Hey, guys. So now that I know the basics of completely inelastic collisions, I want to show you another type of problem where you have a mass that's added onto a system that's already moving. So let's go ahead and check this out. The problem we're going to work out down here, we have a sled that's already moving at some speed, and a box gets dropped onto it, so you're adding mass to a system that's already moving. Basically, the idea is that they're very similar to completely inelastic collisions. Whenever this happens, both objects in the system, right, whatever you had before like the sled plus the new mass like the box, have to be moving with the same final velocity. So let's go ahead and take a look at our problem, and we'll come back to this in just a second here. So we have this 70 kilogram sled and a 30 kilogram box. The sled's already moving to the right with 10 meters per second, and then what happens is the box gets dropped onto it. In part a, we want to figure out the final speed of the system. So let's draw our diagrams for before and after. This is the before. What does the after look like? Well, basically now, this sled is moving to the right, but the box is on top of it. So the box is on top of it like this, and because they're on top of it and they basically become one system or one object, they're both moving with the same v final. And that's what we want to figure out here. So let's go ahead and take a look at our energy or, sorry, our momentum conservation equation. So we're going to use \( m_1 v_{1 \text{ initial}} + m_2 v_{2 \text{ initial}} \), and we can use our shortcut for completely inelastic collisions. We know that we can group together the masses because they're both going to have the same \( v_{\text{final}} \). That's what we want to figure out here. So I'm going to just call this, let's see. I'm going to call the sled 1 and the box 2. Alright? So let's take a look. So we're going to have our sled, that's 70. That's \( 70 \times 10 + 30 \times \) some speed here equals \( 70 + 30 \times v_{\text{final}} \). So what goes inside of this parenthesis right here? What's the initial speed of the block? Well, what happens here is that this block gets dropped vertically onto the sled, which means that it has some initial y velocity that I actually don't know. But it turns out it doesn't matter that I don't know it because the box is only dropping vertically, which means it doesn't contribute any x momentum to the system. Basically, if all the velocity is just vertical, what we can say is that \( v_{2x} \) is just equal to 0. It doesn't contribute any horizontal momentum to the system. So what we can do is in our momentum conservation equation, we can just cancel this out and there's actually 0 initial speed. So this actually makes our equation even simpler because now we can do is figure out \( v_{\text{final}} \). So now what we can do is this is 700, and when we divide the 100 from the other side, this becomes our \( v_{\text{final}} \), and this is going to be 7 meters per second. So that's our answer. So it turns out what happens is that you have a sled that's initially moving at 10, and then you're adding mass to the system, and then the final velocity is going to be less. It's going to be 7 meters per second. This should make some sense to you because momentum conservation, \( p = mv \), says that in order for momentum to be conserved, if your mass is increasing, then in order for you to have the same \( p \) as a system, your \( v \) has to go down. If your mass increases, your speed has to decrease proportionally so that you keep the same momentum. Alright? So that's what's happening here. Alright. So now let's go ahead and take a look at parts b and c. So in part b, what we want to do is calculate the change in the momentum of the box. So that's going to be \( \Delta p_2 \). So what's \( \Delta p \)? Remember, it's just going to be \( m_2 (v_{\text{final}} - v_{\text{initial}}) \). It's \( v_{\text{final}} - v_{\text{initial}} \) here. So what we can do is you can group this together, \( m_2 (v_{\text{final}} - v_{\text{initial}}) \) here. Okay. So we have the 30 kilogram box, and then what's the \( v_{\text{final}} \)? The \( v_{\text{final}} \) is just the 7 meters per second that we just calculated here. So 7 minus what's the initial speed of the box? Well, remember, it's just 0. So what ends up happening is you got a change of momentum of 210. Let's do the same exact thing now for part c, except now we want to calculate the change in momentum of the sled. So this is going to be the same exact equation. I'm just going to skip ahead here. It's going to be \( m_1 (v_{\text{final}} - v_{\text{initial}}) \). So \( m_1 \) here is going to be 70, not the 30, but now we're going to use the final velocity, which is again 7. What's the initial velocity of the sled? Remember the sled was actually moving already at 10 meters per second, that's the initial. So it turns out what happens is you're going to get negative 210 kilogram meters per second. So if you take a look at these two numbers here, they're the same but they're opposites and these two things are related. Basically, what we've had here is a situation where we've had momentum conservation, but one object has gained momentum, and that means that the other one has to lose the same amount. For momentum to be conserved, if one object gains momentum, the other one has to lose the same amount, and the opposite's true. If one object loses momentum, the other one has to gain the same amount. There's always basically a transfer or an exchange of momentum. The sled has to do some work in accelerating the box to the final speed of 7 meters per second, and so the sled loses some speed, the box gains that speed. Alright? So that's it for this one, guys. Let me know if you have any questions.
