Determining final speed of a billiard ball after elastic collision











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A billiard ball traveling at 3.00 m/s collides perfectly elastically with an identical billiard ball initially at rest on the level table. The initially moving billiard ball deflects 30.0° from its original direction. What is the speed of the initially stationary billiard ball after the collision?



I set up two relationships involving momentum as follows



Let $m$ be the mass of both identical billiard balls, $v_1$ be speed of the initially moving billiard ball after the collision, $v_2$ be speed of the initially stationary billiard ball after the collision, and $theta$ be the angle between the velocity vector of the second billiard ball after the collision and the direction of the initial momentum vector



Based on conservation of momentum:



$$1) quad(3m/s)m=mv_1cos(30^circ)+mv_2cos(theta)$$
$$(3m/s)=v_1cos(30^circ)+v_2cos(theta)$$
$$2) quad v_1sin(30^circ)=v_2sin(theta)$$



However this is as far as I got and I don't know how to solve for $v_2$.
Am I missing something?



Btw I know that the answer is 1.5m/s.










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  • you are missing that energy is conserved in an elastic collision and $v_1^2 + v_2^2 = 3^2$
    – Doug M
    Nov 13 at 1:13















up vote
1
down vote

favorite












A billiard ball traveling at 3.00 m/s collides perfectly elastically with an identical billiard ball initially at rest on the level table. The initially moving billiard ball deflects 30.0° from its original direction. What is the speed of the initially stationary billiard ball after the collision?



I set up two relationships involving momentum as follows



Let $m$ be the mass of both identical billiard balls, $v_1$ be speed of the initially moving billiard ball after the collision, $v_2$ be speed of the initially stationary billiard ball after the collision, and $theta$ be the angle between the velocity vector of the second billiard ball after the collision and the direction of the initial momentum vector



Based on conservation of momentum:



$$1) quad(3m/s)m=mv_1cos(30^circ)+mv_2cos(theta)$$
$$(3m/s)=v_1cos(30^circ)+v_2cos(theta)$$
$$2) quad v_1sin(30^circ)=v_2sin(theta)$$



However this is as far as I got and I don't know how to solve for $v_2$.
Am I missing something?



Btw I know that the answer is 1.5m/s.










share|cite|improve this question
























  • you are missing that energy is conserved in an elastic collision and $v_1^2 + v_2^2 = 3^2$
    – Doug M
    Nov 13 at 1:13













up vote
1
down vote

favorite









up vote
1
down vote

favorite











A billiard ball traveling at 3.00 m/s collides perfectly elastically with an identical billiard ball initially at rest on the level table. The initially moving billiard ball deflects 30.0° from its original direction. What is the speed of the initially stationary billiard ball after the collision?



I set up two relationships involving momentum as follows



Let $m$ be the mass of both identical billiard balls, $v_1$ be speed of the initially moving billiard ball after the collision, $v_2$ be speed of the initially stationary billiard ball after the collision, and $theta$ be the angle between the velocity vector of the second billiard ball after the collision and the direction of the initial momentum vector



Based on conservation of momentum:



$$1) quad(3m/s)m=mv_1cos(30^circ)+mv_2cos(theta)$$
$$(3m/s)=v_1cos(30^circ)+v_2cos(theta)$$
$$2) quad v_1sin(30^circ)=v_2sin(theta)$$



However this is as far as I got and I don't know how to solve for $v_2$.
Am I missing something?



Btw I know that the answer is 1.5m/s.










share|cite|improve this question















A billiard ball traveling at 3.00 m/s collides perfectly elastically with an identical billiard ball initially at rest on the level table. The initially moving billiard ball deflects 30.0° from its original direction. What is the speed of the initially stationary billiard ball after the collision?



I set up two relationships involving momentum as follows



Let $m$ be the mass of both identical billiard balls, $v_1$ be speed of the initially moving billiard ball after the collision, $v_2$ be speed of the initially stationary billiard ball after the collision, and $theta$ be the angle between the velocity vector of the second billiard ball after the collision and the direction of the initial momentum vector



Based on conservation of momentum:



$$1) quad(3m/s)m=mv_1cos(30^circ)+mv_2cos(theta)$$
$$(3m/s)=v_1cos(30^circ)+v_2cos(theta)$$
$$2) quad v_1sin(30^circ)=v_2sin(theta)$$



However this is as far as I got and I don't know how to solve for $v_2$.
Am I missing something?



