A ball with a mass of #4 kg # and velocity of #3 m/s# collides with a second ball with a mass of #5 kg# and velocity of #- 2 m/s#. If #20%# of the kinetic energy is lost, what are the final velocities of the balls?

Answer 1

Ball 1: #\vec(v_(1_f)) = -2.11# m/s
Ball 2: #\vec(v_(2_f)) = 2.21# m/s

Collisions can be represented using momentum relations.

Momentum is defined as: #\vecp=m\vecv#
Using the values provided, we see the initial momenta are: #\vec(p_(1_i)) = (4)(3) = 12# kg#*#m/s #\vec(p_(2_i)) = (5)(-2) = -10# kg#*#m/s
The total net momentum of the system initially is: #\vec(p_(Total_i)) = \vec(p_(1_i))+\vec(p_(2_i)) = 12 -10=2# kg#*#m/s
Since momentum is conserved, we know the magnitude of the momentum after the collision is also #2# kg#*#m/s.
Energy (kinetic) is defined as: #E = 1/2 m v^2#
Using the values provided, we see the initial energies are: #E_(1_i) = 1/2(4)(3)^2 = 18# J #E_(2_i) = 1/2 (5)(-2)^2 = 10# J
The total energy of the system initially is: #E_(Total_i) = E_1 + E_2 = 18+10=28# J
Since we are told 20% of the energy is lost (80% remains), the energy is NOT conserved after the collision. The energy after the collision is: #E_(Total_f) = 0.8E_(Total_i) = (0.8)(28) = 22.4# J

Now we can form some equations describing the post-collision system, which we can use to find the velocities of the balls.

They are magnitude of total momentum: #4v_(1_f) + 5v_(2_f) = 2# kg#*#m/s
and total energy: #2v_(1_f)^2 + 5/2 v_(2_f)^2 = 22.4# J
We can now solve this system of equations (1) #4v_(1_f) + 5v_(2_f) = 2# (2) #2v_(1_f)^2 + 2.5 v_(2_f)^2 = 22.4#
We can divide equation (1) by 4 and solve for #v_(1_f)#: (3) #v_(1_f) = 0.5 - 1.25v_(2_f)#
Substituting (3) into (2) gives: #2(0.5 - 1.25v_(2_f))^2 + 2.5 v_(2_f)^2 = 22.4# #2(0.25-1.25v_(2_f)+1.5625v_(2_f)^2) + 2.5 v_(2_f)^2 = 22.4# #0.5-2.5v_(2_f)+3.125v_(2_f)^2 + 2.5 v_(2_f)^2 = 22.4# #5.625v_(2_f)^2-2.5v_(2_f)-21.9 = 0#
This quadratic can now be solved using the quadratic equation: #v_(2_f)=(-b+-sqrt(b^2-4ac))/(2a)# where #a=5.625#, #b=-2.5#, and #c=-21.9#
This gives: #v_(2_f) = 2.21# m/s and #v_(2_f) = -1.76# m/s
Since ball 2 originally travels in the negative direction, after the collision it will go in the positive direction. So we accept the root that is positive. Hence: #v_(2_f) = 2.21# m/s
Now we can use this value in equation (1) to find the value of #v_(1_f)#: #4v_(1_f) + 5(2.21) = 2# #v_(1_f) = -2.11# m/s

It is good that this value is negative, as ball 1 was originally traveling in the positive direction. Post-collision, it should go the opposite direction.

Hence we have found the final velocities of the balls:

Ball 1: #\vec(v_(1_f)) = -2.11# m/s Ball 2: #\vec(v_(2_f)) = 2.21# m/s
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Answer 2

To find the final velocities of the balls after the collision, we can use the principle of conservation of momentum and the equation for kinetic energy.

  1. Conservation of momentum: (m_1v_1 + m_2v_2 = m_1v_{1f} + m_2v_{2f})

  2. Equation for kinetic energy: (KE = \frac{1}{2}mv^2)

Using these equations, we can solve for the final velocities (v_{1f}) and (v_{2f}):

For the first ball: Initial momentum: (4 \times 3 + 5 \times (-2) = 12 - 10 = 2) kg m/s Initial kinetic energy: (\frac{1}{2} \times 4 \times 3^2 = 18) J Final kinetic energy: (0.8 \times 18 = 14.4) J Final velocity: (\sqrt{\frac{2 \times 14.4}{4}} = 1.2) m/s

For the second ball: Initial momentum: (4 \times 3 + 5 \times (-2) = 12 - 10 = 2) kg m/s Initial kinetic energy: (\frac{1}{2} \times 5 \times (-2)^2 = 10) J Final kinetic energy: (0.8 \times 10 = 8) J Final velocity: (\sqrt{\frac{2 \times 8}{5}} \approx 0.8) m/s

So, the final velocities of the balls are approximately (1.2 , \text{m/s}) and (0.8 , \text{m/s}) respectively.

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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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