IB Physics Quiz: Apply Forces And Momentum
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Apply Forces And MomentumQuestion 1 of 20

A block of mass mm moving with speed vv makes a head-on perfectly inelastic collision with a stationary block of mass (3m). The two blocks stick together. What fraction of the initial kinetic energy is converted to other forms of energy?

1/4
1/3
2/3
3/4
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IB Physics Quiz

IB Physics Quiz: Apply Forces And Momentum

Practice Apply Forces And Momentum in IB Physics with focused quiz questions that help you check what you know, review explanations, and build confidence with test-style prompts.

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Question 1

A block of mass mm moving with speed vv makes a head-on perfectly inelastic collision with a stationary block of mass (3m). The two blocks stick together. What fraction of the initial kinetic energy is converted to other forms of energy?

  1. 1/4
  2. 1/3
  3. 2/3
  4. 3/4 (correct answer)
Explanation: Initial momentum is pi=mvp_i = mv. Initial kinetic energy is KEi=12mv2KE_i = \frac{1}{2}mv^2. After the collision, the combined mass is (4m). By conservation of momentum, mv=(4m)vfmv = (4m)v_f, so the final velocity is vf=v/4v_f = v/4. The final kinetic energy is KEf=12(4m)vf2=12(4m)(v/4)2=12(4m)(v2/16)=18mv2KE_f = \frac{1}{2}(4m)v_f^2 = \frac{1}{2}(4m)(v/4)^2 = \frac{1}{2}(4m)(v^2/16) = \frac{1}{8}mv^2. The energy lost is ΔKE=KEiKEf=12mv218mv2=38mv2\Delta KE = KE_i - KE_f = \frac{1}{2}mv^2 - \frac{1}{8}mv^2 = \frac{3}{8}mv^2. The fraction of energy lost is ΔKEKEi=38mv212mv2=34\frac{\Delta KE}{KE_i} = \frac{\frac{3}{8}mv^2}{\frac{1}{2}mv^2} = \frac{3}{4}.

Question 2

A large truck of mass MM collides with a small car of mass mm (where M>mM > m). During the collision, which of the following statements is always correct?

  1. The force exerted by the truck on the car is greater than the force exerted by the car on the truck.
  2. The change in momentum of the truck is equal in magnitude to the change in momentum of the car. (correct answer)
  3. The acceleration of the truck is equal in magnitude to the acceleration of the car.
  4. The change in kinetic energy of the truck is equal to the change in kinetic energy of the car.
Explanation: According to Newton's third law, the force the truck exerts on the car is equal in magnitude and opposite in direction to the force the car exerts on the truck. Since the forces are equal and act for the same time interval, the impulses (FΔtF\Delta t) on both vehicles are equal in magnitude. Since impulse is equal to the change in momentum, the magnitudes of the changes in momentum are equal.

Question 3

A block of mass 3.0 kg rests on a rough horizontal table (coefficient of kinetic friction 0.20). It is connected by a light string over a frictionless pulley to a hanging block of mass 1.0 kg. The system is released from rest. What is the acceleration of the system? (Use g=10 m s2g = 10 \text{ m s}^{-2})

  1. 1.0 m s⁻² (correct answer)
  2. 1.3 m s⁻²
  3. 2.5 m s⁻²
  4. 3.3 m s⁻²
Explanation: The driving force is the weight of the hanging block: Fdrive=mhangg=1.0×10=10 NF_{drive} = m_{hang}g = 1.0 \times 10 = 10 \text{ N}. The opposing friction force is Ff=μkFN=μkmtableg=0.20×3.0×10=6.0 NF_f = \mu_k F_N = \mu_k m_{table}g = 0.20 \times 3.0 \times 10 = 6.0 \text{ N}. The net force on the system is Fnet=FdriveFf=106.0=4.0 NF_{net} = F_{drive} - F_f = 10 - 6.0 = 4.0 \text{ N}. This net force accelerates the total mass of the system, Mtotal=mhang+mtable=1.0+3.0=4.0 kgM_{total} = m_{hang} + m_{table} = 1.0 + 3.0 = 4.0 \text{ kg}. Using Newton's second law, a=Fnet/Mtotal=4.0/4.0=1.0 m s2a = F_{net} / M_{total} = 4.0 / 4.0 = 1.0 \text{ m s}^{-2}.

