A ball with a mass of #12 kg# moving at #3 m/s# hits a still ball with a mass of #21 kg#. If the first ball stops moving, how fast is the second ball moving? How much kinetic energy was lost as heat in the collision?

Answer 1

#vec v_1^'=-9/11 " "m/s#
#v_2^'=24/11 " "m/s#

#"Momentums before collision :"#
#vec P_1=m_1*vec v_1" (for the first object)"# #vec P_1=12*3=" "36 kg.m/s#
#vec P_2=m_2*vec v_2" (for the second object)"# #vec P_2=21*0=0#
#Sigma vec P_b=vec P_1+ vec P_2" (total momentum before collision)"# #Sigma vec P_b=36+0=36" " kg*m/s#
#"Momentums after collision :"#
#vec P_1^'=m_1*v_1^'" (for the first object)"# #vec P_1^'=12*v_1^'#
#vec P_2^'=m_2*v_2^'" (for the second object)"# #vec P_2^'=21*v_2^'#
#Sigma vec P_a=vec P_1^'+vec P_2^'" (total momentum after collision)"# #Sigma vec P_a=12*v_1^'+21*v_2^'#
#Sigma vec P_b=Sigma vec P_a" (conservation of momentum")# #36=12*vec v_1^'+21*vec v_2^'" (1)"#
#"We can fallow two ways to solve problem:"#
#"1 )............................................................"#
#v_1+v_1^'=v_2+v_2^' " (using the conservation of kinetic energy)"# #3+v_1^'=0+v_2^'# #v_2^'=3+v_1^' " (2)"#
#"let' use (1)" # #36=12*vec v_1^'+21*(3+vec v_1^')# #36=12*vec v_1^'+63+21*vec v_1^'# #36-63=33*vec v_1^'# #-27=33*vec vec v_1^'#
#vec v_1^'=-27/33" "vec v_1^'=-9/11 " "m/s#
#"now ,let's use (2)"#
#vec v_2^'=3+vec v_1^'# #vec v_2^'=3-9/11" "vec v_2^'=(33-9)/11" "v_2^'=24/11 " "m/s#
#"2)............................................................."#
#v_1^'=(2*Sigma vec P_b)/(m_1+m_2)-v_1#
#v_1^'=(2*36)/(12+21)-3#
#v_1^'=72/33-3" "v_1^'=(72-99)/33 " "v_1^'=-27/33=-9/11 " m/s" #
#v_2^'=(2*Sigma vec P_b)/(m_1+m_2)-v_2#
#v_2^'=(2*36)/(12+21)-0#
#v_2^'=72/33=" "v_2^'=24/11 " "m/s#
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Answer 2

To solve for the final velocity of the second ball, we can use the principle of conservation of momentum:

[m_1v_1 + m_2v_2 = (m_1 + m_2)v_f]

Given:

  • (m_1 = 12 , \text{kg}) (mass of the first ball)
  • (v_1 = 3 , \text{m/s}) (initial velocity of the first ball)
  • (m_2 = 21 , \text{kg}) (mass of the second ball)
  • (v_2 = ?) (initial velocity of the second ball, assumed to be zero)
  • (v_f = 0) (final velocity of both balls)

Using the conservation of momentum equation:

[12 , \text{kg} \times 3 , \text{m/s} + 21 , \text{kg} \times 0 = (12 , \text{kg} + 21 , \text{kg}) \times 0]

[36 , \text{kg}\cdot\text{m/s} = 33 , \text{kg}\cdot\text{m/s}]

[v_2 = \frac{36 , \text{kg}\cdot\text{m/s}}{21 , \text{kg}}]

[v_2 ≈ 1.71 , \text{m/s}]

To find the kinetic energy lost as heat in the collision, we can use the principle of conservation of mechanical energy:

[KE_{\text{initial}} - KE_{\text{final}} = \text{heat energy lost}]

Given:

  • (KE_{\text{initial}} = \frac{1}{2}m_1v_1^2) (initial kinetic energy of the first ball)
  • (KE_{\text{final}} = \frac{1}{2}(m_1 + m_2)v_f^2) (final kinetic energy of both balls, assumed to be zero)
  • (m_1 = 12 , \text{kg}) (mass of the first ball)
  • (v_1 = 3 , \text{m/s}) (initial velocity of the first ball)
  • (m_2 = 21 , \text{kg}) (mass of the second ball)
  • (v_f = 0) (final velocity of both balls)

Using the kinetic energy equations:

[KE_{\text{initial}} = \frac{1}{2}(12 , \text{kg})(3 , \text{m/s})^2] [KE_{\text{initial}} = 54 , \text{J}]

[KE_{\text{final}} = \frac{1}{2}(12 , \text{kg} + 21 , \text{kg}) \times 0^2] [KE_{\text{final}} = 0]

[\text{heat energy lost} = 54 , \text{J} - 0] [\text{heat energy lost} = 54 , \text{J}]

Therefore, the second ball is moving at approximately (1.71 , \text{m/s}), and (54 , \text{J}) of kinetic energy was lost as heat in the collision.

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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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