:j 553:m 547:j 534:i 530:m 524:i 511:i 507:v 501:i 497:m 491:i 483:= 480:) 475:c 471:V 462:i 458:v 454:( 449:i 445:m 439:i 431:= 423:i 419:v 413:i 409:m 403:i 395:= 387:i 383:p 377:i 341:i 337:m 331:i 319:i 315:v 309:i 305:m 299:i 288:= 283:c 279:V 252:, 247:c 243:V 236:v 233:= 226:v 212:S 204:S 200:S 142:( 125:) 119:( 114:) 110:( 100:· 93:· 86:· 79:· 52:. 20:)

Index

Center of momentum

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"Center-of-momentum frame"
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physics
inertial frame
momentum
center of mass
rest
special relativity
Galilean transformation
energy
inertial reference frames
relativity
Noether's theorem
rest energy
speed of light
rest mass
invariant mass
invariant mass
rest mass
photons

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