Question 4

A small sphere falls through a viscous fluid and reaches a terminal velocity vtv_t. If the experiment is repeated with a sphere of the same size and material but in a fluid with four times the viscosity, what will be the new terminal velocity?

  1. vt/4v_t/4 (correct answer)
  2. vt/2v_t/2
  3. 2vt2v_t
  4. 4vt4v_t
Explanation: At terminal velocity, the net force on the sphere is zero. The downward gravitational force (weight) is balanced by the upward buoyant force and the viscous drag force. Thus, Fg=Fb+FdF_g = F_b + F_d. The drag force is given by Stokes' Law, Fd=6πηrvtF_d = 6\pi\eta r v_t. Since FgF_g and FbF_b are constant for the same sphere and fluid density, the drag force FdF_d must also be constant at terminal velocity. This means the product ηvt\eta v_t is constant. If the viscosity η\eta is multiplied by 4, the terminal velocity vtv_t must be divided by 4 to keep the product constant.

Question 5

A person stands on a weighing scale in a lift. The scale shows a reading R1R_1 as the lift starts moving upwards from rest, R2R_2 as it moves upwards at a constant speed, and R3R_3 as it slows to a stop at a higher floor. Which statement correctly compares the magnitudes of the readings?

  1. R1>R2>R3R_1 > R_2 > R_3 (correct answer)
  2. R3>R2>R1R_3 > R_2 > R_1
  3. R1=R3>R2R_1 = R_3 > R_2
  4. R2>R1>R3R_2 > R_1 > R_3
Explanation: The scale reading equals the normal force FNF_N. Let mm be the person's mass. When accelerating upwards (starting), FNmg=maF_N - mg = ma, so R1=m(g+a)>mgR_1 = m(g+a) > mg. When moving at constant speed, a=0a=0, so FNmg=0F_N - mg = 0, and R2=mgR_2 = mg. When decelerating upwards (slowing), the acceleration is downwards, so FNmg=maF_N - mg = -ma, and R3=m(ga)<mgR_3 = m(g-a) < mg. Therefore, the order of the readings is R1>R2>R3R_1 > R_2 > R_3.

Question 6

An object of mass 5.0 kg is initially at rest. It is subjected to two perpendicular forces, F1=30F_1 = 30 N and F2=40F_2 = 40 N. What is the magnitude of the object's acceleration?

  1. 2.0 m s⁻²
  2. 10 m s⁻² (correct answer)
  3. 14 m s⁻²
  4. 50 m s⁻²
Explanation: The net force on the object is the vector sum of the two perpendicular forces. The magnitude of the net force can be found using the Pythagorean theorem: Fnet=F12+F22=302+402=900+1600=2500=50 NF_{net} = \sqrt{F_1^2 + F_2^2} = \sqrt{30^2 + 40^2} = \sqrt{900 + 1600} = \sqrt{2500} = 50 \text{ N}. According to Newton's second law, Fnet=maF_{net} = ma. Therefore, the acceleration is a=Fnet/m=50 N/5.0 kg=10 m s2a = F_{net} / m = 50 \text{ N} / 5.0 \text{ kg} = 10 \text{ m s}^{-2}.

Question 7

Three blocks with masses m1=1.0m_1 = 1.0 kg, m2=2.0m_2 = 2.0 kg, and m3=3.0m_3 = 3.0 kg are connected by light, inextensible strings. The blocks are pulled along a frictionless horizontal surface by a horizontal force F=12F = 12 N applied to m3m_3. What is the tension in the string connecting m1m_1 and m2m_2?

  1. 6.0 N
  2. 4.0 N
  3. 2.0 N (correct answer)
  4. 12 N
Explanation: First, find the acceleration of the entire system. The total mass is M=m1+m2+m3=1.0+2.0+3.0=6.0 kgM = m_1 + m_2 + m_3 = 1.0 + 2.0 + 3.0 = 6.0 \text{ kg}. The net force on the system is F=12 NF = 12 \text{ N}. The acceleration is a=F/M=12 N/6.0 kg=2.0 m s2a = F/M = 12 \text{ N} / 6.0 \text{ kg} = 2.0 \text{ m s}^{-2}. The tension in the string between m1m_1 and m2m_2, let's call it T1T_1, is the force that accelerates m1m_1. Applying Newton's second law to m1m_1 alone: T1=m1a=1.0 kg×2.0 m s2=2.0 NT_1 = m_1 a = 1.0 \text{ kg} \times 2.0 \text{ m s}^{-2} = 2.0 \text{ N}.

