Physics Chapter 9: Linear Momentum
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A particle of mass m moves with momentum of magnitude p. (a) Show that the kinetic energy of the particle is K = p²/2m.

The kinetic energy of the particle is given by K = 1/2mv², where v is the speed of the particle. We know that the momentum of the particle is given by p = mv. We can rearrange this to find that v = p/m. Substituting this expression for v in the kinetic energy equation, we get K = 1/2m(p/m)², which simplifies to K = p²/2m. This is the desired result.

A particle of mass m moves with momentum of magnitude p. (b) Express the magnitude of the particle's momentum in terms of its kinetic energy and mass.

Solving the equation in part (a) for the momentum, we get p = √[2mK]. This expresses the magnitude of the particle's momentum in terms of its kinetic energy and mass.

A 3.00-kg particle has a velocity of (3.00i – 4.00j) m/s. (a) Find its x and y components of momentum.

The momentum is given by p = mv. Using the given velocity, the x-component of momentum is px = (3.00 kg)(3.00 m/s) = 9.00 kg·m/s. The y-component of momentum is py = (3.00 kg)(-4.00 m/s) = -12.0 kg·m/s. The negative sign indicates that the y-component of momentum is in the negative y direction.

A 3.00-kg particle has a velocity of (3.00i – 4.00j) m/s. (b) Find the magnitude and direction of its momentum.

<p>The magnitude of the momentum is given by <em>p = √(px² + py²) = √[(9.00 kg·m/s)² + (-12.0 kg·m/s)²] = 15.0 kg·m/s</em>. The direction of the momentum is given the angle <em>θ = tan⁻¹ (py/px) = tan⁻¹ (-12.0 kg·m/s / 9.00 kg·m/s) = -53.1°</em>. The momentum is directed 53.1° to the right of the negative y-axis (or 36.9° below the positive x-axis).</p> Signup and view all the answers

A baseball approaches home plate at a speed of 45.0 m/s, moving horizontally just before being hit by a bat. The batter hits a pop-up such that after hitting the bat, the baseball is moving at 55.0 m/s straight up. The ball has a mass of 145 g and is in contact with the bat for 2.00 ms. What is the average vector force the ball exerts on the bat during their interaction?

<p>The average vector force exerted by the ball on the bat is <em>F = Δp/Δt</em>. We can calculate the change in momentum as <em>Δp = mvf - mvi</em>. The initial velocity in the x-direction is 45.0 m/s, and the final velocity in the y-direction is 55.0 m/s. Since the ball is in contact with the bat for 2.00 ms which is equal to 0.002 s, the average force exerted by the ball on the bat is <em>F = (0.145 kg)(55.0 j m/s - 45.0 i m/s)/0.002 s = 7 250 i N - 4 037.5 j N</em>.</p> Signup and view all the answers

A 65.0-kg boy and his 40.0-kg sister, both wearing roller blades, face each other at rest. The girl pushes the boy hard, sending him backward with a velocity of 2.90 m/s toward the west. Ignore friction. (a) Describe the subsequent motion of the girl.

<p>Since the total momentum is zero, there will be an equal but opposite momentum for the girl. So, the girl will move eastward at the velocity of 2.90 m/s, as <em>m1v1 = m2v2</em>.</p> Signup and view all the answers

A 65.0-kg boy and his 40.0-kg sister, both wearing roller blades, face each other at rest. The girl pushes the boy hard, sending him backward with a velocity of 2.90 m/s toward the west. Ignore friction. (b) How much potential energy in the girl's body is converted into mechanical energy of the boy-girl system?

<p>The potential energy converted to mechanical energy is given by <em>1/2(m1v1² + m2v2²) = 1/2(65.0 kg)(2.90 m/s)² + 1/2(40.0 kg)(2.90 m/s)² = 320 J</em>.</p> Signup and view all the answers

A 65.0-kg boy and his 40.0-kg sister, both wearing roller blades, face each other at rest. The girl pushes the boy hard, sending him backward with a velocity of 2.90 m/s toward the west. Ignore friction. (d) There are large forces acting?

<p>True</p> Signup and view all the answers

A 65.0-kg boy and his 40.0-kg sister, both wearing roller blades, face each other at rest. The girl pushes the boy hard, sending him backward with a velocity of 2.90 m/s toward the west. Ignore friction. (e) There is no motion beforehand and plenty of motion afterward.

<p>True</p> Signup and view all the answers

Two blocks of masses m and 3m are placed on a frictionless, horizontal surface. A light spring is attached to the more massive block, and the blocks are pushed together with the spring between them (Fig. P9.5). A cord initially holding the blocks together is burned; after that happens, the block of mass 3m moves to the right with a speed of 2.00 m/s. (a) What is the velocity of the block of mass m?

