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Name : Rahmawati Yusri
NIM : RSA1C311001
APLICATION


               SUBDUCTION

THE MATERIAL   PENDULUM

                  SUBDUCTION TWO
                    DIMENSIONS

                ROCKET
IMPULSE AND MOMENTUM RELATIONSHIP

• Outgrow style that employs at object up to subduction
  happening can be depicted by relationship graph among f by
  t, with that assumption constant styled.
           F(t)




                  t1                 t2     t
                          t
• One particle gets mass m one that moving with speed v having linear
                                       .
  momentum p one that constitute multiple among that particle speed
  with its mass
                 v
          m                     p = mv.
  Legally Newton II. resultant inspires that is conected with one
  straight proportionate object with velocity

                                   F = ma.

                                   d ( mv )    dp
                            F
                                     dt         dt

                                 dp=Fdt

      If each diintegralkan therefore acquired:
p2            t2

                       p1     p2           dp              F .dt
                                      p1             t1



Linear Momentum continuity

       If resultant external style that employs at system equal to zero, therefore
       momentum vector total system makes a abode constant

                                     dp
                                                   0
                                     dt
 For particle system
                                p1     p2       ........      pn   p
SEVERALLY MOMENTUM PRINCIPLE PURPOSE


• Two logs A and b one gets mA's masses and mB, one that
  linked by one spiral spring and lie upon horizontal table
  without friction. Our spiral spring strungs strikingly both of log
  to sideways as on image.


                  y




                      A
                                         B
                                                x
              O
The one log gets positive momentum( A moves in aim + x) and bemomentum negative's
the other log (B moving deep tenor –x) from hokum our conservation of momentum
gets:

         Early momentum = final momentum

                             0     mBvB        m Av A
                        mBvB         m Av A
                  Or                 mB
                             vA           vB
                                     mA
SUBDUCTION


     sebelum                        selama          setelah




SUBDUCTION TYPES


1. Subduction Dashes Away perfect
    A subduction is said dash away perfect
     if jumlahan object kinetic energies that
    get good subduction before and after subduction with
    . (Energy continuity law kinetic)
m2                                   m1               m2
 m1
         v1                    v2


                                                   v’1
                                                                                      v’2

        sebelum                                                 sesudah


                  Gambar 6.4. Tumbukan dua benda




momentun early totaled:               paw = m1v1 + m2v2

                                          Ekaw = m1v12 + m2v22.
total early kinetic energy:

 second totaled momentum that object subduction afters is

                                            pak = m1v’1 + m2v’2

 totaled kinetic energy after subduction is
                                                                  Ekak = m1v’12 + m2v2’ 2.
paw = pak             m1v1 + m2v2 = m1v’1 + m2v’2                    m1(v1 − v’1) = m2(v’2 − v2),


  Ekaw = Ekak          m1v12 + m2v22 = m1v’12 + m2v2’ 2                  or

                       m1v12 − m1v’12 = m2v2’ 2 − m2v22                  or

                           m1 (v1 − v’1)( v1 + v’1) = m2(v’2 − v2) (v’2 +
                                                                      v2)
Of two box deep equations tingle to be gotten

                                                        v ' 2 v '1
        v1 + v’1 = v’2 + v2               ot                         1
                                                        v2     v1


                                                v ' 2 v '1
       In common compare                                      e
                                                v2     v1
2. Subduction Dashes Away to play favorites

         After subduction there is a portion changed mechanical energy as heat energy, sound
         or the other energy. So after subduction available exempt energy. Mechanical energy
         continuity law inoperative. On this subduction is distinguished its elasticity price is 0
         <e<1


    3. Subduction Does Not Dash Away absolutely
         After second object subduction clings to become one and moving with afterses same
         speed subduction both of menyatu's object. E=0's price
BALLISTIC PENDULUM




                                         h
                                                              V’

v
    Gambar 6.5 Bandul-Balistik untuk menentukan kecepatan peluru
If shot mass is m and pendulum mass be m, with momentum
  continuity is gotten

                   mv           (m         M )v '
system energy on the turn as shot potential energy with pendulum until up
until shot oscillation top pendulum


    1                  2
        (m    M )v '       (m       M ) gh           or         v'          2 gh
    2

   If equation in yellow box at merged acquired:


                                m        M
                       v                           2 gh
                                     m
SUBDUCTION IN TWO DIMENSIONS




y                              y




                                             m1




         vo
                         x                             x
    m1        m2




                                                  m2
kelesterian is momentum for each one aim
      Wicked aim x:               m m vo   m 1 v 1 cos .        m 2 v 2 cos .