Question 8

A block of mass mm rests on the floor of a lift that is accelerating upwards with acceleration aa. A horizontal force FF is applied to the block, but the block does not move. The coefficient of static friction between the block and the floor is μs\mu_s. What is the maximum possible value of FF for which the block will not move?

  1. μsmg\mu_s m g
  2. μsma\mu_s m a
  3. μsm(ga)\mu_s m (g-a)
  4. μsm(g+a)\mu_s m (g+a) (correct answer)
Explanation: The net vertical force on the block is FNmg=maF_N - mg = ma, where FNF_N is the normal force. Therefore, FN=m(g+a)F_N = m(g+a). The maximum static friction force is Ff,max=μsFNF_{f,max} = \mu_s F_N. For the block not to move, the applied horizontal force FF must be less than or equal to the maximum static friction force. The maximum possible value of FF is thus Fmax=μsFN=μsm(g+a)F_{max} = \mu_s F_N = \mu_s m(g+a).

Question 9

A car travels at a constant speed over a circular hump-backed bridge of radius rr. What is the maximum speed the car can have at the highest point of the bridge without losing contact with the road?

  1. gr\sqrt{gr} (correct answer)
  2. 2gr\sqrt{2gr}
  3. grgr
  4. g/r\sqrt{g/r}
Explanation: At the highest point of the bridge, the net force on the car provides the centripetal force required for circular motion. The forces acting on the car are gravity (mgmg, downwards) and the normal force from the road (FNF_N, upwards). The net force is mgFNmg - F_N, directed towards the center of the circle (downwards). So, mgFN=mv2/rmg - F_N = mv^2/r. The car loses contact with the road when the normal force FNF_N becomes zero. Setting FN=0F_N = 0, we get mg=mvmax2/rmg = mv_{max}^2/r. Solving for vmaxv_{max} gives vmax=grv_{max} = \sqrt{gr}.

Question 10

A block of mass mm is on a horizontal surface with a coefficient of static friction μs\mu_s. A pulling force FF is applied at an angle θ\theta above the horizontal. What is the minimum magnitude of FF that will cause the block to start moving?

  1. μsmgcosθ\frac{\mu_s mg}{\cos\theta}
  2. μsmgcosθ+μssinθ\frac{\mu_s mg}{\cos\theta + \mu_s \sin\theta} (correct answer)
  3. μsmg\mu_s mg
  4. μsmgcosθμssinθ\frac{\mu_s mg}{\cos\theta - \mu_s \sin\theta}
Explanation: To start moving, the horizontal component of the applied force must overcome static friction: FcosθFfF\cos\theta \ge F_f. The normal force FNF_N is reduced by the upward component of FF, so FN+Fsinθ=mgF_N + F\sin\theta = mg, which means FN=mgFsinθF_N = mg - F\sin\theta. The maximum static friction is Ff,max=μsFN=μs(mgFsinθ)F_{f,max} = \mu_s F_N = \mu_s(mg - F\sin\theta). Setting the forces equal for the minimum condition: Fcosθ=μs(mgFsinθ)F\cos\theta = \mu_s(mg - F\sin\theta). Rearranging to solve for F: Fcosθ=μsmgμsFsinθF\cos\theta = \mu_s mg - \mu_s F\sin\theta, so F(cosθ+μssinθ)=μsmgF(\cos\theta + \mu_s \sin\theta) = \mu_s mg. Thus, F=μsmgcosθ+μssinθF = \frac{\mu_s mg}{\cos\theta + \mu_s \sin\theta}.

