Physics guide

Newton's Second Law Problems With Solutions: Net Force to Acceleration

Solve four F=ma problems step by step, including friction, an elevator, and an incline. Learn to draw forces, choose signs, and check your answer.

Illustration of a wooden block resting on an inclined plane

Newton's second law says the net force on an object equals its mass times its acceleration: ∑F=ma\sum F=ma. In a typical problem, draw the forces acting on the chosen object, pick a positive direction, add force components with their signs, and only then divide by the mass. A 4 kg object with a 20 N net force accelerates at 5 m/s².

The common trap is using just one force when several act. A 5050 N push opposed by 1818 N of friction produces 3232 N of net force, not 5050 N.

A repeatable four-step method

  1. Choose the object or system. Only draw forces acting on that system. An object does not exert a force on itself.
  2. Draw a free-body diagram. Label weight, normal force, tension, applied force and friction only when they really act. Our free-body-diagram guide goes deeper on this step.
  3. Choose axes and write a signed net-force equation for each relevant axis. For a horizontal push, right might be positive. For an incline, an axis parallel to the slope is often easier.
  4. Solve and check. Use 1 N=1 kg⋅m/s21\text{ N}=1\text{ kg}\cdot\text{m/s}^2. Acceleration should point in the net-force direction.

The second law uses net force, which is a vector sum. Forces at right angles cannot simply be added as ordinary positive numbers. OpenStax's treatment of Newton's law and other forces shows how axes make those components manageable.

Example 1: one horizontal net force

Problem: A 44 kg cart has a net horizontal force of 2020 N to the right. Find its acceleration.

Force picture: The problem already gives the net force. A full diagram of individual forces cannot be inferred from that information, but the resulting force arrow points right.

∑Fx=max,20=4ax,ax=5 m/s2.\sum F_x=ma_x,\qquad 20=4a_x,\qquad a_x=5\text{ m/s}^2.

Answer: 5 m/s25\text{ m/s}^2 to the right. The units check: N/kg is m/s2\text{m/s}^2. Do not assume the cart's velocity is 5 m/s5\text{ m/s}; acceleration and velocity are different quantities.

Example 2: a push opposed by friction

Problem: An 88 kg box moves on a level floor. A 5050 N force pushes it right, and kinetic friction is 1818 N left. Find its acceleration. Assume no vertical acceleration.

Free-body diagram, with the box as the system:

              normal force
                   ↑
friction 18 N ← [ box ] → push 50 N
                   ↓
                  weight

The normal force balances weight vertically. Horizontally, right is positive:

∑Fx=50−18=32 N=8ax,ax=4 m/s2.\sum F_x=50-18=32\text{ N}=8a_x, \qquad a_x=4\text{ m/s}^2.

Answer: 4 m/s24\text{ m/s}^2 right. Friction reduces the acceleration but does not reverse it because the push is larger.

Example 3: tension in an accelerating elevator

Problem: A 33 kg load hangs from a cable in an elevator accelerating upward at 2 m/s22\text{ m/s}^2. What is the cable tension? Use g=9.8 m/s2g=9.8\text{ m/s}^2 and ignore air resistance.

Force picture: Tension TT acts up on the load; weight mgmg acts down. Choose up as positive. Weight is 3(9.8)=29.43(9.8)=29.4 N.

∑Fy=T−mg=may,T=3(2)+29.4=35.4 N.\sum F_y=T-mg=ma_y,\qquad T=3(2)+29.4=35.4\text{ N}.

Answer: 35.435.4 N. It is greater than the 29.429.4 N weight, as it must be for upward acceleration. If the elevator moved upward at constant speed, acceleration would be zero and tension would equal weight.

Example 4: a block sliding down a rough incline

Problem: A 55 kg block is sliding down a 30∘30^\circ slope. The coefficient of kinetic friction is μk=0.20\mu_k=0.20. Find the acceleration down the slope. Use g=9.8 m/s2g=9.8\text{ m/s}^2.

Force picture: Weight mgmg points vertically down; the normal force NN points perpendicular to the slope; kinetic friction fkf_k points up the slope because it opposes the sliding. Choose downhill as the positive slope direction. Resolve weight into mgsin⁡30∘mg\sin30^\circ downhill and mgcos⁡30∘mg\cos30^\circ into the slope.

There is no acceleration perpendicular to the slope, so

N=mgcos⁡30∘=5(9.8)(0.8660)≈42.44 N.N=mg\cos30^\circ=5(9.8)(0.8660)\approx42.44\text{ N}.

Kinetic friction is fk=μkN≈0.20(42.44)=8.49f_k=\mu_kN\approx0.20(42.44)=8.49 N. The downhill weight component is mgsin⁡30∘=24.5mg\sin30^\circ=24.5 N. Therefore,

∑F∥=24.5−8.49=5a,a≈3.20 m/s2 downhill.\sum F_{\parallel}=24.5-8.49=5a, \qquad a\approx3.20\text{ m/s}^2\text{ downhill}.

Check: Without friction, the acceleration would be gsin⁡30∘=4.9 m/s2g\sin30^\circ=4.9\text{ m/s}^2 downhill. Friction makes 3.203.20 smaller, which is sensible. This calculation assumes the block is already sliding, so kinetic rather than static friction applies.

What to check before accepting an answer

Symptom Likely issue Fix
Acceleration points opposite the stated net force Sign error Redraw arrows and choose one positive direction
Acceleration is in N or kg Unit error a=Fnet/ma=F_{\rm net}/m must be in m/s2\text{m/s}^2
Normal force automatically set equal to mgmg on a slope Missing components Use N=mgcos⁡θN=mg\cos\theta for the simple incline setup
Applied force used in place of net force Missing friction or tension List every external force acting on the system

If the question continues from force to distance or stopping time, use the acceleration from ∑F=ma\sum F=ma in the kinematics equation guide. The Physics Solver can help check a pictured setup, and physics resources collects related tools.

Practice answers

1. A 6 kg cart has a 24 N net force left. Find its acceleration.

a=24/6=4 m/s2a=24/6=\mathbf{4\text{ m/s}^2} left. Choosing right as positive would produce a=−4 m/s2a=-4\text{ m/s}^2, which describes the same result.

2. A 10 kg box is pushed right with 45 N against 15 N of friction. Find its acceleration.

Fnet=45−15=30F_{\rm net}=45-15=30 N right, so a=30/10=3 m/s2a=30/10=\mathbf{3\text{ m/s}^2} right.

3. What tension supports a 2 kg load accelerating downward at 1 m/s²?

With up positive, T−mg=m(−1)T-mg=m(-1). Thus T=2(9.8−1)=17.6 NT=2(9.8-1)=\mathbf{17.6\text{ N}}, less than its 19.619.6 N weight.