Animated Solution for Physics - System of Particles: Two particles of equal mass m have respective initial velocities ui^ and u(2i^+j^). They collide completely inelastically. The energy lost in the process is
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Visualized Solution
Visualizing the Collision
v1=ui^
v2=2u(i^+j^)
Conservation of Momentum
Completely Inelastic Collision
Pi=Pf
Setting up the Equation
m(ui^)+m(2ui^+2uj^)=(2m)v
Solving for Final Velocity
ui^+2ui^+2uj^=2v
23ui^+21uj^=2v
v=43ui^+41uj^
Energy Loss Framework
ΔK=Ki−Kf
v2=vx2+vy2
Initial Kinetic Energy
Ki=21mu2+21m[(2u)2+(2u)2]
Ki=21mu2+21m(2u2)
Ki=21mu2+41mu2=43mu2
Final Kinetic Energy
Kf=21(2m)v2
Kf=m[(43u)2+(41u)2]
Kf=m(169u2+161u2)=85mu2
Energy Lost
ΔK=43mu2−85mu2
ΔK=(86−85)mu2
ΔK=81mu2
The Way Forward
Energy is dissipated as heat/sound.
tanθ=vxvy=3/41/4=31
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The Sigma Insight: Conservation of Linear Momentum
Solution Diagram
In the fascinating world of mechanics, collisions are a perfect playground to test our understanding of conservation laws. When two objects collide, the outcome depends heavily on the nature of the collision. In this problem, we are dealing with a completely inelastic collision, a scenario where objects stick together upon impact, moving as a single entity afterwards.
Let's break down the physics and mathematics behind this event step-by-step.
Setting the Stage
The Collision Course
Imagine two particles, each possessing a mass m, moving in a two-dimensional plane. The first particle is moving purely along the x-axis with a velocity vector:
v1=ui^
The second particle is moving at an angle, with its velocity vector given by:
v2=2u(i^+j^)=2ui^+2uj^
These two particles are on a collision course. Because the collision is completely inelastic, they will merge into a single combined mass of 2m moving with some final velocity v.
The Master Equation
Conservation of Momentum
In any collision where external forces are absent, the total linear momentum of the system is strictly conserved. This is our master key to unlocking the final velocity. We equate the initial momentum of the system to its final momentum:
Pi=Pf
Substituting the momenta of our particles, we get:
m(ui^)+m(2ui^+2uj^)=(2m)v
Notice how the mass m is common to all terms. We can elegantly cancel it out, simplifying our equation to:
ui^+2ui^+2uj^=2v
Combining the i^ components, we find:
23ui^+21uj^=2v
Dividing the entire equation by 2 yields the final velocity vector of the combined mass:
v=43ui^+41uj^
Calculating the Kinetic Energies
To find the energy lost during the collision, we must calculate the kinetic energy before and after the impact. Remember, kinetic energy is a scalar quantity defined as K=21mv2. For a velocity vector, the square of the speed v2 is simply the sum of the squares of its orthogonal components (v2=vx2+vy2).
Let's calculate the initial kinetic energy (Ki), which is the sum of the kinetic energies of the two individual particles:
Ki=21mu2+21m[(2u)2+(2u)2]
Ki=21mu2+21m(4u2+4u2)
Ki=21mu2+21m(2u2)=21mu2+41mu2
Ki=43mu2
Now, let's calculate the final kinetic energy (Kf) of the combined mass 2m moving with velocity v:
Kf=21(2m)v2=m[(43u)2+(41u)2]
Kf=m(169u2+161u2)=m(1610u2)
Kf=85mu2
The Final Reveal
Energy Lost
In a completely inelastic collision, maximum kinetic energy is dissipated (usually as heat, sound, or deformation energy). The energy lost (ΔK) is the difference between the initial and final kinetic energies:
ΔK=Ki−Kf
ΔK=43mu2−85mu2
To subtract these fractions, we find a common denominator of 8:
ΔK=(86−85)mu2
ΔK=81mu2
This elegant result shows exactly how much of the system's initial kinetic energy was sacrificed to bind the two particles together!