Question 11

A 20 kg crate is pushed 5.0 m up a rough incline at a constant velocity by a force parallel to the incline. The incline is at 30° to the horizontal and the coefficient of kinetic friction is 0.20. What is the work done by the applied force? (Use g=10 m s2g = 10 \text{ m s}^{-2})

  1. 500 J
  2. 670 J (correct answer)
  3. 700 J
  4. 1000 J
Explanation: Since velocity is constant, the net force is zero. The applied force FappF_{app} must balance the force of friction FfF_f and the component of gravity parallel to the incline, mgsinθmg\sin\theta. Fapp=Ff+mgsinθF_{app} = F_f + mg\sin\theta. The normal force is FN=mgcosθ=20×10×cos(30)=173.2 NF_N = mg\cos\theta = 20 \times 10 \times \cos(30^{\circ}) = 173.2\text{ N}. The friction force is Ff=μkFN=0.20×173.2=34.64 NF_f = \mu_k F_N = 0.20 \times 173.2 = 34.64\text{ N}. The gravity component is mgsinθ=20×10×sin(30)=100 Nmg\sin\theta = 20 \times 10 \times \sin(30^{\circ}) = 100\text{ N}. So, Fapp=34.64+100=134.64 NF_{app} = 34.64 + 100 = 134.64\text{ N}. The work done is W=Fapp×d=134.64×5.0=673.2 JW = F_{app} \times d = 134.64 \times 5.0 = 673.2\text{ J}, which is approximately 670 J.

Question 12

A child and a skateboard have a combined mass of 49 kg. They are stationary on a frictionless horizontal surface. The child throws a 1.0 kg ball horizontally with a speed of 50 m s⁻¹ relative to the skateboard. What is the magnitude of the final velocity of the skateboard?

  1. 0.98 m s⁻¹
  2. 1.0 m s⁻¹ (correct answer)
  3. 1.02 m s⁻¹
  4. 1.04 m s⁻¹
Explanation: Let MM be the mass of the child and skateboard (49 kg) and mm be the mass of the ball (1.0 kg). Let vsv_s be the final velocity of the skateboard and vbv_b be the final velocity of the ball, both relative to the ground. The velocity of the ball relative to the skateboard is vrel=vbvs=50 m s1v_{rel} = v_b - v_s = 50 \text{ m s}^{-1}. So, vb=50+vsv_b = 50 + v_s. Total momentum is conserved, and the initial momentum is zero. Mvs+mvb=0Mv_s + mv_b = 0. Substituting for vbv_b: Mvs+m(50+vs)=0Mv_s + m(50 + v_s) = 0. (M+m)vs+50m=0(M+m)v_s + 50m = 0. vs=50mM+m=50×1.049+1.0=5050=1.0 m s1v_s = -\frac{50m}{M+m} = -\frac{50 \times 1.0}{49+1.0} = -\frac{50}{50} = -1.0 \text{ m s}^{-1}. The magnitude is 1.0 m s⁻¹.

Question 13

An object of mass 2.0 kg is initially at rest. A time-varying horizontal force acts on it. The force starts at 0 N, increases linearly to 10 N over 2.0 s, and then decreases linearly to 0 N over the next 2.0 s. What is the final speed of the object, assuming no friction?

  1. 5.0 m s⁻¹
  2. 10 m s⁻¹ (correct answer)
  3. 20 m s⁻¹
  4. 40 m s⁻¹
Explanation: The change in momentum of the object is equal to the impulse, which is the area under the force-time graph. The graph described is a triangle with a base of 4.0 s (2.0 s + 2.0 s) and a height of 10 N. The area is Impulse=12×base×height=12×4.0 s×10 N=20 Ns\text{Impulse} = \frac{1}{2} \times \text{base} \times \text{height} = \frac{1}{2} \times 4.0 \text{ s} \times 10 \text{ N} = 20 \text{ Ns}. Since impulse equals change in momentum (J=Δp=mΔvJ = \Delta p = m\Delta v) and the object starts from rest, 20 Ns=(2.0 kg)×vf20 \text{ Ns} = (2.0 \text{ kg}) \times v_f. Solving for the final speed gives vf=20/2.0=10 m s1v_f = 20 / 2.0 = 10 \text{ m s}^{-1}.

Question 14

An object of mass mm is attached to a string and moves in a horizontal circle of radius rr as a conical pendulum. The string makes an angle θ\theta with the vertical. What is the speed of the object?

  1. gr\sqrt{gr}
  2. grtanθ\sqrt{gr \tan\theta} (correct answer)
  3. grsinθ\sqrt{gr \sin\theta}
  4. gr/tanθ\sqrt{gr / \tan\theta}
Explanation: Let TT be the tension in the string. Vertically, the forces are balanced: Tcosθ=mgT \cos\theta = mg. Horizontally, the net force provides the centripetal force: Tsinθ=mv2/rT \sin\theta = mv^2/r. Dividing the second equation by the first gives TsinθTcosθ=mv2/rmg\frac{T \sin\theta}{T \cos\theta} = \frac{mv^2/r}{mg}, which simplifies to tanθ=v2/(gr)\tan\theta = v^2/(gr). Rearranging for the speed vv gives v=grtanθv = \sqrt{gr \tan\theta}.

