Conservation of Momentum and Energy for a System of Connected Particles

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SUMMARY

The discussion focuses on the conservation of momentum and energy for a system of three connected particles: Q (mass 2m) and P, R (each mass m), constrained by inextensible strings on a smooth horizontal table. The initial conditions specify that particle Q is projected with speed u in the positive x-direction. The conservation equations are established, leading to the derivation of the relationship for theta, expressed as (theta-dot)^2=(u^2/a^2)*(1/(2-cos^2(theta))). The participants confirm the setup of the conservation equations and the validity of the derived expressions.

PREREQUISITES
  • Understanding of conservation of momentum principles
  • Familiarity with conservation of energy equations
  • Knowledge of angular motion and kinematics
  • Basic proficiency in calculus for deriving relationships
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  • Study the derivation of conservation laws in multi-particle systems
  • Learn about the dynamics of connected particles and constraints
  • Explore the application of Lagrangian mechanics in similar systems
  • Investigate the effects of different initial velocities on system behavior
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This discussion is beneficial for physics students, educators, and anyone interested in classical mechanics, particularly in the analysis of systems involving multiple connected bodies and the application of conservation laws.

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Homework Statement



A particle Q has mass 2m and two other particles P, R, each of mass m, are connected to Q by light inextensible strings of length a. The system is free to move on a smooth horizontal table. Initially P, Q R are at the points (0,a),(0,0),(0,-a) respectively so that they lie in a straight line with the strings taut. Q is then projected in the positive x-direction with speed u. express the conservation of linear momentum and energy for this system in terms of the coordinates x(the displacement of Q) and theta(the angle by each of the strings(.

Show that theta satisfies the equation

(theta-dot)^2=(u^2/a^2)*(1/(2-cos^2(theta))


Homework Equations



equations for conservation of energy
equation for conservation of momemtum.


The Attempt at a Solution



F [tex]\cdot[/tex] x-hat=0
p [tex]\cdot[/tex]x-hat=0

p[tex]\cdot[/tex]x-hat=(m1*v1+m2*v2) [tex]\cdot[/tex] x-hat= 2m*v_x+m(v_x+(a*theta_dot*cos(theta))= 3m(v_x)+m*a*theta_dot*cos(theta)==> 3*(v_x)+a*theta_dot*cos(theta)=0

T_1+T_2; T_1 is the kinetic energy initial and T_2 is the final kinetic energy.
V=V_1-V_2=0-m*g*a*cos(theta)
rail is smooth therefore constraint force does no work and E is convserved.

T=T_1+T_2=.5*(2m)*v_x^2+.5*m*(v_2)^2

v_2=v_2x+v_2theta

v_2= (v_x)^2+(a*theta_dot)^2+2*v_x*(a*theta_dot)*cos(theta)

T_1 would be zero since the mass is initiall at rest.

1/2*m*(3v_x^2+a^2*theta_dot^2+2*a*x_dot*theta_dot*cos(theta))-mga=mga*cos(theta)

Did I set up my conservation of energy equation correctly ?
 
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