     Wicked aim y:                0    m 1 v1 sin          m 2 v 2 sin

  If subduction gets elastic character          1          2      1        2        1       2
                                                    m1v o             m 1 v1            m2v2
                                                2                 2                 2

  But if inelastis's subduction            1      2         1       2      1            2
                                               mv
                                                1 o
                                                                mv1 1
                                                                                   m 2v2       Ei
                                           2                2                  2



  billiard's ball with speed 30 m / s menumbuk serves a ball biliard II. one holds tongue
  and get masses with. After subduction, moving i. ball deviates 30 o of aim originally.
  Look for speed each ball and power aim serves a ball II.. (elastic reputed subduction)
One log gets mass m 1 = 2,0 kg moves along
                        ultrasmooth table surface with runaway speed 10 m / dt.
              In front log is it first available one log get mass m 2 = 5,0 kg moves
                      with runaway speed 3,0 m / unidirectional dt with first log.
                          One spiral spring with tetapan k = 1120 n / m glued on
          second log as it were is shown on image gets what far that spiral spring
                                          termampatkan upon happens subduction?

                                 3,0 m/dt

10 m/dt




   m1                                  m2




                          Kunci = 0,25 m
Rocket Thruster energy
• Rockets early momentum p 1 =mv
• Upon + dt rocket speed increases v + dv. For example
  m mass that gushes about satuan time. Rocket mass
  stays behind m? dt, detached fueled mass? dt.
• If vr relative rocket speed to fuel that gushes.
• v ’ =v vr
• Eventual momentum is (m? dt) (v + dv)
• Fueled momentum that tersembu is v ’ dt
Therefore prevailing: -
mgdt=((m- dt)(v+dv)+v’ dt)-mv

 If m huge therefore m dtdv can be ignored
            So: mdv=vr dt-mgdt
                   dm=- dt, so is gotten:
                                    dm
                     dv        vr             gdt
                                    m
                   By integrates is gotten:
              v=-vrlnm-gt+C
If modan vo mass and kec while t=0 therefore
               vo=-vrlnmo+C
              Dan v=vo-gt+vrln(mo/m)
Neutrino case
• If two object fly to be diqoined by speeds v 1
  and v 2 therefore kinetic energy it also
  separate:
•           Q=K 1 + K 2 =1 / 2 m 1 2 +1 / 2 m 2 2
•     Second particle momentum has to equal
  zero so:
•                       m 1 v 1 = -m 2 v 2
• If both of dikuadratkan's equation and at
  divides two therefore acquired:
1/2m12v12=1/2m22v22
     m1K1=m2K2
If this equation compounded by
equation upon acquired:



      m2                 m1
K1   m1 m 2
              Q   K2   m1 m 2
                                Q
I THINK THAT’S ALL MY PRESENTATION…
    FORGIVE ME FOR MY MISTAKE..
AND SEE YOU IN THE NEXT CONDITION..
ASSALAMU’ALAYKUM WA RAHMATULLAH
          WA BARAKATUH…

