Conservation of Momentum

The law of conservation of momentum states that total momentum doesn't change over time, even if two objects collide. When a property doesn't change over time we say that the property is conserved.

$$m_1v_1 + m_2v_2 = \text{total momentum}$$ Click the simulation below a few times and watch the sum of the total horizontal momentum before and after the collision.

Conservation of momentum means we can set the total momentums at two points in time equal to each other. (as long as there are no outside forces)

derivation of conservation of momentum

First we are going to rewrite force in terms of a change in velocity.

$$F = ma $$ $$a = \frac{\Delta v}{\Delta t}$$ $$F = m \frac{\Delta v}{\Delta t}$$ $$F = m \frac{(v-u)}{\Delta t}$$

When two bodies collide they each experience an equal but opposite force for an equal period of time as explained by Newton's third law.

F 1 F 2 $$ F_1 \Delta t = -F_2 \Delta t $$ $$m_1 \frac{(v_1-u_1)}{\Delta t} \Delta t= -m_2 \frac{(v_2-u_2)}{\Delta t}\Delta t$$ $$m_1 (v_1-u_1) = -m_2 (v_2-u_2)$$ $$m_1 v_1- m_1 u_1 = -m_2 v_2 + m_2 u_2$$ $$ m_1 u_1 + m_2 u_2= m_2 v_2 + m_1 v_1$$

symmetry and conservation laws

Conservation of momentum is a law. It's a pattern we see when we collect data. We didn't have a explanation for conservation laws until 1915 when Emmy Noether published a mathematical proof that conservation can be understood as a consequence of symmetry. So, momentum is conserved because space is symmetrical.

Symmetry is a property that doesn't change after a transformation. If you translate (move) your location in space the total momentum of a system of particles doesn't change. So we say that momentum is conserved.

There are a few different conservation laws in classical physics:

  • Conservation of energy occurs because of time symmetry. The laws of physics work the same at any time.
  • Conservation of momentum occurs because of translational symmetry. The laws of physics work the same anywhere in space.
  • Conservation of angular momentum occurs because of rotational symmetry. The laws of physics work the same at any angle.
  • Conservation of electric charge occurs because of gauge invariance. This is a quantum mechanical principle related to magnitude and phase of a wave function.
  • There are also a few more conservation laws in quantum mechanics: parity, lepton number, baryon number
  • You might have heard of conservation of mass, but mass isn't always conserved. You can destroy or produce mass because mass is a type of energy.

    m m $$ \sum p_i = \sum p_f$$ $$m_1 u_1 + m_2u_2 = m_1v_1 + m_2v_2$$ \(p\) = momentum [kg m/s] vector
    \(u\) = initial velocity [m/s] vector
    \(v\) = final velocity [m/s] vector
    \(m\) = mass [kg]
    Example: A green box and a  white  box collide. The green box has a mass of 2 kg and is moving to the right at 3 m/s. The white box is moving to the left at 1 m/s and has a mass of 10 kg. If the white box has stopped after the collision what is the velocity of the green box?
    solution $$\sum p_{\mathrm{initial}} = \sum p_{\mathrm{final}}$$ $$\text{green + white = green + white}$$ $$m_{1}u_{1}+m_{2}u_{2}=m_{1}v_{1}+m_{2}v_{2}$$ $$(2)(3)+(10)(-1)=(2)v_{1}+(10)(0)$$ $$6-10=(2)v_{1}$$ $$-4=(2)v_{1}$$ $$-2 \mathrm{\tfrac{m}{s}} =v_{1}$$
    Question: When does the total momentum change in this simulation?
    answer

    The total momentum changes when one of the objects collides with the walls.


    Question: Why does the total momentum change? Is this a violation of conservation of momentum?
    answer

    The total momentum is conserved, but we aren't including the walls in our calculations. It can be very difficult to measure the change in velocity for very massive objects, like the ground or a wall.