Btw I know that the answer is 1.5m/s.







classical-mechanics






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edited Nov 13 at 1:02









David G. Stork

8,97621232




8,97621232










asked Nov 13 at 0:53









Anson Pang

523




523












  • you are missing that energy is conserved in an elastic collision and $v_1^2 + v_2^2 = 3^2$
    – Doug M
    Nov 13 at 1:13


















  • you are missing that energy is conserved in an elastic collision and $v_1^2 + v_2^2 = 3^2$
    – Doug M
    Nov 13 at 1:13
















you are missing that energy is conserved in an elastic collision and $v_1^2 + v_2^2 = 3^2$
– Doug M
Nov 13 at 1:13




you are missing that energy is conserved in an elastic collision and $v_1^2 + v_2^2 = 3^2$
– Doug M
Nov 13 at 1:13










2 Answers
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If the question is about an elastic collision then no energy is lost in the collision, kinetic energy in = kinetic energy out. This should give you another equation to solve your problem - at the moment you have 3 unknowns and 2 equations - conserve energy and you will have 3 equations and should be able to solve.



The three unknowns are $v_1$, $v_2$ and $theta$, of course, and the two equations you have are linear momentum conservation in the 2 dimensions of the 2D plane the collision occurs in - add conservation of energy and you should be able to solve the problem.






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    Momentum and energy must be conserved.



    $v_1 cos 30^circ + v_2 cos theta = 3\
    v_1 sin 30^circ + v_2 sin theta = 0\
    v_1^2 + v_2^2 = 9$



    The first two equations describe the momentum of the system, the last describes the energy.



    $theta = arcsin frac {v_1}{2v_2}\
    v_1 frac {sqrt 3}{2} + v_2 sqrt {1-frac {v_1^2}{4v_2^2}} = 3\
    v_1 sqrt 3+ sqrt {4v_2^2-v_1^2} = 6\
    sqrt {36 - 5v_1^2} = 6 - v_1sqrt 3\
    36 - 5v_1^2 = 36 - v_112sqrt 3 + 3v_1^2\
    12sqrt 3 v_1 = 8v_1^2\
    v_1 = 0 text { or } v_1 = frac {3sqrt 3}{2}$



    If $v_1 = 0$ then it isn't rolling away at a $30^circ$ deflection.



    $v_2 = 9 - frac {27}{4} = 2.25$






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      2 Answers
      2






      active

      oldest

      votes








      2 Answers
      2






      active

      oldest

      votes









      active

      oldest

      votes






      active

      oldest

      votes








      up vote
      0
      down vote













      If the question is about an elastic collision then no energy is lost in the collision, kinetic energy in = kinetic energy out. This should give you another equation to solve your problem - at the moment you have 3 unknowns and 2 equations - conserve energy and you will have 3 equations and should be able to solve.



      The three unknowns are $v_1$, $v_2$ and $theta$, of course, and the two equations you have are linear momentum conservation in the 2 dimensions of the 2D plane the collision occurs in - add conservation of energy and you should be able to solve the problem.






      share|cite|improve this answer

























        up vote
        0
        down vote













        If the question is about an elastic collision then no energy is lost in the collision, kinetic energy in = kinetic energy out. This should give you another equation to solve your problem - at the moment you have 3 unknowns and 2 equations - conserve energy and you will have 3 equations and should be able to solve.



        The three unknowns are $v_1$, $v_2$ and $theta$, of course, and the two equations you have are linear momentum conservation in the 2 dimensions of the 2D plane the collision occurs in - add conservation of energy and you should be able to solve the problem.






        share|cite|improve this answer























          up vote
          0
          down vote










          up vote
          0
          down vote









          If the question is about an elastic collision then no energy is lost in the collision, kinetic energy in = kinetic energy out. This should give you another equation to solve your problem - at the moment you have 3 unknowns and 2 equations - conserve energy and you will have 3 equations and should be able to solve.



          The three unknowns are $v_1$, $v_2$ and $theta$, of course, and the two equations you have are linear momentum conservation in the 2 dimensions of the 2D plane the collision occurs in - add conservation of energy and you should be able to solve the problem.






          share|cite|improve this answer












          If the question is about an elastic collision then no energy is lost in the collision, kinetic energy in = kinetic energy out. This should give you another equation to solve your problem - at the moment you have 3 unknowns and 2 equations - conserve energy and you will have 3 equations and should be able to solve.



          The three unknowns are $v_1$, $v_2$ and $theta$, of course, and the two equations you have are linear momentum conservation in the 2 dimensions of the 2D plane the collision occurs in - add conservation of energy and you should be able to solve the problem.







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered Nov 13 at 1:02









          tom

          1429




          1429






















              up vote
              0
              down vote













              Momentum and energy must be conserved.