<p>The initial momentum of the system was zero. This is because both blocks were at rest, and the initial momentum of the system is given by <em>m1vi1 + m2vi2</em>. Since the initial momentum of the system is zero, and the momentum is conserved, the final momentum of the system is also zero. This means <em>m1vf1 + m2vf2 = 0</em>. The final momentum of the block with mass <em>3m</em> is <em>3m</em> * 2.00 m/s*. Therefore, the momentum of the block with mass <em>m</em> is <em>m</em> * (-6.00 m/s)* and the final velocity of the block with mass <em>m</em> is <em>- 6.00 m/s</em>. The negative sign indicates that the block of mass <em>m</em> is moving to the left.</p> Signup and view all the answers

Two blocks of masses m and 3m are placed on a frictionless, horizontal surface. A light spring is attached to the more massive block, and the blocks are pushed together with the spring between them (Fig. P9.5). A cord initially holding the blocks together is burned; after that happens, the block of mass 3m moves to the right with a speed of 2.00 m/s. (b) Find the system's original elastic potential energy, taking m = 0.350 kg.

<p>The original elastic potential energy stored in the spring is equal to the sum of the kinetic energies of the two blocks after the blocks are released. This is because after the cord is burned, the energy stored in the spring is released, and the kinetic energies of the two blocks are obtained. So, the original elastic potential energy is given by <em>KEtotal = 1/2m1v1² + 1/2m2v2² = 1/2(0.350 kg)(-6.00 m/s)² + 1/2(3</em>0.350 kg)(2.00 m/s)² = 7.35 J*.</p> Signup and view all the answers

Two blocks of masses m and 3m are placed on a frictionless, horizontal surface. A light spring is attached to the more massive block, and the blocks are pushed together with the spring between them (Fig. P9.5). A cord initially holding the blocks together is burned; after that happens, the block of mass 3m moves to the right with a speed of 2.00 m/s. (c) Is the original energy in the spring or in the cord?

<p>True</p> Signup and view all the answers

Two blocks of masses m and 3m are placed on a frictionless, horizontal surface. A light spring is attached to the more massive block, and the blocks are pushed together with the spring between them (Fig. P9.5). A cord initially holding the blocks together is burned; after that happens, the block of mass 3m moves to the right with a speed of 2.00 m/s. (d) Explain your answer to part (c).

<p>True</p> Signup and view all the answers

Two blocks of masses m and 3m are placed on a frictionless, horizontal surface. A light spring is attached to the more massive block, and the blocks are pushed together with the spring between them (Fig. P9.5). A cord initially holding the blocks together is burned; after that happens, the block of mass 3m moves to the right with a speed of 2.00 m/s. (e) Is the momentum of the system conserved in the bursting-apart process?

<p>True</p> Signup and view all the answers

Two blocks of masses m and 3m are placed on a frictionless, horizontal surface. A light spring is attached to the more massive block, and the blocks are pushed together with the spring between them (Fig. P9.5). A cord initially holding the blocks together is burned; after that happens, the block of mass 3m moves to the right with a speed of 2.00 m/s. (f) There are large forces acting?

<p>True</p> Signup and view all the answers

Two blocks of masses m and 3m are placed on a frictionless, horizontal surface. A light spring is attached to the more massive block, and the blocks are pushed together with the spring between them (Fig. P9.5). A cord initially holding the blocks together is burned; after that happens, the block of mass 3m moves to the right with a speed of 2.00 m/s. (g) There is no motion beforehand and plenty of motion afterward?

<p>True</p> Signup and view all the answers

When you jump straight up as high as you can, what is the order of magnitude of the maximum recoil speed that you give to the Earth? Model the Earth as a perfectly solid object.

<p>The recoil speed is the speed at which the Earth would move in response to you jumping. It is given by <em>vEarth = (mYou/mEarth)vYou</em>. Since the mass of the Earth is very large compared to your mass, the recoil speed is very small and can be considered negligible.</p> Signup and view all the answers

Match the following programming languages with their primary usage:

<p>Python = General-purpose programming JavaScript = Client-side scripting for web applications SQL = Database queries CSS = Styling web pages</p> Signup and view all the answers

A glider of mass m is free to slide along a horizontal air track. It is pushed against a launcher at one end of the track. Model the launcher as a light spring of force constant k compressed by a distance x. The glider is released from rest. (a) Show that the glider attains a speed of v = x(k/m)1/2.

<p>The potential energy stored in the spring is given by <em>U = 1/2kx²</em>. The potential energy is converted into kinetic energy of the glider as the glider is released. Hence, <em>1/2mv² = 1/2kx²</em>. Solving this equation for the speed of the glider, we get <em>v = x(k/m)1/2</em>.</p> Signup and view all the answers

A glider of mass m is free to slide along a horizontal air track. It is pushed against a launcher at one end of the track. Model the launcher as a light spring of force constant k compressed by a distance x. The glider is released from rest. (b) Show that the magnitude of the impulse imparted to the glider is given by the expression I = x(km)1/2.