- 0. Math Review31m
- 1. Intro to Physics Units1h 23m
- 2. 1D Motion / Kinematics3h 56m
- Vectors, Scalars, & Displacement13m
- Average Velocity32m
- Intro to Acceleration7m
- Position-Time Graphs & Velocity26m
- Conceptual Problems with Position-Time Graphs22m
- Velocity-Time Graphs & Acceleration5m
- Calculating Displacement from Velocity-Time Graphs15m
- Conceptual Problems with Velocity-Time Graphs10m
- Calculating Change in Velocity from Acceleration-Time Graphs10m
- Graphing Position, Velocity, and Acceleration Graphs11m
- Kinematics Equations37m
- Vertical Motion and Free Fall19m
- Catch/Overtake Problems23m
- 3. Vectors2h 43m
- Review of Vectors vs. Scalars1m
- Introduction to Vectors7m
- Adding Vectors Graphically22m
- Vector Composition & Decomposition11m
- Adding Vectors by Components13m
- Trig Review24m
- Unit Vectors15m
- Introduction to Dot Product (Scalar Product)12m
- Calculating Dot Product Using Components12m
- Intro to Cross Product (Vector Product)23m
- Calculating Cross Product Using Components17m
- 4. 2D Kinematics1h 42m
- 5. Projectile Motion3h 6m
- 6. Intro to Forces (Dynamics)3h 22m
- 7. Friction, Inclines, Systems2h 44m
- 8. Centripetal Forces & Gravitation7h 26m
- Uniform Circular Motion7m
- Period and Frequency in Uniform Circular Motion20m
- Centripetal Forces15m
- Vertical Centripetal Forces10m
- Flat Curves9m
- Banked Curves10m
- Newton's Law of Gravity30m
- Gravitational Forces in 2D25m
- Acceleration Due to Gravity13m
- Satellite Motion: Intro5m
- Satellite Motion: Speed & Period35m
- Geosynchronous Orbits15m
- Overview of Kepler's Laws5m
- Kepler's First Law11m
- Kepler's Third Law16m
- Kepler's Third Law for Elliptical Orbits15m
- Gravitational Potential Energy21m
- Gravitational Potential Energy for Systems of Masses17m
- Escape Velocity21m
- Energy of Circular Orbits23m
- Energy of Elliptical Orbits36m
- Black Holes16m
- Gravitational Force Inside the Earth13m
- Mass Distribution with Calculus45m
- 9. Work & Energy1h 59m
- 10. Conservation of Energy2h 51m
- Intro to Energy Types3m
- Gravitational Potential Energy10m
- Intro to Conservation of Energy29m
- Energy with Non-Conservative Forces20m
- Springs & Elastic Potential Energy19m
- Solving Projectile Motion Using Energy13m
- Motion Along Curved Paths4m
- Rollercoaster Problems13m
- Pendulum Problems13m
- Energy in Connected Objects (Systems)24m
- Force & Potential Energy18m
- 11. Momentum & Impulse3h 40m
- Intro to Momentum11m
- Intro to Impulse14m
- Impulse with Variable Forces12m
- Intro to Conservation of Momentum17m
- Push-Away Problems19m
- Types of Collisions4m
- Completely Inelastic Collisions28m
- Adding Mass to a Moving System8m
- Collisions & Motion (Momentum & Energy)26m
- Ballistic Pendulum14m
- Collisions with Springs13m
- Elastic Collisions24m
- How to Identify the Type of Collision9m
- Intro to Center of Mass15m
- 12. Rotational Kinematics2h 59m
- 13. Rotational Inertia & Energy7h 4m
- More Conservation of Energy Problems54m
- Conservation of Energy in Rolling Motion45m
- Parallel Axis Theorem13m
- Intro to Moment of Inertia28m
- Moment of Inertia via Integration18m
- Moment of Inertia of Systems23m
- Moment of Inertia & Mass Distribution10m
- Intro to Rotational Kinetic Energy16m
- Energy of Rolling Motion18m
- Types of Motion & Energy24m
- Conservation of Energy with Rotation35m
- Torque with Kinematic Equations56m
- Rotational Dynamics with Two Motions50m
- Rotational Dynamics of Rolling Motion27m
- 14. Torque & Rotational Dynamics2h 5m
- 15. Rotational Equilibrium3h 39m
- 16. Angular Momentum3h 6m
- Opening/Closing Arms on Rotating Stool18m
- Conservation of Angular Momentum46m
- Angular Momentum & Newton's Second Law10m
- Intro to Angular Collisions15m
- Jumping Into/Out of Moving Disc23m
- Spinning on String of Variable Length20m
- Angular Collisions with Linear Motion8m
- Intro to Angular Momentum15m
- Angular Momentum of a Point Mass21m
- Angular Momentum of Objects in Linear Motion7m
- 17. Periodic Motion2h 9m
- 18. Waves & Sound3h 40m
- Intro to Waves11m
- Velocity of Transverse Waves21m
- Velocity of Longitudinal Waves11m
- Wave Functions31m
- Phase Constant14m
- Average Power of Waves on Strings10m
- Wave Intensity19m
- Sound Intensity13m
- Wave Interference8m
- Superposition of Wave Functions3m
- Standing Waves30m
- Standing Wave Functions14m
- Standing Sound Waves12m
- Beats8m
- The Doppler Effect7m
- 19. Fluid Mechanics2h 27m
- 20. Heat and Temperature3h 7m
- Temperature16m
- Linear Thermal Expansion14m
- Volume Thermal Expansion14m
- Moles and Avogadro's Number14m
- Specific Heat & Temperature Changes12m
- Latent Heat & Phase Changes16m
- Intro to Calorimetry21m
- Calorimetry with Temperature and Phase Changes15m
- Advanced Calorimetry: Equilibrium Temperature with Phase Changes9m
- Phase Diagrams, Triple Points and Critical Points6m
- Heat Transfer44m
