A ball with a mass of #4# #kg# and velocity of #5# #ms^-1# collides with a second ball with a mass of #6# #kg# and velocity of #-1# #ms^-1#. If #20%# of the kinetic energy is lost, what are the final velocities of the balls?

Answer 1

Momentum is conserved. Kinetic energy is not, but in this case we know that final #E_k# is 0.8 times initial #E_k#.

The final velocity of the #4# #kg# ball is #-2.38# #ms^-1# and the final velocity of the #6# #kg# ball is #2.73# #ms^-1#.

Let's call the #4# #kg# ball Ball 1 and the #6# #kg# ball Ball 2, just for the convenience of subscripts...

Prior to the collision:

vigor:

#p=m_1v_1+m_2v_2=4xx5+6xx(-1)=14# #kgms^-1#

Energy in motion:

#E_k=1/2m_1v_1^2+1/2m_2v_2^2=1/2xx4xx5^2+1/2xx6xx(-1)^2# #=50+3=53# #J#

Following the collision:

vigor:

#p=m_1v_1+m_2v_2=4v_1+6v_2#

Energy in motion:

#E_k=1/2m_1v_1^2+1/2m_2v_2^2=1/2xx4xxv_1^2+1/2xx6xxv_2^2#
We know that momentum is conserved, so the momentum after the collision will be #14# #kgms^-1#, as it was before the collision.
20% of the kinetic energy is lost to other forms of energy like heat and sound, so 80% will remain: #0.8xx53=33.9# #J#

We are left with two equations involving two unknowns:

Equation 1: #4v_1+6v_2=14#
Equation 2: #2v_1^2+3v_2^2=33.9#
Rearranging Equation 1 to make #v_1# the subject:
#v_1=(14-6v_2)/4#

Putting this in place of Equation 2:

#2((14-6v_2)/4)^2+3v_2^2=33.9#

It's just algebra, so I'll leave you to solve this equation, which involves solving a quadratic equation.

The solution is that #v_2=2.73# or #1.75# #ms^-1#
Substituting this back into Equation 1 and solving we find that #v_1=-2.38# or #3.5# #ms^-1# respectively.

Assume that the "+" direction is from left to right and the "-" direction is from right to left in order to determine which set of answers we want.

Initially, the #4# #kg# ball was moving left-to-right and the #6# #kg# ball was moving right-to-left. After the collision, we can imagine that they have both bounced in the opposite direction: the #4# #kg# ball is now traveling right-to-left and has a negative velocity, the #6# #kg# ball has a positive velocity.

Physically speaking, the other set of answers is nonsensical because it assumes that the left-hand ball is moving more quickly to the right than the right-hand ball.

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Answer 2

#4kg " ball"=-1ms^-1 and 6kg " ball"=3ms^-1#
#4kg " ball"=1.52ms^-1 and 6kg " ball"=1.32ms^-1#

We notice that velocity of one ball is given as #5ms^-1# and of the other is given as #-1ms^-1#. This implies that both the balls are moving in a direction opposite to each other. both the balls have been given. Let #x# direction be defined by the positive velocity.

Before the collision

Momentum, in #x# direction only
#p_i=4xx5+6xx(-1)=14kgms^-1#
Kinetic energy #KE_i=1/2xx4xx5^2+1/2xx6xx(-1)^2#
#=50+3=53J#
After the collision Let #v_(1x) and v_(2x)# be #x# components of respective velocities of #4kg and 6kg# balls and #v_(1y) and v_(2y)# be #y# components of their respective velocities.

Momentum:

#p_(fx)=4v_(1x)+6v_(2x)# and #p_(fy)=4v_(1y)+6v_(2y)# Since momentum is conserved, we have
#14=4v_(1x)+6v_(2x)# .....(1) #0=4v_(1y)+6v_(2y)# .....(2)

Kinetic energy:

#KE_f=1/2xx 4(v_(1x)^2+v_(1y)^2)+1/2 xx6(v_(2x)^2+v_(2y)^2)#
Given is that #20%# kinetic energy is lost. #:. KE_f=0.8xx53=42.4J# This gives us
#42.4=2(v_(1x)^2+v_(1y)^2)+3(v_(2x)^2+v_(2y)^2)# .....(3)
Thus we have three equations in four unknowns. To find a solution lets assume that even after collision the balls move along the #x# direction only. Implies that equation (2) vanishes. And we have two equations to solve for two variables.
#4v_(1x)+6v_(2x)=14# ......(4)
#2v_(1x)^2+3v_(2x)^2=42.4# ....(5)
Dropping the suffix #x# we get
#4v_1+6v_2=14# ......(6)
#2v_1^2+3v_2^2=42.4# ....(7)
Substituting value of #v_1# from (6) in (7) #v_1=(14-6v_2)/4#
#=>2((14-6v_2)/4)^2+3v_2^2=42.4# #=>(196-168v_2+36v_2^2)+3v_2^2=42.4# #=>39v_2^2-168v_2+153.6=0# #=>13v_2^2-56v_2+51.2=0# Solving the quadratic #v_2=(-(-56)+-sqrt((-56)^2+4xx13xx51.2))/(2xx13)# #v_2=(56+-sqrt(3136-4xx13xx51.2))/(26)# #v_2=(56+-21.8)/(26)# #v_2=3, 1.32# From (6) corresponding values of #v_1=-1, 1.52#
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Answer 3

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

Let ( v_1 ) and ( v_2 ) be the final velocities of the first and second balls, respectively.

According to the conservation of momentum:

( m_1 \cdot v_{1i} + m_2 \cdot v_{2i} = m_1 \cdot v_1 + m_2 \cdot v_2 )

where ( m_1 ) and ( m_2 ) are the masses of the first and second balls, and ( v_{1i} ) and ( v_{2i} ) are their initial velocities.

Given: ( m_1 = 4 ) kg, ( v_{1i} = 5 ) m/s, ( m_2 = 6 ) kg, ( v_{2i} = -1 ) m/s.

Applying the conservation of momentum:

( 4 \cdot 5 + 6 \cdot (-1) = 4 \cdot v_1 + 6 \cdot v_2 )

( 20 - 6 = 4v_1 + 6v_2 )

( 14 = 4v_1 + 6v_2 ) ...(1)

Now, to consider the kinetic energy loss, let ( KE_i ) be the initial kinetic energy and ( KE_f ) be the final kinetic energy.

Given that 20% of kinetic energy is lost, ( KE_f = 0.8 \times KE_i ).

( KE_i = \frac{1}{2} m_1 v_{1i}^2 + \frac{1}{2} m_2 v_{2i}^2 )

( KE_f = \frac{1}{2} m_1 v_1^2 + \frac{1}{2} m_2 v_2^2 )

Substituting the given values:

( 0.8 \times (\frac{1}{2} \cdot 4 \cdot 5^2 + \frac{1}{2} \cdot 6 \cdot (-1)^2) = \frac{1}{2} \cdot 4 \cdot v_1^2 + \frac{1}{2} \cdot 6 \cdot v_2^2 )

( 0.8 \times (50 + 3) = 2v_1^2 + 3v_2^2 )

( 0.8 \times 53 = 2v_1^2 + 3v_2^2 )

( 42.4 = 2v_1^2 + 3v_2^2 ) ...(2)

Now, we have two equations (equation 1 and equation 2) with two unknowns ( v_1 ) and ( v_2 ). We can solve them simultaneously to find the final velocities of the balls.

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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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