Question 15

A mass mm is attached to a vertical spring with spring constant kk. The mass is at rest at its equilibrium position. It is then displaced downwards by a distance AA and released. What is the magnitude of the net force on the mass when it is at a distance A/2A/2 above the equilibrium position?

  1. kA/2kA/2 (correct answer)
  2. mgkA/2mg - kA/2
  3. mg+kA/2mg + kA/2
  4. kAkA
Explanation: At the equilibrium position, the upward spring force balances the downward force of gravity, kx0=mgkx_0 = mg, where x0x_0 is the equilibrium extension. When the mass is a distance y=A/2y = A/2 above equilibrium, the spring extension is x0yx_0 - y. The upward spring force is Fspring=k(x0y)=kx0ky=mgkyF_{spring} = k(x_0 - y) = kx_0 - ky = mg - ky. The net force is Fnet=Fspringmg=(mgky)mg=kyF_{net} = F_{spring} - mg = (mg - ky) - mg = -ky. The magnitude of this restoring force is kyky. Substituting y=A/2y=A/2, the magnitude of the net force is k(A/2)k(A/2).

Question 16

A rocket of total mass MM is at rest in deep space. It expels a small mass of gas Δm\Delta m with a high speed uu relative to the rocket. What is the approximate recoil speed, Δv\Delta v, of the rocket?

  1. uΔmMu \frac{\Delta m}{M} (correct answer)
  2. uMΔmu \frac{M}{\Delta m}
  3. uΔmMΔmu \frac{\Delta m}{M - \Delta m}
  4. uu
Explanation: The total momentum of the rocket-gas system is conserved and is initially zero. After the gas is expelled, the rocket has mass MΔmM - \Delta m and velocity Δv\Delta v. The gas has mass Δm\Delta m and its velocity relative to the rocket is u-u. Its velocity relative to the initial rest frame is vgas=Δvuv_{gas} = \Delta v - u. By conservation of momentum: 0=(MΔm)Δv+Δm(Δvu)0 = (M - \Delta m)\Delta v + \Delta m (\Delta v - u). Expanding gives 0=MΔvΔmΔv+ΔmΔvuΔm0 = M\Delta v - \Delta m \Delta v + \Delta m \Delta v - u\Delta m, which simplifies to MΔv=uΔmM\Delta v = u\Delta m. For a small expelled mass, we can approximate the rocket's mass as M, so ΔvuΔmM\Delta v \approx u \frac{\Delta m}{M}.

Question 17

A stationary object of mass 3.0 kg explodes into three fragments of equal mass (1.0 kg each). Immediately after the explosion, one fragment moves east at 8.0 m s⁻¹ and a second fragment moves north at 6.0 m s⁻¹. What is the speed of the third fragment?

  1. 2.0 m s⁻¹
  2. 7.0 m s⁻¹
  3. 10 m s⁻¹ (correct answer)
  4. 14 m s⁻¹
Explanation: The total momentum of the system is conserved and is initially zero. Let the momentum vectors of the three fragments be p1p_1, p2p_2, and p3p_3. By conservation of momentum, p1+p2+p3=0p_1 + p_2 + p_3 = 0, so p3=(p1+p2)p_3 = -(p_1 + p_2). Let east be the x-direction and north be the y-direction. p1=(1.0 kg)(8.0 m s1)i^=8.0i^ Nsp_1 = (1.0 \text{ kg})(8.0 \text{ m s}^{-1}) \hat{i} = 8.0 \hat{i} \text{ Ns}. p2=(1.0 kg)(6.0 m s1)j^=6.0j^ Nsp_2 = (1.0 \text{ kg})(6.0 \text{ m s}^{-1}) \hat{j} = 6.0 \hat{j} \text{ Ns}. So, p3=(8.0i^+6.0j^) Nsp_3 = -(8.0 \hat{i} + 6.0 \hat{j}) \text{ Ns}. The magnitude of p3p_3 is p3=(8.0)2+(6.0)2=64+36=100=10 Ns|p_3| = \sqrt{(-8.0)^2 + (-6.0)^2} = \sqrt{64 + 36} = \sqrt{100} = 10 \text{ Ns}. The speed of the third fragment is v3=p3/m3=10 Ns/1.0 kg=10 m s1v_3 = |p_3|/m_3 = 10 \text{ Ns} / 1.0 \text{ kg} = 10 \text{ m s}^{-1}.