<p>The impulse imparted to the glider is given by <em>I = Δp = mv - 0</em> or, <em>I = mv</em>. Substituting the velocity of the glider from part (a) into the impulse equation, we get <em>I = mx(k/m)¹/² = x(km)¹/²</em>.</p> Signup and view all the answers

A glider of mass m is free to slide along a horizontal air track. It is pushed against a launcher at one end of the track. Model the launcher as a light spring of force constant k compressed by a distance x. The glider is released from rest. (c) Is more work done on a cart with a large or a small mass?

<p>True</p> Signup and view all the answers

You and your brother argue often about how to safely secure a toddler in a moving car. You insist that special toddler seats are critical in improving the chances of a toddler surviving a crash. Your brother claims that, as long as his wife is buckled in next to him with a seat belt while he drives, she can hold onto their toddler on her lap in a crash. You decide to perform a calculation to try to convince your brother. Consider a hypothetical collision in which the 12-kg toddler and his parents are riding in a car traveling at 60 mi/h relative to the ground. The car strikes a wall, tree, or another car, and is brought to rest in 0.10 s. You wish to demonstrate to your brother the magnitude of the force necessary for his wife to hold onto their child during the collision.

<p>The force required to hold the child is given by <em>F = Δp/Δt = mΔv/Δt</em>. Using the given values, we get <em>F = (12kg)(60mi/h * 0.447 m/s/1mi/h)/0.1s = 3 200 N</em>. The force needed to hold the child is very high, and it could be impossible for a person to exert such a strong force. It clearly shows that it is not safe to hold a child on their lap, and using a car seat for the child is highly recommended.</p> Signup and view all the answers

The front 1.20 m of a 1 400-kg car is designed as a "crumple zone" that collapses to absorb the shock of a collision. If a car traveling 25.0 m/s stops uniformly in 1.20 m, (a) how long does the collision last?

<p>The time it takes for the car to stop is given by <em>t = Δv/a</em>. Using the initial velocity and distance covered, we get <em>t = 25.0 m/s / (25.0 m/s)²/ (2 * 1.20 m) = 0.192 s</em>. The collision lasts for 0.192 seconds.</p> Signup and view all the answers

The front 1.20 m of a 1 400-kg car is designed as a "crumple zone" that collapses to absorb the shock of a collision. If a car traveling 25.0 m/s stops uniformly in 1.20 m, (b) what is the magnitude of the average force on the car?

<p>The average force exerted on the car is given by <em>F = mΔv/Δt = (1 400 kg)(25.0 m/s)/0.192 s = 1.82 × 10⁵ N</em>. The average force exerted on the car is 1.82 × 10⁵ N.</p> Signup and view all the answers

The front 1.20 m of a 1 400-kg car is designed as a "crumple zone" that collapses to absorb the shock of a collision. If a car traveling 25.0 m/s stops uniformly in 1.20 m, (c) what is the magnitude of the acceleration of the car? Express the acceleration as a multiple of the acceleration due to gravity.

<p>The acceleration of the car is given by <em>a = Δv/Δt = (25.0 m/s)/0.192s = 130 m/s²</em>. The magnitude of the acceleration is about 13 times the acceleration due to gravity, which is 9.8 m/s².</p> Signup and view all the answers

The magnitude of the net force exerted in the x direction on a 2.50-kg particle varies in time as shown in Figure P9.10 (page 244). Find (a) the impulse of the force over the 5.00-s time interval.

<p>The impulse of the force is given by <em>I = Δp = FΔt</em>. The impulse is the change in momentum. The impulse is given by the area under the force versus time graph. Finding the area of the triangular shape from <em>t = 0</em> to <em>t = 3</em> is <em>1/2(3 sec)(3 N) = 4.5 N·s</em>. The area of the rectangular is <em>1(3 N) = 3 N·s</em>. So, the total impulse is given by <em>(4.5 N·s + 3 N·s) = 7.5 N·s</em>.</p> Signup and view all the answers

The magnitude of the net force exerted in the x direction on a 2.50-kg particle varies in time as shown in Figure P9.10 (page 244). Find (b) the final velocity the particle attains if it is originally at rest.

<p>The final velocity of the particle is given by <em>vf = vi + Δv</em>. The final velocity is given by the change in the momentum and the initial velocity. We can calculate the change in velocity from the impulse as <em>Δv = I/m = 7.5 N·s / 2.50 kg = 3.00 m/s</em>. Therefore, the final velocity of the particle is <em>vf = 0 + 3.00 m/s = 3.00 m/s</em>.</p> Signup and view all the answers

The magnitude of the net force exerted in the x direction on a 2.50-kg particle varies in time as shown in Figure P9.10 (page 244). Find (c) its final velocity if its original velocity is -2.001 m/s.

<p>The final velocity of the particle is given by <em>vf = vi + Δv</em>. The impulse is independent of the initial velocity, so the change in velocity is still <em>Δv = 3.00 m/s</em>. The final velocity is, therefore, <em>vf = -2.00 m/s + 3.00 m/s = 1.00 m/s</em>.</p> Signup and view all the answers

The magnitude of the net force exerted in the x direction on a 2.50-kg particle varies in time as shown in Figure P9.10 (page 244). Find (d) the average force exerted on the particle for the time interval between 0 and 5.00 s.

