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 » topic 4 (4b)
- - - Unit 2 - - -
 » topic 5 (6&7a)
    here! ⇒
 » topic 6 (7b&8)
 » topic 7 (19)
 » topic 8 (20)
- - - Unit 3 - - -
 » topic 9 (10&11)
 » topic10 (12&9a)
 » topic11 (13&9b)

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College Physics I (PHY.201 - §201, 2018 Spring => CRN 4575)
Class Meets in :    Science 276 ... Mon & Wed & Fri   8:00 - 8:50 (am)
My office:   Science 159 (below ramp to 3rd Ave)     e-mail :   foltzc @ marshall.edu     phone :   (304) 696-2519
... Quiz 5 was done Mon.Mar.12 ... Wed.Mar.14 ... Fri.Mar.16 . . . here is my grading key as jpeg image
. . . here's the topic 5 overview power-point link (incomplete, but you asked ...)

Physics 1 Topic 5: Work done by Force (scalar Δx) Transfers Energy (scalar)

. . . Energy perspective is mostly about place rather than time
. . . Work is done to an object as the Force (its contact point) displaces
... (cf: Impulse done as Force endures time-wise)
. . . Force that is function of location can be treated as Potential Energy (function of location)
. . . a Potential Energy   abbreviated PE or U   stores Energy due to its condition (object in environment)

a Force does positive Work if the displacement projection is along the Force (similar direction)
. . . a Force does negative Work if the Force projection opposes the displacement ("opposite" direction)
. . . a Force does zero (0) Work if the displacement is perpendicular to the Force.

motional Energy : accumulated momentum, weighted by its velocity   has Kinetic Energy KE = ½ m v² . . . always positive !
local gravity :   Fgrav = m g   has PEgrav = m g h . . . gravity down, so height measured upward (from arbitrary "zero level").
pressure Force : Fpress = P A   has PEpress ≈ P V . . . roughly ... (should measure outside Volume)
spring Force :   Felast = − k s   has PEspr = ½ k s² . . . always positive !
general gravity: FS = mp GMS / r²   has PES = − mp GMS / r . . . always negative !
. . . there are only 3 conservative Forces this semester, so it is not a long list (local grav is an approx to "G" grav)

rope's Tension Force always does zero Work itself (Force is along rope length, but length does not change)
. . . but can transmit Work along the rope, if the rope attachment place moves (parallel rope) .

friction Force : Ffr = μ F_|_   always does negative Work (or 0), so has no formula for PE
. . . you must use Wfr = Ffr · Δx . . . same for viscous Force and drag Force.
. . . these forces transform KE into Thermal Energy ... yeah, raising their Temperatures ... wait till Topic 9.


Important statement #6 about how the Universe works : Energy is Conserved

. . . each Force from an external subject can do Work to the system ... if the Force pierces the system boundary (bag) ;
      positive (+) W transfers Energy from the subject (which applied that Force) into the object (system).
=> KEsystem,start + Σ Wby all F = KEsystem,end . . . this statement is called the "Work-Energy Theorem".

the 3rd Law for Forces says that , if the Force from me to the rock does positive Work , then the Force from the rock to me does the same negative Work.
. . . every Force has a 3rd Law pair-mate , so the Energy simply gets moved from item to item by those pairs.

. . . it is often useful ("easiest") to consider what Work the applied Forces might potentially do ;
      and ascribe that quantity to the system as Potential Energy ... with with this perspective
      a Force's (+) Work   transforms its Potential Energy into some other form of Energy, as it is actualized (made real rather than potential).
=> Σ Estart + Σ Wby F not in PE list = Σ Eend , for a system . . . that's the way we want to do it.


. . . Examples . . .


maintained by Curt Foltz - email comments to foltzc@marshall.edu
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