Question 18

An object with a volume of 5.0×104 m35.0 \times 10^{-4} \text{ m}^3 and a density of 800 kg m⁻³ is fully submerged in water (density 1000 kg m⁻³). It is held stationary by a vertical string attached to the bottom of the tank. What is the tension in the string? (Use g=10 m s2g = 10 \text{ m s}^{-2})

  1. 5.0 N
  2. 4.0 N
  3. 1.0 N (correct answer)
  4. 9.0 N
Explanation: The forces acting on the object are its weight (downwards), the buoyant force (upwards), and the tension in the string (downwards). For equilibrium, the upward force equals the sum of the downward forces: Fb=W+TF_b = W + T. The weight is W=mobjg=(ρobjV)g=(800×5.0×104)×10=4.0 NW = m_{obj}g = (\rho_{obj}V)g = (800 \times 5.0 \times 10^{-4}) \times 10 = 4.0 \text{ N}. The buoyant force is Fb=ρwaterVg=(1000×5.0×104)×10=5.0 NF_b = \rho_{water}Vg = (1000 \times 5.0 \times 10^{-4}) \times 10 = 5.0 \text{ N}. The tension is T=FbW=5.0 N4.0 N=1.0 NT = F_b - W = 5.0 \text{ N} - 4.0 \text{ N} = 1.0 \text{ N}.

Question 19

A 50 g ball strikes a rigid wall horizontally at a speed of 20 m s⁻¹ and rebounds horizontally at a speed of 15 m s⁻¹. The ball is in contact with the wall for 10 ms. What is the magnitude of the average force exerted by the wall on the ball?

  1. 25 N
  2. 75 N
  3. 100 N
  4. 175 N (correct answer)
Explanation: The impulse is equal to the change in momentum, J=Δp=FavgΔtJ = \Delta p = F_{avg} \Delta t. Momentum is a vector. Let the initial direction be positive. Initial momentum pi=0.050 kg×20 m s1=1.0 Nsp_i = 0.050 \text{ kg} \times 20 \text{ m s}^{-1} = 1.0 \text{ Ns}. Final momentum pf=0.050 kg×(15 m s1)=0.75 Nsp_f = 0.050 \text{ kg} \times (-15 \text{ m s}^{-1}) = -0.75 \text{ Ns}. Change in momentum Δp=pfpi=0.751.0=1.75 Ns\Delta p = p_f - p_i = -0.75 - 1.0 = -1.75 \text{ Ns}. The magnitude of the impulse is 1.75 Ns. The average force is Favg=Δp/Δt=1.75 Ns/(10×103 s)=175 NF_{avg} = |\Delta p| / \Delta t = 1.75 \text{ Ns} / (10 \times 10^{-3} \text{ s}) = 175 \text{ N}.

Question 20

A rocket of initial mass 1500 kg burns fuel at a rate of 8.0 kg/s, ejecting exhaust at 2400 m/s relative to the rocket. The rocket starts from rest in space. What is the rocket's acceleration when its mass has decreased to 1200 kg?

  1. 12.8 m/s² because thrust equals mass flow rate times exhaust velocity
  2. 16.0 m/s² because acceleration increases as mass decreases linearly (correct answer)
  3. 14.4 m/s² because thrust depends on instantaneous mass and fuel consumption
  4. 18.2 m/s² because exhaust momentum creates proportional acceleration increase
Explanation: For a rocket, thrust F=dmdtve=8.0×2400=19200F = \frac{dm}{dt} v_e = 8.0 \times 2400 = 19200 N. When the rocket's mass is 1200 kg, acceleration a=Fm=192001200=16.0a = \frac{F}{m} = \frac{19200}{1200} = 16.0 m/s². The thrust remains constant as long as fuel burn rate and exhaust velocity are constant. Choice A incorrectly calculates thrust division by wrong mass. Choice C uses an incorrect formula mixing instantaneous mass with flow rate incorrectly. Choice D uses an incorrect proportionality assumption about momentum and acceleration.