              $v_1 cos 30^circ + v_2 cos theta = 3\
              v_1 sin 30^circ + v_2 sin theta = 0\
              v_1^2 + v_2^2 = 9$



              The first two equations describe the momentum of the system, the last describes the energy.



              $theta = arcsin frac {v_1}{2v_2}\
              v_1 frac {sqrt 3}{2} + v_2 sqrt {1-frac {v_1^2}{4v_2^2}} = 3\
              v_1 sqrt 3+ sqrt {4v_2^2-v_1^2} = 6\
              sqrt {36 - 5v_1^2} = 6 - v_1sqrt 3\
              36 - 5v_1^2 = 36 - v_112sqrt 3 + 3v_1^2\
              12sqrt 3 v_1 = 8v_1^2\
              v_1 = 0 text { or } v_1 = frac {3sqrt 3}{2}$



              If $v_1 = 0$ then it isn't rolling away at a $30^circ$ deflection.



              $v_2 = 9 - frac {27}{4} = 2.25$






              share|cite|improve this answer

























                up vote
                0
                down vote













                Momentum and energy must be conserved.



                $v_1 cos 30^circ + v_2 cos theta = 3\
                v_1 sin 30^circ + v_2 sin theta = 0\
                v_1^2 + v_2^2 = 9$



                The first two equations describe the momentum of the system, the last describes the energy.



                $theta = arcsin frac {v_1}{2v_2}\
                v_1 frac {sqrt 3}{2} + v_2 sqrt {1-frac {v_1^2}{4v_2^2}} = 3\
                v_1 sqrt 3+ sqrt {4v_2^2-v_1^2} = 6\
                sqrt {36 - 5v_1^2} = 6 - v_1sqrt 3\
                36 - 5v_1^2 = 36 - v_112sqrt 3 + 3v_1^2\
                12sqrt 3 v_1 = 8v_1^2\
                v_1 = 0 text { or } v_1 = frac {3sqrt 3}{2}$



                If $v_1 = 0$ then it isn't rolling away at a $30^circ$ deflection.



                $v_2 = 9 - frac {27}{4} = 2.25$






                share|cite|improve this answer























                  up vote
                  0
                  down vote










                  up vote
                  0
                  down vote









                  Momentum and energy must be conserved.



                  $v_1 cos 30^circ + v_2 cos theta = 3\
                  v_1 sin 30^circ + v_2 sin theta = 0\
                  v_1^2 + v_2^2 = 9$



                  The first two equations describe the momentum of the system, the last describes the energy.



                  $theta = arcsin frac {v_1}{2v_2}\
                  v_1 frac {sqrt 3}{2} + v_2 sqrt {1-frac {v_1^2}{4v_2^2}} = 3\
                  v_1 sqrt 3+ sqrt {4v_2^2-v_1^2} = 6\
                  sqrt {36 - 5v_1^2} = 6 - v_1sqrt 3\
                  36 - 5v_1^2 = 36 - v_112sqrt 3 + 3v_1^2\
                  12sqrt 3 v_1 = 8v_1^2\
                  v_1 = 0 text { or } v_1 = frac {3sqrt 3}{2}$



                  If $v_1 = 0$ then it isn't rolling away at a $30^circ$ deflection.



                  $v_2 = 9 - frac {27}{4} = 2.25$






                  share|cite|improve this answer












                  Momentum and energy must be conserved.



                  $v_1 cos 30^circ + v_2 cos theta = 3\
                  v_1 sin 30^circ + v_2 sin theta = 0\
                  v_1^2 + v_2^2 = 9$



                  The first two equations describe the momentum of the system, the last describes the energy.



                  $theta = arcsin frac {v_1}{2v_2}\
                  v_1 frac {sqrt 3}{2} + v_2 sqrt {1-frac {v_1^2}{4v_2^2}} = 3\
                  v_1 sqrt 3+ sqrt {4v_2^2-v_1^2} = 6\
                  sqrt {36 - 5v_1^2} = 6 - v_1sqrt 3\
                  36 - 5v_1^2 = 36 - v_112sqrt 3 + 3v_1^2\
                  12sqrt 3 v_1 = 8v_1^2\
                  v_1 = 0 text { or } v_1 = frac {3sqrt 3}{2}$



                  If $v_1 = 0$ then it isn't rolling away at a $30^circ$ deflection.



                  $v_2 = 9 - frac {27}{4} = 2.25$







                  share|cite|improve this answer












                  share|cite|improve this answer



                  share|cite|improve this answer










                  answered Nov 13 at 1:37









                  Doug M

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