<p>The average force exerted on the particle is given by <em>F = I/Δt</em>. The average force is the impulse of the force over the time interval. The average force is <em>F = 7.5 N·s / 5.00 s = 1.5 N</em>.</p> Signup and view all the answers

Water falls without splashing at a rate of 0.250 L/s from a height of 2.60 m into a bucket of mass 0.750 kg on a scale. If the bucket is originally empty, what does the scale read in newtons 3.00 s after water starts to accumulate in it?

<p>The scale reads the weight of the bucket plus the weight of the water in the bucket. The mass of the water in the bucket is given by <em>mwater = (0.250 L/s)(1 kg/L)(3 sec) = 0.75 kg</em>. The weight of the water is given by <em>Fwater = (0.75 kg)(9.8 m/s²) = 7.35 N</em>. The scale reads <em>7.35 N + (0.750 kg)(9.8 m/s²) = 14.7 N</em>.</p> Signup and view all the answers

A 1 200-kg car traveling initially at v₁ = 25.0 m/s in an easterly direction crashes into the back of a 9 000-kg truck moving in the same direction at v₁₁ = 20.0 m/s (Fig. P9.12). The velocity of the car immediately after the collision is ucf = 18.0 m/s to the east. (a) What is the velocity of the truck immediately after the collision?

<p>The initial momentum of the system is <em>m1vi1 + m2vi2 = (1 200 kg)(25.0 m/s) + (9 000 kg)(20.0 m/s) = 2.16 × 10⁵ kg·m/s</em>. Since the momentum is conserved, this must be equal to the final momentum <em>m1vf1 + m2vf2</em>. Solving for <em>vf2</em>, we get <em>vf2 = (2.16 × 10⁵ kg·m/s - (1 200 kg)(18.0 m/s)) / 9 000 kg = 20.8 m/s</em>. Therefore, the final velocity of the truck is 20.8 m/s.</p> Signup and view all the answers

A 1 200-kg car traveling initially at v₁ = 25.0 m/s in an easterly direction crashes into the back of a 9 000-kg truck moving in the same direction at v₁₁ = 20.0 m/s (Fig. P9.12). The velocity of the car immediately after the collision is ucf = 18.0 m/s to the east. (b) What is the change in mechanical energy of the car-truck system in the collision?

<p>The initial kinetic energy of the system is <em>1/2m1v1² + 1/2m2v2² = 1/2(1 200 kg)( 25.0 m/s)² + 1/2(9 000 kg)(20 m/s)² = 2.43 × 10⁶ J</em>. The final kinetic energy of the system is <em>1/2m1vf1² + 1/2m2vf2² = 1/2(1 200 kg)(18 m/s)² + 1/2(9 000 kg)(20.8 m/s)² = 2.23 × 10⁶ J</em>. The change in the mechanical energy is <em>ΔKE = (2.23 × 10⁶ J - 2.43 × 10⁶ J) = -2.0 × 10⁵ J</em>. The mechanical energy of the system is not conserved during the collision.</p> Signup and view all the answers

A 1 200-kg car traveling initially at v₁ = 25.0 m/s in an easterly direction crashes into the back of a 9 000-kg truck moving in the same direction at v₁₁ = 20.0 m/s (Fig. P9.12). The velocity of the car immediately after the collision is ucf = 18.0 m/s to the east. (c) Account for this change in mechanical energy.

<p>The loss in the mechanical energy is converted into other forms of energy, such as sound, heat, and deformation of the car and the truck. The collision is not perfectly elastic, so the mechanical energy is not conserved. The initial kinetic energy is converted into other forms of energy and the final kinetic energy is less than the initial kinetic energy. The initial and final momentum of the system is conserved because there are no external forces acting on the car and truck system.</p> Signup and view all the answers

A railroad car of mass 2.50 × 10⁴ kg is moving with a speed of 4.00 m/s. It collides and couples with three other coupled railroad cars, each of the same mass as the single car and moving in the same direction with an initial speed of 2.00 m/s. (a) What is the speed of the four cars after the collision?

<p>The initial momentum of the system is <em>m1vi1 + m2vi2 + m3vi3 + m3vi4 = (2.50 × 10⁴ kg)(4.00 m/s) + (2.50 × 10⁴ kg)(2.00 m/s) + (2.50 × 10⁴ kg)(2.00 m/s) + (2.50 × 10⁴ kg)(2.00 m/s) = 2.50 × 10⁵ kg·m/s</em>. The final momentum of the system is <em>m1vf1 + m2vf2 + m3vf3 + m4vf4 = (2.50 × 10⁴ kg + 2.50 × 10⁴ kg + 2.50 × 10⁴ kg + 2.50 × 10⁴ kg)vf = 10⁵ kgvf</em>. Since the momentum is conserved <em>2.50 × 10⁵ kg·m/s = 10⁵ kgvf</em>. Therefore, the final velocity of the four cars is <em>vf = 2.50 m/s</em>.</p> Signup and view all the answers

A railroad car of mass 2.50 × 10⁴ kg is moving with a speed of 4.00 m/s. It collides and couples with three other coupled railroad cars, each of the same mass as the single car and moving in the same direction with an initial speed of 2.00 m/s. (b) What is the decrease in mechanical energy in the collision?

