In outer space, rock 1 whose mass is5Kg and whose velocity was(3300,-3100,3400)m/s struck rock 2, which was at rest. After the collision, rock 1’s velocity is(2800,-2400,3700)m/s . (a) What is the final momentum of rock 2? (b) Before the collision, what was the kinetic energy of rock 1? (c) Before the collision, what was the kinetic energy of rock 2? (d) After the collision, what is the kinetic energy of rock 1? (e) Suppose that the collision was elastic (that is, there was no change in kinetic energy and therefore no change in thermal or other internal energy of the rocks). In that case, after the collision, what is the kinetic energy of rock 2? (f) On the other hand, suppose that in the collision some of the kinetic energy is converted into thermal energy of the two rocks, whereEthermal,1+Ethermal,2=7.16×106J . What is the final kinetic energy of rock 2? (g) In this case (some of the kinetic energy being converted to thermal energy), what was the transfer of energy Q (microscopic work) from the surroundings into the two-rock system during the collision? (Remember that Q represents energy transfer due to a temperature difference between a system and its surroundings.)

Short Answer

Expert verified
a)(2500,-3500,-1500)kg.m/sb)8.01×107Jc)0Jd)6.82×107Je)1.2×107Jf)4.8×106Jg)0

Step by step solution

01

Identification of the given data

The given data is listed below as,

  • The mass of the rock 1 is,m1=5kg
  • The initial velocity of the rock 1 isv1i=(3300,-3100,3400)m/s
  • The initial velocity of the rock 2 is,v2i=0
  • The final velocity of the first rock is,v1i=(2800,-2400,3700)m/s
02

Significance of the law of conservation of momentum and energy

The law of conservation of momentum states that the momentum of a system before and after collision remains constant if no external force acts.

The law of conservation of energy states that the total initial kinetic energy of a system equals the addition of the total final kinetic energy and the system’s total thermal energy.

03

Determination of the final momentum of the rock 2

The expression for the initial momentum of the system can be expressed as,

Pinitial=m1v1i+m2v2i

Here,Pinitial is the initial momentum of the system,m1 is the mass of the rock 1,m2 is the mass of the rock 2,v1i is the initial velocity of the rock 1 andv2i is the initial velocity of the rock 2.

.

As the mass of the rock 2 is not given, so, it is assumed that the mass of the rock 2 is form2=8kg simplifying the calculations.

Form1=5kg,v1i=(3300,-3100,3400)m/s

Pinitial=(5kg)×(3300,-3100,3400)m/s+(8kg)×(0m/s)=(16500,-15500,17000)kg.m/s_+0=(16500,-15500,17000)kg.m/s

According to the law of conservation of momentum, the initial and the final rate of the system are the same. So, the final velocity of the system is expressed as,

Pfinal=(m1v1i)+(m2v2i)Pinitial=(m1v1i)+(m2v2i)

Here,v2i is the final velocity of rock 2.

ForPinitial=(16500,-15500,17000)kg.m/s,m1=5kg andv1i=(2800,-2400,3700)m/s .

(16500,-15500,17000)kg.m/s=(5kg)×(2800,-2400,3700)m/s+(8kg)×(v)=(14000,-12000,18500)kg.m/s+(8vkg)(2500,-3500,-1500)kg.m/s=(8vkg)v=312.5,-437.5,187.5m/s

Thus, the final momentum of rock 2 is(2500,-3500,-1500)kg.m/s .

04

Determination of the kinetic energies of the rock 1

The expression for the magnitude of the initial velocity of the rock 1 is expressed as,

v1i=vx2+vy2+vz2

Here,role="math" localid="1657949364982" vx,vy andvz are the velocities of the rock 1 at the x, y, and z coordinate respectively.

For vx=3300m/s,vy=-3100m/sandvz=3400m/s .

v1i=33002+-31002+34002m/s=5662.155m/s

The expression of the kinetic energy of the rock 1 before the collision can be expressed as-

K.E.1i=12m1v1i2

Here, is the mass of rock 1 andv1i is the initial velocity of rock 1.

Form1=5kg andv1i=5662.155m/s .

role="math" localid="1657950103667" K.E.1i=12×(5kg)×(5662.155m/s)2=8.01×107kg.m2/s2×1J1kg.m2/s2=8.01×107J

Thus, the kinetic energy of rock 1 before the collision is8.01×107J .

05

Determination of the kinetic energy of the rock 2 before the collision

As rock 2 was at rest before the collision, then the kinetic energy of rock 2 before the collision is 0.

Thus, the kinetic energy of rock 2 before the collision is0J.

06

Determination of the kinetic energy of the rock 1 after the collision

The expression for the magnitude of the final velocity of the rock 1 is as follows,

v1i=vx2+vy2+vz2

Here, vx,vyandvz are the velocity of the rock 1 at the x, y and z coordinate respectively.