    green box blue box orange box
    m = 1.60 kg m = 4.90 kg m = 3.60 kg
    u = 3.0 m/s u = 2.0 m/s u = -1.0 m/s
    v = ??? v = 1.18 m/s v = 1.58 m/s
    Example: Three boxes collide. Use the table to find the final velocity of the green box.
    solution $$\sum p_{\mathrm{initial}} = \sum p_{\mathrm{final}}$$ $$ {\color{Lime} \blacksquare} \quad +\quad {\color{Blue} \blacksquare} \quad+\quad {\color{orange} \blacksquare} \quad = \quad {\color{Lime} \blacksquare} \quad+\quad {\color{Blue} \blacksquare} \quad+\quad {\color{orange} \blacksquare}$$ $$m_{1}u_{1} + m_{2}u_{2} + m_{3}u_{3} = m_{1}v_{1}+m_{2}v_{2}+m_{3}v_{3}$$ $$(1.6)(3)+(4.9)(2)+(3.6)(-1)=(1.6)v_{1}+(4.9)(1.18)+(3.6)(1.58)$$ $$11=1.6v_{1}+11.47$$ $$-0.29 \mathrm{\tfrac{m}{s}} = v_{1}$$
    Example: A photon of red light has a momentum of 9.45 × 10-28 kg m/s. How many photons have to collide with a 100 kg spaceship to get it to speed up from rest to 5 m/s? Assume the photons reflect off the ship after they collide.
    solution

    I'll start by solving for the total momentum needed, so I will not use the momentum per red photon yet.

    $$\sum p_{\mathrm{initial}} = \sum p_{\mathrm{final}}$$ $$p_{\mathrm{photons}} + p_\mathrm{{ship}} = p_\mathrm{{photons}} + p_\mathrm{{ship}}$$ $$p + (100)(0) = -p + (100)(5)$$ $$p = -p + 500$$ $$2p = 500$$ $$p = 250 \space \mathrm{ kg \tfrac{m}{s}}$$

    Light with 250 kg m/s of momentum will accelerate the ship to 5 m/s. In order to count the number of red photons that make up the light we need to divide that number by the momentum of one red photon.

    $$n = \frac{250 \space \mathrm{ kg \tfrac{m}{s}}}{9.45 \times 10^{-28} \space \mathrm{ kg \tfrac{m}{s}}} $$ $$n = 2.77 \times 10^{29} \space \mathrm{photons} $$

    Perfectly Inelastic Collisions

    When objects collide and bounce off without any energy loss we say the collision is elastic. We will learn about how to solve those situations at the end of the energy notes.

    When objects collide and stick together we say the collision is perfectly inelastic. In those situations the equations for conservation of momentum simplify a bit.

    $$m_1u_1 + m_2u_2 = m_1v_1+m_2v_2$$ $$m_1u_1 + m_2u_2 = \left(m_1+m_2\right)v$$
    Click to Randomize Problem: Click above to generate a random problem.
    solution

    Objects can also start as one mass and separate, like in an explosion.

    $$\left(m_1+m_2\right)u = m_1v_1 + m_2v_2$$
    Click to Randomize Problem: Click above to generate a random problem.
    solution
    Example: A 100.0 kg goalie throws a 1.1 kg soccer ball while jumping forward at 3.2 m/s. If the ball flies out of the goalie's hands at 10.0 m/s what speed is the goalie?
    solution $$\sum p_{\mathrm{initial}} = \sum p_{\mathrm{final}}$$ $$\text{goalie holding ball = goalie + ball}$$ $$(m_{1}+m_{2})u=m_{1}v_{1}+m_{2}v_{2}$$ $$(100.0+1.1)(3.2)=(100.0)v_{1}+(1.1)(10.0)$$ $$323.52=(100.0)v_{1}+11$$ $$3.13 \, \mathrm{\tfrac{m}{s}} = v_{1}$$

    2-D Conservation of Momentum

    Momentum is a vector. It has a direction and a magnitude. We can solve for the horizontal and vertical components separately just like how we solved 2-D Motion problems. Although in this case there isn't a time variable to link up the vertical and horizontal equations.

    Horizontal: A pink hexagon and a cyan triangle collide. Before the collision the hexagon has a mass of 5.20 kg and is moving to the right at 2 m/s. The cyan triangle is moving to the left at 1 m/s and has a mass of 1.17 kg. If the triangle bounces off the hexagon at 2.72 m/s to the right what is the horizontal velocity of the hexagon? (ignore the vertical information)
    solution $$\sum p_{\mathrm{initial}} = \sum p_{\mathrm{final}}$$ $$\text{hexagon + triangle = hexagon + triangle}$$ $$m_{1}u_{1}+m_{2}u_{2}=m_{1}v_{1}+m_{2}v_{2}$$ $$(5.20)(2)+(1.17)(-1)=(5.20)v_{1}+(1.17)(2.72)$$ $$10.40-1.17=(5.20)v_{1}+3.18$$ $$6.05=(5.20)v_{1}$$ $$1.16 \, \mathrm{\tfrac{m}{s}}= v_{1}$$