<p>The initial kinetic energy of the system is <em>KEi = 1/2m1v1² + 1/2(m2v2² + m3v3² + m4v4²) = 1/2(2.50 × 10⁴ kg)(4.00 m/s)² + 1/2((2.50 × 10⁴ kg)(2.00 m/s)² + (2.50 × 10⁴ kg)(2.00 m/s)² + (2.50 × 10⁴ kg)(2.00 m/s)²) = 3.75 × 10⁵ J</em>. The final kinetic energy of the system is <em>KEf = 1/2(2.50 × 10⁴ kg + 2.50 × 10⁴ kg + 2.50 × 10⁴ kg + 2.50 × 10⁴ kg)(2.50 m/s)² = 1.56 × 10⁵ J</em>. The decrease in mechanical energy is given by *ΔKE = (KEi - KEf) = 3.75 × 10⁵ J - 1.56 × 10⁵ J = 2.</p> Signup and view all the answers

A 65.0-kg boy and his 40.0-kg sister, both wearing roller blades, face each other at rest. The girl pushes the boy hard, sending him backward with velocity 2.90 m/s toward the west. Ignore friction. Describe the subsequent motion of the girl.

<p>Since the system is isolated and momentum is conserved, the girl will move in the opposite direction with a velocity that ensures the total momentum of the boy-girl system remains zero. The velocity of the girl can be calculated using the conservation of momentum equation: <em>m_b</em> <em>v_b</em> + * m_g* <em>v_g</em> = 0, where <em>m_b</em> is the boy's mass, <em>v_b</em> is the boy's velocity, <em>m_g</em> is the girl's mass, and <em>v_g</em> is the girl's velocity. Solving for <em>v_g</em> gives <em>v_g = - (m_b</em> <em>v_b</em>)/ <em>m_g</em> = - (65.0 kg * 2.90 m/s) / 40.0 kg = - 4.49 m/s*. The girl will move eastward with a velocity of 4.49 m/s.</p> Signup and view all the answers

How much potential energy in the girl's body is converted into mechanical energy of the boy-girl system?

<p>True</p> Signup and view all the answers

Is the momentum of the boy-girl system conserved in the pushing-apart process?

<p>True</p> Signup and view all the answers

There are large forces acting, regarding the pushing-apart process?

<p>True</p> Signup and view all the answers

There is no motion beforehand and plenty of motion afterward, regarding the pushing-apart process?

<p>True</p> Signup and view all the answers

Is the original energy in the spring or in the cord?

<p>True</p> Signup and view all the answers

Is the momentum of the system conserved in the bursting-apart process?

<p>True</p> Signup and view all the answers

A glider of mass m is free to slide along a horizontal air track. It is pushed against a launcher at one end of the track. Model the launcher as a light spring of force constant k compressed by a distance x. The glider is released from rest. Show that the glider attains a speed of v = x(k/m)1/2.

<p>The potential energy stored in the spring is <em>U = (1/2)kx²</em>. When the spring is released, this potential energy is converted into kinetic energy of the glider, <em>(1/2)mv²</em>. Setting these two expressions equal gives <em>(1/2)kx² = (1/2)mv²</em>. Solving for <em>v</em> yields: <em>v = x√(k/m)</em>.</p> Signup and view all the answers

A glider of mass m is free to slide along a horizontal air track. It is pushed against a launcher at one end of the track. Model the launcher as a light spring of force constant k compressed by a distance x. The glider is released from rest. Show that the magnitude of the impulse imparted to the glider is given by the expression I = x(km)1/2.

<p>Impulse is defined as the change in momentum, <em>I = Δp = m(v_f - v_i)</em>. Since the glider starts from rest, <em>v_i = 0</em>. Using the expression for final velocity we derived previously, <em>v_f = x√(k/m)</em>, we can substitute it into the impulse equation giving <em>I = m(x√(k/m)) = x√(km)</em>.</p> Signup and view all the answers

Is more work done on a cart with a large or a small mass?

<p>True</p> Signup and view all the answers

The front 1.20 m of a 1 400-kg car is designed as a "crumple zone" that collapses to absorb the shock of a collision. If a car traveling 25.0 m/s stops uniformly in 1.20 m, how long does the collision last, what is the magnitude of the average force on the car, and what is the magnitude of the acceleration of the car?