Forvx=2800m/s,vy=-2400m/s andvz=3700m/s .

v1i=28002+-24002+37002m/s=5223.98m/s

The expression for the kinetic energy of the rock 1 after the collision can be expressed as,

K.E.1f=12m1v1f2

Here,m1 is the mass of the rock andv1f is the final velocity of rock 1.

Form1=5kg andv1f=5223.98m/s .

role="math" localid="1657951558267" K.E.1f=12×(5kg)×(5223.98m/s)2=6.82×107kg.m2/s2×1J1kg.m2/s2=6.82×107J

Thus, the kinetic energy of rock 1 after the collision is6.82×107J .

07

Determination of the kinetic energy of the rock 2 after collision

If the collision is elastic, then according to the energy balance, the kinetic energy of rock 2 will be the difference between the initial and the final kinetic energy of rock 1 as the kinetic energy remains constant.

The expression of the final kinetic energy of the rock 2 can be expressed as,

KE2f=KE1i-KE1f

Here,KE1i andKE1f are the initial and the final energy of the rock 1 respectively.

ForKE1i=8.01×107J andKE1f=6.82×107J .

KE2f=8.01×107J-6.82×107J=1.2×107J

Thus, the kinetic energy of the rock 2 is1.2×107J .

08

Determination of the final kinetic energy of the rock 2

From the law of conservation of energy, the equation of the total final and the initial kinetic energy of the system can be expressed as,

K.E.1i+K.E.2i=K.E.1f+K.E.2f+Ethermal,1+Ethermal,2

Here,K.E.1i is the initial kinetic energy of the rock 1,K.E.2i is the initial kinetic energy of the rock 2,K.E.1f is the final kinetic energy of rock 1,K.E.2f is the final kinetic energy of rock 2 andEthermal,1+Ethermal,1 is the change in the thermal energy of the rocks.

For KE1i=8.01×107J,KE1f=8.01×107J,KE2i=0andEthermal,1+Ethermal,2=7.61×106J

8.01×107J+0=6.82×107J+K.E.2f+7.16×106JK.E.2f=8.01×107J-68.2×106J-7.16×106J=4.8×106J

Thus, the final kinetic energy of rock 2 is4.8×106J .

09

Determination of the transfer of energy

Assuming this system is an isolated system, the transfer of energy Q will be 0 when the kinetic energy is converted to thermal energy.

Thus, the energy transfer from the surroundings into the two-rock system during the collision is 0.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Redo Problem P21, this time using the concept of the center-of-momentum reference frame.

A car of mass 2300 kg collides with a truck of mass 4300 kg, and just after the collision the car and truck slide along, stuck together, with no rotation. The car’s velocity just before the collision was⟨38, 0, 0⟩m/s, and the truck’s velocity just before the collision was⟨−16, 0, 27⟩m/s. (a) Your first task is to determine the velocity of the stuck-together car and truck just after the collision. What system and principle should you use? (1) Energy Principle (2) Car plus truck (3) Momentum Principle (4) Car alone (5) Truck alone (b) What is the velocity of the stuck-together car and truck just after the collision? (c) In your analysis in part (b), why can you neglect the effect of the force of the road on the car and truck? (d) What is the increase in internal energy of the car and truck (thermal energy and deformation)? (e) Is this collision elastic or inelastic?

Give an example of what we can learn about matter through the use of momentum and energy conservation applied to scattering experiments. Explain what it is that we cannot learn this way, for which we need to measure the distribution of scattering angles.

Redo the analysis of the Rutherford experiment, this time using the concept of the centre-of-momentum reference frame. Let m = the mass of the alpha particle and M = the mass of the gold nucleus. Consider the specific case of the alpha particle rebounding straight back. The incoming alpha particle has a momentum p1 , the outgoing alpha particle has a momentum p3 , and the gold nucleus picks up a momentum p4 . (a) Determine the velocity of the centre of momentum of the system. (b) Transform the initial momenta to that frame (by subtracting the centre-of-momentum velocity from the original velocities). (c) Show that if the momenta in the centre-of-momentum frame simply turn around (180◦), with no change in their magnitudes, both momentum and energy conservation are satisfied, whereas no other possibilitysatisfies both conservation principles. (Try drawing some other
momentum diagrams.) (d) After the collision, transform back to
the original reference frame (by adding the center-of-momentum
velocity to the velocities of the particles in the center-of-mass
frame). Although using the center-of-momentum frame may be
conceptually more difficult, the algebra for solving for the final
speeds is much simpler

In order to close a door, you throw an object at the door. Which would be more effective in closing the door, a 50g tennis ball or a 50g lump of sticky clay? Explain clearly what physics principles you used to draw your conclusion.

You know that a collision must be “elastic” if: (1) The colliding objects stick together. (2) The colliding objects are stretchy or squishy. (3) The sum of the final kinetic energies equals the sum of the initial kinetic energies. (4) There is no change in the internal energies of the objects (thermal energy, vibrational energy, etc.). (5) The momentum of the two-object system doesn’t change.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free