    Vertical: Lets take a look at the vertical aspect of the pink hexagon and cyan triangle collision. Before the collision the hexagon has a mass of 5.20 kg and is not moving up or down. The final vertical velocity of the hexagon is 0.23 m/s down. The final vertical velocity of the triangle is 0.67 m/s up. What is the triangle's initial vertical velocity?
    solution $$\sum p_{\mathrm{initial}} = \sum p_{\mathrm{final}}$$ $$\text{hexagon + triangle = hexagon + triangle}$$ $$m_{1}u_{1}+m_{2}u_{2}=m_{1}v_{1}+m_{2}v_{2}$$ $$(5.20)(0)+(1.17)(u_{2})=(5.20)(-0.23)+(1.17)(0.67)$$ $$(1.17)(u_{2})=-0.41$$ $$u_{2}=-0.35 \, \mathrm{\tfrac{m}{s}}$$
    practice problems (19)

    In case you wanted more practice I used AI to make some more problems. The rest of the site I made by hand, but generating endless problems seemed safe. I did find mistakes in the AI generated problems, and there are probably some I didn't find. Let me know if something could be fixed. I also added a practice problem on each page with no solution. That's intentional. Have fun!

    printout.pdf

    Example: On a low-friction track, a 500 g cart moves right at 0.80 m/s while a 250 g cart waits at rest. What is the total momentum of the two-cart system?
    solution $$500\,\textcolor{DeepPink}{\mathrm{g}}\left(\frac{1\,\mathrm{kg}}{1000\,\textcolor{DeepPink}{\mathrm{g}}}\right)$$ $$0.50\,\mathrm{kg}$$ $$250\,\textcolor{DeepPink}{\mathrm{g}}\left(\frac{1\,\mathrm{kg}}{1000\,\textcolor{DeepPink}{\mathrm{g}}}\right)$$ $$0.25\,\mathrm{kg}$$
    $$\sum p = m_1u_1 + m_2u_2$$ $$\sum p = (0.50)(0.80) + (0.25)(0)$$ $$\sum p = 0.40\,\mathrm{kg\tfrac{m}{s}}$$

    After the carts collide, the total momentum will still be 0.40 kg m/s.

    Example: A 4.0 kg cart moves right at 2.0 m/s, and a 2.0 kg cart moves left at 3.0 m/s. What is the total momentum? Let right be positive.
    solution $$\sum p = m_1u_1 + m_2u_2$$ $$\sum p = (4.0)(2.0) + (2.0)(-3.0)$$ $$\sum p = 8.0 - 6.0$$ $$\sum p = 2.0\,\mathrm{kg\tfrac{m}{s}}$$

    The total momentum is 2.0 kg m/s to the right. The two momenta partly cancel because they point in opposite directions.

    Example: A 2.0 kg cart moving right at 3.0 m/s collides with a 1.0 kg cart at rest. After the collision, the 2.0 kg cart moves right at 1.0 m/s. What is the final velocity of the 1.0 kg cart? The collision lasts 0.020 s. What average force does each cart feel?
    solution $$m_1 = 2.0\,\mathrm{kg}$$ $$u_1 = 3.0\,\mathrm{\tfrac{m}{s}}$$ $$v_1 = 1.0\,\mathrm{\tfrac{m}{s}}$$ $$m_2 = 1.0\,\mathrm{kg}$$ $$u_2 = 0$$ $$v_2 = \,?$$
    $$m_1u_1 + m_2u_2 = m_1v_1 + m_2v_2$$ $$(2.0)(3.0) + (1.0)(0) = (2.0)(1.0) + (1.0)v_2$$ $$6.0 = 2.0 + 1.0v_2$$ $$v_2 = 4.0\,\mathrm{\tfrac{m}{s}}$$

    Use the impulse equation from the momentum page for each cart.

    $$\text{1.0 kg cart}$$ $$F\Delta t = mv - mu$$ $$F(0.020) = (1.0)(4.0) - (1.0)(0)$$ $$F = 200\,\mathrm{N}$$
    $$\text{2.0 kg cart}$$ $$F\Delta t = mv - mu$$ $$F(0.020) = (2.0)(1.0) - (2.0)(3.0)$$ $$F = -200\,\mathrm{N}$$

    The forces are equal and opposite, just like Newton's third law says. That's why the total momentum doesn't change.