<p>(a) The collision lasts for a time interval of Δt = Δx/v = 1.20 m / 25.0 m/s = 0.048 s. (b) The magnitude of the average force acting on the car is F = m(v_f - v_i)/Δt = (1 400 kg)(0 - 25.0 m/s) / 0.048 s = 7.29 x 10⁵ N. (c) The magnitude of the acceleration of the car is a = (v_f - v_i)/Δt = (0 - 25.0 m/s) / 0.048 s = 5.21 x 10² m/s² or 53.1 g, where g is the acceleration due to gravity.</p> Signup and view all the answers

The magnitude of the net force exerted in the x direction on a 2.50-kg particle varies in time as shown in Figure P9.10. Find the impulse of the force over the 5.00-s time interval, the final velocity the particle attains if it is originally at rest, its final velocity if its original velocity is -2.001 m/s, and the average force exerted on the particle for the time interval between 0 and 5.00 s.

<p>(a) The impulse is equal to the area under the force-time curve. Calculating the area under the curve gives <em>I = (1/2)(4 N)(2 s) + (3 N)(1 s) + (1/2)(1 N)(2 s) = 12 N·s</em>. (b) The final velocity of the particle when initially at rest can be calculated using the impulse-momentum theorem: <em>I = m(v_f - v_i)</em>. Substituting the values gives <em>12 N·s = 2.50 kg (v_f - 0)</em>, giving <em>v_f = 4.80 m/s</em>. (c) If the initial velocity is -2.00 m/s, then the final velocity is <em>v_f = I/m + v_i = 12 N·s / 2.50 kg - 2.00 m/s = 2.80 m/s</em>. (d) The average force acting on the particle is the total impulse divided by the time interval. Therefore, <em>F_avg = I/Δt = 12 N·s / 5.00 s = 2.40 N</em>.</p> Signup and view all the answers

A 1 200-kg car traveling initially at v₁ = 25.0 m/s in an easterly direction crashes into the back of a 9 000-kg truck moving in the same direction at v₂ = 20.0 m/s (Fig. P9.12). The velocity of the car immediately after the collision is ucf = 18.0 m/s to the east. What is the velocity of the truck immediately after the collision? What is the change in mechanical energy of the car-truck system in the collision? Account for this change in mechanical energy.

<p>(a) Using the conservation of momentum, we can find the velocity of the truck after the collision: <em>m_car * v_car_i + m_truck * v_truck_i = m_car * v_car_f + m_truck * v_truck_f</em>. Solving for <em>v_truck_f</em> gives: <em>v_truck_f = (m_car * v_car_i + m_truck * v_truck_i – m_car * v_car_f) / m_truck = (1 200 kg * 25.0 m/s + 9 000 kg * 20.0 m/s - 1 200 kg * 18.0 m/s) / 9 000 kg = 20.4 m/s</em>. (b) The change in mechanical energy is <em>ΔKE = KE_f - KE_i = (1/2)m_car</em> <em>v_car_f² + (1/2)m_truck</em> <em>v_truck_f² - (1/2)m_car</em> <em>v_car_i² - (1/2)m_truck</em> <em>v_truck_i² = (1/2)(1 200 kg)(18.0 m/s)² + (1/2)(9 000 kg)(20.4 m/s)² - (1/2)(1 200 kg)(25.0 m/s)² - (1/2)(9 000 kg)(20.0 m/s)² = -7.20 x 10⁴ J</em>. (c) This negative change in mechanical energy is due to the inelastic nature of the collision. Some of the initial kinetic energy was transformed into other forms of energy, such as sound energy and heat energy, which are dissipated in the environment.</p> Signup and view all the answers

A railroad car of mass 2.50 × 10⁴ kg is moving with a speed of 4.00 m/s. It collides and couples with three other coupled railroad cars, each of the same mass as the single car and moving in the same direction with an initial speed of 2.00 m/s. What is the speed of the four cars after the collision? What is the decrease in mechanical energy in the collision?

<p>(a) Using the conservation of momentum, the final speed of the four cars can be calculated by: <em>m1</em> *v1_i + <em>m2</em> <em>v2_i = (m1 + m2) * v_f</em>. where <em>m1</em> = 2.50 x 10⁴ kg, *v1_i = 4.00 m/s, <em>m2</em> = 3(2.50 x 10⁴ kg) = 7.50 x 10⁴ kg, and <em>v2_i = 2.00 m/s</em>. Solving for <em>v_f</em> gives <em>v_f = (m1 * v1_i + m2 * v2_i) / (m1 + m2) = (2.50 x 10⁴ kg * 4.00 m/s + 7.50 x 10⁴ kg * 2.00 m/s) / (2.50 x 10⁴ kg + 7.50 x 10⁴ kg) = 2.67 m/s</em>. (b) The decrease in mechanical energy is <em>ΔKE = KE_i - KE_f = (1/2)m1</em> <em>v1_i² + (1/2)m2</em> <em>v2_i² - (1/2)(m1 + m2)</em> <em>v_f² = (1/2)(2.50 x 10⁴ kg)(4.00 m/s)² + (1/2)(7.50 x 10⁴ kg)(2.00 m/s)² - (1/2)(2.50 x 10⁴ kg + 7.50 x 10⁴ kg)(2.67 m/s)² = -1.67 x 10⁵ J</em>. This negative change in mechanical energy is due to the inelastic nature of the collision, where some of the kinetic energy was converted to other forms of energy, such as heat and sound.</p> Signup and view all the answers

Four railroad cars, each of mass 2.50 × 10⁴ kg, are coupled together and coasting along horizontal tracks at speed v toward the south. A very strong but foolish movie actor, riding on the second car, uncouples the front car and gives it a big push, increasing its speed to 4.00 m/s southward. The remaining three cars continue moving south, now at 2.00 m/s. Find the initial speed of the four cars. By how much did the potential energy within the body of the actor change? State the relationship between the process described here and the process in Problem 13.