- 21. Kinetic Theory of Ideal Gases1h 50m
- 22. The First Law of Thermodynamics1h 26m
- 23. The Second Law of Thermodynamics3h 11m
- 24. Electric Force & Field; Gauss' Law3h 42m
- 25. Electric Potential1h 51m
- 26. Capacitors & Dielectrics2h 2m
- 27. Resistors & DC Circuits3h 8m
- 28. Magnetic Fields and Forces2h 23m
- 29. Sources of Magnetic Field2h 30m
- Magnetic Field Produced by Moving Charges10m
- Magnetic Field Produced by Straight Currents27m
- Magnetic Force Between Parallel Currents12m
- Magnetic Force Between Two Moving Charges9m
- Magnetic Field Produced by Loops and Solenoids42m
- Toroidal Solenoids aka Toroids12m
- Biot-Savart Law (Calculus)18m
- Ampere's Law (Calculus)17m
- 30. Induction and Inductance3h 37m
- 31. Alternating Current2h 37m
- Alternating Voltages and Currents18m
- RMS Current and Voltage9m
- Phasors20m
- Resistors in AC Circuits9m
- Phasors for Resistors7m
- Capacitors in AC Circuits16m
- Phasors for Capacitors8m
- Inductors in AC Circuits13m
- Phasors for Inductors7m
- Impedance in AC Circuits18m
- Series LRC Circuits11m
- Resonance in Series LRC Circuits10m
- Power in AC Circuits5m
- 32. Electromagnetic Waves2h 14m
- 33. Geometric Optics2h 57m
- 34. Wave Optics1h 15m
- 35. Special Relativity2h 10m
Adding Mass to a Moving System - Online Tutor, Practice Problems & Exam Prep
In a system where mass is added to a moving object, such as a sled with a box dropped onto it, momentum conservation is key. The final velocity of the combined system can be calculated using the equation m_1 × v_1i + m_2 × v_2i = (m+m)vf. The sled's speed decreases as mass increases, demonstrating the principle of momentum transfer, where one object's gain in momentum equals another's loss.
Adding Mass to a Moving System
Video transcript
A 40-kg skater runs parallel to a 3-kg skateboard. Both are moving to the right at 10m/s. The skater jumps on the board, and they move continue moving right (i.e. no change in direction). Calculate the final speed of the system.
Do you want more practice?
More setsHere’s what students ask on this topic:
What is the final velocity of a system when mass is added to a moving object?
The final velocity of a system when mass is added to a moving object can be calculated using the principle of momentum conservation. The equation is:
Here, and are the masses of the objects, and and are their initial velocities. is the final velocity of the combined system. By solving for , you can determine the final velocity after the mass is added.
How does adding mass to a moving system affect its velocity?
Adding mass to a moving system decreases its velocity. This is due to the principle of momentum conservation, which states that the total momentum of a system remains constant if no external forces act on it. The equation for momentum conservation is:
When mass is added, the total mass increases, and to keep the momentum constant, the velocity must decrease proportionally.
What is the principle of momentum conservation in the context of adding mass to a moving system?
The principle of momentum conservation states that the total momentum of a closed system remains constant if no external forces act on it. In the context of adding mass to a moving system, this principle implies that the initial momentum of the system (before adding mass) must equal the final momentum (after adding mass). The equation is:
Here, and are the masses, and and are their initial velocities. is the final velocity of the combined system.
How do you calculate the change in momentum when mass is added to a moving system?
The change in momentum when mass is added to a moving system can be calculated using the formula:
Here, is the mass added, is the final velocity of the system, and is the initial velocity of the added mass. The change in momentum is the difference between the final and initial momentum of the added mass.
Why does the velocity decrease when mass is added to a moving system?
The velocity decreases when mass is added to a moving system due to the principle of momentum conservation. The total momentum of the system must remain constant if no external forces act on it. The equation for momentum conservation is:
When mass is added, the total mass increases. To keep the momentum constant, the velocity must decrease proportionally. This ensures that the product of mass and velocity (momentum) remains unchanged.
Your Physics tutor
- Three identical train cars, coupled together, are rolling east at speed v0. A fourth car traveling east at 2v0...
- A 10-m-long glider with a mass of 680 kg (including the passengers) is gliding horizontally through the air at...
- A 10,000 kg railroad car is rolling at 2.0 m/s when a 4000 kg load of gravel is suddenly dropped in. What is t...
- (I) A 7150-kg railroad car travels alone on a level frictionless track with a constant speed of 15.0 m/s. A 36...