    Example: At an amusement park, a 180 kg bumper car (including its rider) moving right at 4.0 m/s hits a 120 kg bumper car moving left at 1.0 m/s. After the collision, the 180 kg car moves right at 2.0 m/s. What is the velocity of the 120 kg car?
    solution

    Let right be positive.

    $$m_1u_1 + m_2u_2 = m_1v_1 + m_2v_2$$ $$(180)(4.0) + (120)(-1.0) = (180)(2.0) + (120)v_2$$ $$720 - 120 = 360 + 120v_2$$ $$240 = 120v_2$$ $$v_2 = 2.0\,\mathrm{\tfrac{m}{s}}$$

    The 120 kg car reverses direction and now moves right at 2.0 m/s.

    Example: A 90 kg linebacker running at 5.0 m/s tackles a 75 kg running back who is running straight toward him at 6.0 m/s. They hold on to each other. What is their velocity right after the tackle?
    solution

    Let the linebacker's direction be positive. They stick together, so this is a perfectly inelastic collision.

    $$m_1u_1 + m_2u_2 = (m_1 + m_2)v$$ $$(90)(5.0) + (75)(-6.0) = (90 + 75)v$$ $$450 - 450 = 165v$$ $$0 = 165v$$ $$v = 0$$

    The two players stop dead. They had the same size momentum in opposite directions, so the total momentum was zero before the tackle and stays zero after it.

    Example: A 1.5 kg lump of clay is thrown right at 8.0 m/s. It hits and sticks to a 2.5 kg cart that is rolling left at 2.0 m/s. What is their final velocity?
    solution $$m_1u_1 + m_2u_2 = (m_1 + m_2)v$$ $$(1.5)(8.0) + (2.5)(-2.0) = (1.5 + 2.5)v$$ $$12 - 5.0 = 4.0v$$ $$7.0 = 4.0v$$ $$v = 1.75\,\mathrm{\tfrac{m}{s}}$$

    The clay had more momentum, so the combined object moves right.

    Example: A 30 000 kg railroad car rolling at 2.0 m/s bumps into and couples with a 20 000 kg car rolling in the same direction at 0.50 m/s. How fast do the coupled cars move?
    solution $$m_1u_1 + m_2u_2 = (m_1 + m_2)v$$ $$(30\,000)(2.0) + (20\,000)(0.50) = (30\,000 + 20\,000)v$$ $$60\,000 + 10\,000 = 50\,000v$$ $$70\,000 = 50\,000v$$ $$v = 1.4\,\mathrm{\tfrac{m}{s}}$$

    The answer falls between the two starting speeds, which makes sense for objects that stick together.

    Example: A 0.010 kg bullet is fired into a 2.0 kg wooden block resting on ice. The bullet stays in the block, and the block slides away at 2.5 m/s. How fast was the bullet moving?
    solution $$m_1 = 0.010\,\mathrm{kg}$$ $$u_1 = \,?$$ $$m_2 = 2.0\,\mathrm{kg}$$ $$u_2 = 0$$ $$v = 2.5\,\mathrm{\tfrac{m}{s}}$$
    $$m_1u_1 + m_2u_2 = (m_1 + m_2)v$$ $$(0.010)u_1 + (2.0)(0) = (0.010 + 2.0)(2.5)$$ $$0.010u_1 = 5.03$$ $$u_1 = \frac{5.03}{0.010}$$ $$u_1 = 503\,\mathrm{\tfrac{m}{s}}$$

    This is a real method, called a ballistic pendulum, for measuring bullet speeds. A slow, easy-to-measure block tells you the speed of a very fast bullet.

    Example: Two carts on a track are held together at rest with a compressed spring between them. When the spring is released, the 2.0 kg cart moves right at 3.0 m/s. What is the velocity of the 3.0 kg cart?
    solution

    Both carts start at rest, so the starting momentum is zero.

    $$(m_1 + m_2)u = m_1v_1 + m_2v_2$$ $$(2.0 + 3.0)(0) = (2.0)(3.0) + (3.0)v_2$$ $$0 = 6.0 + 3.0v_2$$ $$-6.0 = 3.0v_2$$ $$v_2 = -2.0\,\mathrm{\tfrac{m}{s}}$$

    The 3.0 kg cart moves left. The heavier cart moves more slowly, so the two momenta still add to zero.