<p>(a) Since the momentum of the system is conserved, the total initial momentum of the four cars must equal the total final momentum. We can write this equation as: <em>m_1</em> *v_i + <em>m_2</em> *v_i + <em>m_3</em> *v_i + <em>m_4</em> *v_i = <em>m_1</em> *v_1_f + <em>m_2</em> *v_2_f + <em>m_3</em> <em>v_3_f</em>. Since all the cars have the same mass (2.50 x 10⁴ kg), we can simplify this to <em>4mv_i = mv_1_f + 3mv_2_f</em>. Substituting the values for the final velocities we obtain <em>4v_i = 4.00 m/s + 3(2.00 m/s)</em>. Solving for <em>v_i</em> gives: <em>v_i = 2.50 m/s</em>. (b) The potential energy of the actor did not change because the actor exerted a force on the front car, pushing it, but the actor himself was already moving at the initial speed of 2.50 m/s. This means that the total kinetic energy of the actor did not change during the pushing process. (c) The process described here is essentially the reverse of the process in Problem 13. In Problem 13, the coupling of the four cars resulted in a decrease in kinetic energy, while in this problem, the uncoupling and pushing of the front car results in an increase in kinetic energy. Both problems illustrate the principle of conservation of momentum and energy, but they involve different scenarios and emphasize different aspects of these principles.</p> Signup and view all the answers

A car of mass m moving at a speed v₁ collides and couples with the back of a truck of mass 2m moving initially in the same direction as the car at a lower speed v₂. What is the speed of the two vehicles immediately after the collision? What is the change in kinetic energy of the car-truck system in the collision?

<p>(a) The total momentum of the system (car + truck) is conserved in the collision. We can write this as <em>m1</em> <em>v1_i + <em>m2</em> <em>v2_i = (<em>m1 + <em>m2</em>) * v_f</em>, where <em>m1</em> = <em>m</em>, <em>v1_i</em> = <em>v1</em>, <em>m2</em> = 2</em>m</em>, <em>v2_i</em> = <em>v2</em>, and <em>v_f</em> is the final velocity of the combined system. Solving for <em>v_f</em> gives: <em>v_f = (<em>m1</em> <em>v1_i + <em>m2</em> <em>v2_i) / (<em>m1 + <em>m2</em>) = (<em>m</em> <em>v1</em> + 2</em>m</em> <em>v2</em>) / (3</em>m</em>) = (v1 + 2v2) / 3*. (b) The change in kinetic energy is *ΔKE = KE_f - KE_i = (1/2)(*m1 + <em>m2</em>) <em>v_f² - (1/2)<em>m1</em> <em>v1_i² - (1/2)<em>m2</em> <em>v2_i² = (1/2)(3</em>m</em>)(v1 + 2v2)² / 9 - (1/2)<em>m</em> <em>v1² - (1/2)(2</em>m</em>) <em>v2² = -m(v1² + 2v1v2 + 4v2²) / 18</em>. The negative sign indicates that the kinetic energy of the system decreased during the collision.</p> Signup and view all the answers

A 7.00-g bullet, when fired from a gun into a 1.00-kg block of wood held in a vise, penetrates the block to a depth of 8.00 cm. This block of wood is next placed on a frictionless horizontal surface, and a second 7.00-g bullet is fired from the gun into the block. To what depth will the bullet penetrate the block in this case?

<p>The depth to which the bullet penetrates the block depends on the work done by the bullet's force. The work done is equal to the change in kinetic energy of the bullet. Since the bullet is fired at the same initial speed in both cases, and the work done is equal to the change in kinetic energy, which is the same in both cases, the penetration depth will be the same in both cases, 8.00 cm.</p> Signup and view all the answers

A tennis ball of mass 57.0 g is held just above a basketball of mass 590 g as shown in Figure P9.17. With their centers vertically aligned, both balls are released from rest at the same time, to fall through a distance of 1.20 m. Find the magnitude of the downward velocity with which the basketball reaches the ground. Assume that an elastic collision with the ground instantaneously reverses the velocity of the basketball while the tennis ball is still moving down. Next, the two balls meet in an elastic collision. To what height does the tennis ball rebound?