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IMPULS AND MOMENTUM

  • 1. Name : Rahmawati Yusri NIM : RSA1C311001
  • 2. APLICATION SUBDUCTION THE MATERIAL PENDULUM SUBDUCTION TWO DIMENSIONS ROCKET
  • 3. IMPULSE AND MOMENTUM RELATIONSHIP • Outgrow style that employs at object up to subduction happening can be depicted by relationship graph among f by t, with that assumption constant styled. F(t) t1 t2 t t
  • 4. • One particle gets mass m one that moving with speed v having linear . momentum p one that constitute multiple among that particle speed with its mass v m p = mv. Legally Newton II. resultant inspires that is conected with one straight proportionate object with velocity F = ma. d ( mv ) dp F dt dt dp=Fdt If each diintegralkan therefore acquired:
  • 5. p2 t2 p1 p2 dp F .dt p1 t1 Linear Momentum continuity If resultant external style that employs at system equal to zero, therefore momentum vector total system makes a abode constant dp 0 dt For particle system p1 p2 ........ pn p
  • 6. SEVERALLY MOMENTUM PRINCIPLE PURPOSE • Two logs A and b one gets mA's masses and mB, one that linked by one spiral spring and lie upon horizontal table without friction. Our spiral spring strungs strikingly both of log to sideways as on image. y A B x O
  • 7. The one log gets positive momentum( A moves in aim + x) and bemomentum negative's the other log (B moving deep tenor –x) from hokum our conservation of momentum gets: Early momentum = final momentum 0 mBvB m Av A mBvB m Av A Or mB vA vB mA
  • 8. SUBDUCTION sebelum selama setelah SUBDUCTION TYPES 1. Subduction Dashes Away perfect A subduction is said dash away perfect if jumlahan object kinetic energies that get good subduction before and after subduction with . (Energy continuity law kinetic)
  • 9. m2 m1 m2 m1 v1 v2 v’1 v’2 sebelum sesudah Gambar 6.4. Tumbukan dua benda momentun early totaled: paw = m1v1 + m2v2 Ekaw = m1v12 + m2v22. total early kinetic energy: second totaled momentum that object subduction afters is pak = m1v’1 + m2v’2 totaled kinetic energy after subduction is Ekak = m1v’12 + m2v2’ 2.
  • 10. paw = pak m1v1 + m2v2 = m1v’1 + m2v’2 m1(v1 − v’1) = m2(v’2 − v2), Ekaw = Ekak m1v12 + m2v22 = m1v’12 + m2v2’ 2 or m1v12 − m1v’12 = m2v2’ 2 − m2v22 or m1 (v1 − v’1)( v1 + v’1) = m2(v’2 − v2) (v’2 + v2) Of two box deep equations tingle to be gotten v ' 2 v '1 v1 + v’1 = v’2 + v2 ot 1 v2 v1 v ' 2 v '1 In common compare e v2 v1
  • 11. 2. Subduction Dashes Away to play favorites After subduction there is a portion changed mechanical energy as heat energy, sound or the other energy. So after subduction available exempt energy. Mechanical energy continuity law inoperative. On this subduction is distinguished its elasticity price is 0 <e<1 3. Subduction Does Not Dash Away absolutely After second object subduction clings to become one and moving with afterses same speed subduction both of menyatu's object. E=0's price
  • 12. BALLISTIC PENDULUM h V’ v Gambar 6.5 Bandul-Balistik untuk menentukan kecepatan peluru
  • 13. If shot mass is m and pendulum mass be m, with momentum continuity is gotten mv (m M )v ' system energy on the turn as shot potential energy with pendulum until up until shot oscillation top pendulum 1 2 (m M )v ' (m M ) gh or v' 2 gh 2 If equation in yellow box at merged acquired: m M v 2 gh m
  • 14. SUBDUCTION IN TWO DIMENSIONS y y m1 vo x x m1 m2 m2
  • 15. kelesterian is momentum for each one aim Wicked aim x: m m vo m 1 v 1 cos . m 2 v 2 cos . Wicked aim y: 0 m 1 v1 sin m 2 v 2 sin If subduction gets elastic character 1 2 1 2 1 2 m1v o m 1 v1 m2v2 2 2 2 But if inelastis's subduction 1 2 1 2 1 2 mv 1 o mv1 1 m 2v2 Ei 2 2 2 billiard's ball with speed 30 m / s menumbuk serves a ball biliard II. one holds tongue and get masses with. After subduction, moving i. ball deviates 30 o of aim originally. Look for speed each ball and power aim serves a ball II.. (elastic reputed subduction)
  • 16. One log gets mass m 1 = 2,0 kg moves along ultrasmooth table surface with runaway speed 10 m / dt. In front log is it first available one log get mass m 2 = 5,0 kg moves with runaway speed 3,0 m / unidirectional dt with first log. One spiral spring with tetapan k = 1120 n / m glued on second log as it were is shown on image gets what far that spiral spring termampatkan upon happens subduction? 3,0 m/dt 10 m/dt m1 m2 Kunci = 0,25 m
  • 17. Rocket Thruster energy • Rockets early momentum p 1 =mv • Upon + dt rocket speed increases v + dv. For example m mass that gushes about satuan time. Rocket mass stays behind m? dt, detached fueled mass? dt. • If vr relative rocket speed to fuel that gushes. • v ’ =v vr • Eventual momentum is (m? dt) (v + dv) • Fueled momentum that tersembu is v ’ dt
  • 18. Therefore prevailing: - mgdt=((m- dt)(v+dv)+v’ dt)-mv If m huge therefore m dtdv can be ignored So: mdv=vr dt-mgdt dm=- dt, so is gotten: dm dv vr gdt m By integrates is gotten: v=-vrlnm-gt+C If modan vo mass and kec while t=0 therefore vo=-vrlnmo+C Dan v=vo-gt+vrln(mo/m)
  • 19. Neutrino case • If two object fly to be diqoined by speeds v 1 and v 2 therefore kinetic energy it also separate: • Q=K 1 + K 2 =1 / 2 m 1 2 +1 / 2 m 2 2 • Second particle momentum has to equal zero so: • m 1 v 1 = -m 2 v 2 • If both of dikuadratkan's equation and at divides two therefore acquired:
  • 20. 1/2m12v12=1/2m22v22 m1K1=m2K2 If this equation compounded by equation upon acquired: m2 m1 K1 m1 m 2 Q K2 m1 m 2 Q
  • 21. I THINK THAT’S ALL MY PRESENTATION… FORGIVE ME FOR MY MISTAKE.. AND SEE YOU IN THE NEXT CONDITION.. ASSALAMU’ALAYKUM WA RAHMATULLAH WA BARAKATUH…