    Example: A 60 kg hockey player gliding at 5.0 m/s grabs onto a teammate who is standing still on the ice. They glide off together. What is their velocity?
    solution

    This cannot be solved from the information given. Conservation of momentum needs the mass of the teammate. The more massive the teammate, the slower they'll glide together.

    $$(60)(5.0) + m_2(0) = (60 + m_2)v$$

    With two unknowns, m₂ and v, one equation isn't enough.

    Example: A 3000 kg spacecraft is coasting at 4000 m/s. Explosive bolts separate it into a 2000 kg capsule and a 1000 kg empty rocket stage. After the separation, the capsule moves forward at 4500 m/s. What is the velocity of the rocket stage?
    solution $$(m_1 + m_2)u = m_1v_1 + m_2v_2$$ $$(2000 + 1000)(4000) = (2000)(4500) + (1000)v_2$$ $$12\,000\,000 = 9\,000\,000 + 1000v_2$$ $$3\,000\,000 = 1000v_2$$ $$v_2 = 3000\,\mathrm{\tfrac{m}{s}}$$

    The stage keeps moving forward, but more slowly. The push from the bolts sped up the capsule and slowed down the stage.

    Example: A 55 kg astronaut is floating at rest 20 m from the space station. To get back, she throws a 2.0 kg wrench directly away from the station at 8.0 m/s. How long does it take her to reach the station?
    solution

    Let the direction of the wrench be positive.

    $$(m_1 + m_2)u = m_1v_1 + m_2v_2$$ $$(55 + 2.0)(0) = (55)v_1 + (2.0)(8.0)$$ $$0 = 55v_1 + 16$$ $$v_1 = \frac{-16}{55}$$ $$v_1 = -0.29\,\mathrm{\tfrac{m}{s}}$$

    She moves toward the station at a constant 0.29 m/s, because there's no friction in space.

    $$v = \frac{\Delta x}{\Delta t}$$ $$0.29 = \frac{20}{\Delta t}$$ $$\Delta t = \frac{20}{0.29}$$ $$\Delta t = 69\,\mathrm{s}$$

    It takes a little over a minute. Throwing something is one of the only ways to change your velocity in space.

    Example: A 70 kg skater standing still on smooth ice catches a 5.0 kg backpack thrown at 6.0 m/s. What is the skater's velocity after the catch?
    solution $$m_1u_1 + m_2u_2 = (m_1 + m_2)v$$ $$(70)(0) + (5.0)(6.0) = (70 + 5.0)v$$ $$30 = 75v$$ $$v = 0.40\,\mathrm{\tfrac{m}{s}}$$

    Catching the backpack pushes the skater in the direction the backpack was moving.

    Example: Three air-track gliders collide. A 2.0 kg glider moves right at 3.0 m/s, a 1.0 kg glider moves left at 4.0 m/s, and a 5.0 kg glider is at rest. After the collision, the 1.0 kg glider moves right at 1.0 m/s and the 5.0 kg glider moves right at 0.50 m/s. What is the final velocity of the 2.0 kg glider?
    solution $$m_1u_1 + m_2u_2 + m_3u_3 = m_1v_1 + m_2v_2 + m_3v_3$$ $$(2.0)(3.0) + (1.0)(-4.0) + (5.0)(0) = (2.0)v_1 + (1.0)(1.0) + (5.0)(0.50)$$ $$2.0 = 2.0v_1 + 3.5$$ $$-1.5 = 2.0v_1$$ $$v_1 = -0.75\,\mathrm{\tfrac{m}{s}}$$

    The 2.0 kg glider bounces back to the left.

    Example: A 0.40 kg air-track glider moving right at 0.50 m/s runs into a 0.20 kg glider that is moving right more slowly. After the collision, the 0.40 kg glider moves right at 0.30 m/s and the 0.20 kg glider moves right at 0.60 m/s. How fast was the 0.20 kg glider moving before the collision?
    solution $$m_1u_1 + m_2u_2 = m_1v_1 + m_2v_2$$ $$(0.40)(0.50) + (0.20)u_2 = (0.40)(0.30) + (0.20)(0.60)$$ $$0.20 + 0.20u_2 = 0.12 + 0.12$$ $$0.20u_2 = 0.04$$ $$u_2 = 0.20\,\mathrm{\tfrac{m}{s}}$$

    This makes sense. The front glider had to be moving slower than 0.50 m/s, or the back glider would never have caught up.