<p>(a) The final velocity of the basketball when it hits the ground can be calculated using the equation <em>v² = 2gh</em>: <em>v = √(2gh) = √(2 x 9.8 m/s² x 1.20 m) = 4.85 m/s</em>. (b) Since the collision is perfectly elastic, the kinetic energy of the system (basketball + tennis ball) is conserved. Let <em>v1</em> and <em>v2</em> be the velocities of the basketball and the tennis ball, respectively, before the collision, and <em>v1’</em> and <em>v2’</em> be their velocities after the collision. We can apply the conservation of energy equation: <em>(1/2)m1v1² + (1/2)m2v2² = (1/2)m1v1’² + (1/2)m2v2’²</em>. Since both the tennis ball and the basketball have the same mass, <em>m1 = m2 = m</em>, and since the collision is elastic, the speeds of the two balls are swapped after the collision. <em>v2 = 4.85 m/s</em> and <em>v1 = -4.85 m/s</em>. Therefore, <em>v2’ = 4.85 m/s</em> and *v1’ = -4.85 m/s.</p> Signup and view all the answers

Study Notes

Problems

  • Various physics problems are presented, covering topics like linear momentum, analysis models, and collisions.

SECTION 9.1 Linear Momentum

  • Kinetic Energy: Kinetic energy (K) of a particle with momentum (p) and mass (m) is K = p²/2m.
  • Momentum Magnitude: The magnitude of a particle's momentum can be expressed in terms of its kinetic energy and mass.
  • Momentum Components: Examples show how to find the x and y components of momentum for a particle with given mass and velocity.
  • Momentum Magnitude and Direction: Examples show how to find the overall magnitude and direction of a particle's momentum given its components.

SECTION 9.2 Analysis Model: Isolated System (Momentum)

  • Isolated System: A 65 kg boy and 40 kg sister, pushing each other, are examples of an isolated system (ignoring friction).
  • Conservation of Momentum: The momentum of the boy-girl system is conserved during the pushing-apart process, even though there are large forces acting and significant changes in motion.
  • Elastic Potential Energy: The original elastic potential energy initially stored in a spring is converted into kinetic energy of the blocks after the spring is released.
  • Momentum Conservation in Bursting Apart: Momentum conservation in an isolated system is possible even with large forces and significant changes in motion.

SECTION 9.3 Analysis Model: Nonisolated System (Momentum)

  • Glider Motion: A glider on an air track, pushed by a spring, demonstrates how to relate force constant, distance of compression, and mass to the glider's speed.
  • Impulse Definition: Impulse imparted to a glider is calculated using the spring constant and compression distance.
  • Work and Mass: More work is done on a cart with a smaller mass.

SECTION 9.4 Collisions in One Dimension

  • One-Dimensional Collision: A 1200 kg car and a 9000 kg truck example illustrates one-dimensional collision, where momentum is conserved.
  • Change in Mechanical Energy: Calculations explore and explain the changes in mechanical energy during collisions. Examples calculate changes in energy due to collisions.
  • Speed of Four Coupled Railroad Cars: Given initial speeds in a collision, calculate the single final speed of the four cars that couple together.

SECTION 9.5 Collisions in Two Dimensions

  • Collisions in Two Dimensions: Problems that involve two dimensions during collisions, such as a collision between two discs.
  • Final Speed of Each Disk: Computes the final speed of both disks in a glancing collision.
  • Perfectly Inelastic Collision: Illustrates the perfectly inelastic collision between a fullback and an opponent, demonstrating the conservation of momentum in the collision.

SECTION 9.6 The Center of Mass

  • Center of Mass: Calculates the x and y coordinates of the center of mass of a uniform piece of sheet metal.
  • Vector Position: Finds the vector position, linear momentum, velocity, acceleration, and net force of a particle with given mass and varying position in time.
  • Systems of Many Particles: Coordinates, velocities, and momentum of systems with multiple particles.

SECTION 9.7 Systems of Many Particles

  • Two Particle System: Calculates the position of the center of mass of a two-particle system in the xy plane.
  • Total Momentum: Computes the total linear momentum of the system.

SECTION 9.8 Deformable Systems

  • Maximum Spring Extension: A projectile fired from a cannon attached to a carriage causes the spring to extend to a maximum value due to recoil.
  • Work Done by Spring: Calculates the maximum force exerted by the spring on the carriage, and mechanical energy conservation.
  • Bullet Fired into a Block: A bullet fired into a block of wood resting on a table rises to a maximum height, and its initial velocity is calculated.

SECTION 9.9 Rocket Propulsion

  • Rocket Propulsion: Calculates the amount of fuel needed for a rocket to reach a given speed.
  • Rocket Velocity: Describes the velocity of a rocket as a function of time during its burn.
  • Rocket Acceleration: Displays formulas and graphs of acceleration as a function of time for a rocket.
  • Rocket Position: Shows graphs of a rocket's position during a burn.

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Explore the principles of linear momentum through various physics problems. This quiz covers kinetic energy, momentum components, and the conservation of momentum in isolated systems. Test your understanding of these vital concepts in classical mechanics.

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