User contributions for Foretony
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1 September 2014
- 13:0713:07, 1 September 2014 diff hist +15 Forest UCM PnCP ProjMotion →Friction depends linearly on velocity
- 13:0213:02, 1 September 2014 diff hist +1 Forest UCM PnCP ProjMotion →Range equation
- 13:0113:01, 1 September 2014 diff hist +193 Forest UCM PnCP ProjMotion →Range equation
- 12:5912:59, 1 September 2014 diff hist +175 Forest UCM PnCP ProjMotion →Range equation
- 12:5812:58, 1 September 2014 diff hist +214 Forest UCM PnCP ProjMotion →Range equation
- 12:5512:55, 1 September 2014 diff hist +152 Forest UCM PnCP ProjMotion →Range equation
- 12:5412:54, 1 September 2014 diff hist +54 Forest UCM PnCP ProjMotion →Range equation
- 12:5312:53, 1 September 2014 diff hist −1 Forest UCM PnCP ProjMotion →Range equation
- 12:5212:52, 1 September 2014 diff hist +50 Forest UCM PnCP ProjMotion →Range equation
- 12:5012:50, 1 September 2014 diff hist +1 Forest UCM PnCP ProjMotion →Range equation
- 12:4912:49, 1 September 2014 diff hist −5 Forest UCM PnCP ProjMotion →Range equation
- 12:4812:48, 1 September 2014 diff hist +37 Forest UCM PnCP ProjMotion →Range equation
- 12:4612:46, 1 September 2014 diff hist +27 Forest UCM PnCP ProjMotion →Friction depends linearly on velocity
- 12:4312:43, 1 September 2014 diff hist +20 Forest UCM PnCP LinAirRes →Example: falling object with linear air friction current
- 12:4112:41, 1 September 2014 diff hist +192 Forest UCM PnCP LinAirRes →Example: falling object with linear air friction
- 12:3512:35, 1 September 2014 diff hist +702 Forest UCM PnCP ProjMotion →Friction depends linearly on velocity
- 12:1712:17, 1 September 2014 diff hist 0 Forest UCM PnCP ProjMotion →Friction depends lienarly on velocity
- 12:1712:17, 1 September 2014 diff hist −6 Forest UCM PnCP LinAirRes →Example: falling object with linear air friction
- 12:1612:16, 1 September 2014 diff hist +166 Forest UCM PnCP ProjMotion →Friction depends lienarly on velocity
- 12:1512:15, 1 September 2014 diff hist +495 Forest UCM PnCP ProjMotion →Friction depends lienarly on velocity
- 12:1212:12, 1 September 2014 diff hist +161 Forest UCM PnCP ProjMotion →Friction depends lienarly on velocity
- 12:1012:10, 1 September 2014 diff hist +1 Forest UCM PnCP LinAirRes →Example: falling object with linear air friction
- 12:0912:09, 1 September 2014 diff hist +9 Forest UCM PnCP LinAirRes →Example: falling object with linear air friction
- 12:0912:09, 1 September 2014 diff hist +201 Forest UCM PnCP LinAirRes →Example: falling object with linear air friction
- 12:0212:02, 1 September 2014 diff hist +126 Forest UCM PnCP LinAirRes →Example: falling object with linear air friction
- 11:5911:59, 1 September 2014 diff hist +86 Forest UCM PnCP LinAirRes →Example: falling object with linear air friction
- 11:5611:56, 1 September 2014 diff hist +272 Forest UCM PnCP LinAirRes →Example: falling object with linear air friction
- 11:5311:53, 1 September 2014 diff hist +533 Forest UCM PnCP ProjMotion →Friction depends lienarly on velocity
- 11:4411:44, 1 September 2014 diff hist +102 N Forest UCM PnCP ProjMotion Created page with "=Projectile Motion= ==Friction depends lienarly on velocity== Forest_UCM_PnCP#Projecile_Motion"
- 11:4211:42, 1 September 2014 diff hist +32 Forest UCM PnCP →Projecile Motion
31 August 2014
- 14:1314:13, 31 August 2014 diff hist +20 Forest UCM PnCP →Another block on incline example
- 14:1014:10, 31 August 2014 diff hist −67 Forest UCM PnCP QubUniBfield →Determine the position as a function of time
- 14:0814:08, 31 August 2014 diff hist +3,438 N Forest UCM PnCP QubUniBfield Created page with " Consider a charged particle moving the x-y plane in the presence of a uniform magnetic field with field lines in the z-dierection. :<math>\vec{v} = v_x \hat i + v_y \hat j</ma…"
- 14:0714:07, 31 August 2014 diff hist −3,343 Forest UCM PnCP →Charged Particle in uniform B-Field
- 14:0614:06, 31 August 2014 diff hist +1,010 N Forest UCM PnCP QuadAirRes Created page with " Consider a ball falling under the influence of gravity and a frictional force that is proportion to its velocity squared :<math>\sum \vec{F}_{ext} = mg -bv^2 = m \frac{dv}{dt}<…"
- 14:0514:05, 31 August 2014 diff hist −970 Forest UCM PnCP →quadratic friction
- 14:0514:05, 31 August 2014 diff hist −33 Forest UCM PnCP →Example: falling object with quadratic air friction
- 14:0414:04, 31 August 2014 diff hist +32 Forest UCM PnCP →Example: falling object with quadratic air friction
- 14:0014:00, 31 August 2014 diff hist 0 Forest UCM PnCP LinAirRes →Example: falling object with linear air friction
- 13:5913:59, 31 August 2014 diff hist +62 Forest UCM PnCP LinAirRes →Example: falling object with linear air friction
- 13:5513:55, 31 August 2014 diff hist +5 Forest UCM PnCP LinAirRes No edit summary
- 13:5413:54, 31 August 2014 diff hist +821 Forest UCM PnCP LinAirRes No edit summary
- 13:5413:54, 31 August 2014 diff hist −798 Forest UCM PnCP →Example: falling object with linear air friction
- 13:5313:53, 31 August 2014 diff hist +44 Forest UCM PnCP LinAirRes No edit summary
- 13:5313:53, 31 August 2014 diff hist +1,030 N Forest UCM PnCP LinAirRes Created page with "; Horizontal motion If <math>n</math> is unity then the velocity is exponentially approaching zero. :<math>F(v) = -bv</math>: negative sign indicates a retarding force and <ma…"
- 13:5313:53, 31 August 2014 diff hist −1,001 Forest UCM PnCP →Linear Air Resistance
- 13:4913:49, 31 August 2014 diff hist +64 Forest UCM PnCP →Example: falling object with linear air friction
- 13:4813:48, 31 August 2014 diff hist +56 Forest UCM PnCP →Example: falling object with linear air friction
- 13:4713:47, 31 August 2014 diff hist +67 Forest UCM PnCP →Example: falling object with linear air friction
- 13:4613:46, 31 August 2014 diff hist −16 Forest UCM PnCP →Example: falling object with linear air friction