    Example: On a pool table, a 0.17 kg cue ball moving east at 2.0 m/s hits a 0.17 kg ball at rest. After the collision, the cue ball moves 1.0 m/s east and 0.87 m/s north. What are the east and north velocity components of the other ball?
    solution

    Solve the east-west and north-south directions separately. Let east and north be positive.

    $$\text{east-west}$$ $$m_1u_1 + m_2u_2 = m_1v_1 + m_2v_2$$ $$(0.17)(2.0) + (0.17)(0) = (0.17)(1.0) + (0.17)v_2$$ $$0.34 = 0.17 + 0.17v_2$$ $$v_2 = 1.0\,\mathrm{\tfrac{m}{s}}$$
    $$\text{north-south}$$ $$m_1u_1 + m_2u_2 = m_1v_1 + m_2v_2$$ $$(0.17)(0) + (0.17)(0) = (0.17)(0.87) + (0.17)v_2$$ $$0 = 0.148 + 0.17v_2$$ $$v_2 = -0.87\,\mathrm{\tfrac{m}{s}}$$

    The other ball moves 1.0 m/s east and 0.87 m/s south. The north-south momentum started at zero, so the two balls have to move in opposite north-south directions. Using the Pythagorean theorem, the ball's speed is 1.3 m/s.

    Example: A 200 g toy car moving right at 1.2 m/s sticks to a 300 g toy truck moving left at 0.30 m/s. What is their final velocity?
    solution $$200\,\textcolor{DeepPink}{\mathrm{g}}\left(\frac{1\,\mathrm{kg}}{1000\,\textcolor{DeepPink}{\mathrm{g}}}\right)$$ $$0.20\,\mathrm{kg}$$ $$300\,\textcolor{DeepPink}{\mathrm{g}}\left(\frac{1\,\mathrm{kg}}{1000\,\textcolor{DeepPink}{\mathrm{g}}}\right)$$ $$0.30\,\mathrm{kg}$$
    $$m_1u_1 + m_2u_2 = (m_1 + m_2)v$$ $$(0.20)(1.2) + (0.30)(-0.30) = (0.20 + 0.30)v$$ $$0.24 - 0.09 = 0.50v$$ $$0.15 = 0.50v$$ $$v = 0.30\,\mathrm{\tfrac{m}{s}}$$

    The pair moves right, the direction of the car's larger momentum.

    Example: In a simplified crash model, a 900 kg compact car moving at 36 km/h rear-ends a 1500 kg van moving in the same direction at 18 km/h. The two vehicles lock together. Ignore braking during the short collision. What is their speed right after the collision?
    solution $$36\,\mathrm{\tfrac{\textcolor{DeepPink}{km}}{\textcolor{DodgerBlue}{h}}}\left(\frac{1000\,\mathrm{m}}{1\,\textcolor{DeepPink}{\mathrm{km}}}\right)\left(\frac{1\,\textcolor{DodgerBlue}{\mathrm{h}}}{3600\,\mathrm{s}}\right)$$ $$10\,\mathrm{\tfrac{m}{s}}$$ $$18\,\mathrm{\tfrac{\textcolor{DeepPink}{km}}{\textcolor{DodgerBlue}{h}}}\left(\frac{1000\,\mathrm{m}}{1\,\textcolor{DeepPink}{\mathrm{km}}}\right)\left(\frac{1\,\textcolor{DodgerBlue}{\mathrm{h}}}{3600\,\mathrm{s}}\right)$$ $$5.0\,\mathrm{\tfrac{m}{s}}$$
    $$m_1u_1 + m_2u_2 = (m_1 + m_2)v$$ $$(900)(10) + (1500)(5.0) = (900 + 1500)v$$ $$9000 + 7500 = 2400v$$ $$16\,500 = 2400v$$ $$v = 6.9\,\mathrm{\tfrac{m}{s}}$$

    That's about 25 km/h. The van speeds up and the car slows down.

    Question: When you jump, your momentum changes from zero to a large upward momentum. Does that break the law of conservation of momentum?
    answer

    No. Your legs push down on the Earth, and the Earth pushes up on you. The Earth gets exactly as much downward momentum as you get upward momentum, so the total stays zero.

    The Earth's mass is so huge that its change in velocity is far too small to notice. This is the same reason the total momentum seemed to change when the objects hit the walls in the simulation on this page.