Forces and Newton's Laws
Why bodies move the way they do. What a force is and the forces you will meet in every problem, inertia and the first law, F = ma, free-body diagrams drawn one force at a time, the third law and its pairs, and the plan that solves every dynamics problem.
Why this chapter
Kinematics told you how a body moves: where it is, how fast, how its velocity changes. It never asked why. This chapter answers that question with three laws that Newton wrote on a single page in 1687. A body keeps its velocity unless a force acts. A net force changes the velocity at a rate fixed by the mass. Every force has a partner on another body. With these laws and one careful drawing, the free-body diagram, you can work out the motion of anything from a Metro train to a cricket ball.
You will learn
- Name every force on a body, with its agent and its direction: weight, normal force, tension, spring force and an applied force.
- State the first law, explain inertia with Galileo's argument, and say when the net force on a body is zero.
- Use \(\sum \vec F = m\vec a\) as a vector law, along each axis, and tell mass from weight.
- Draw a complete free-body diagram, one force at a time, with no missing force and no invented one.
- Identify third-law pairs correctly and solve a single-body problem with the four-step plan.
Before you begin
You should know the kinematics of Unit 2: velocity and acceleration as vectors, the equations of motion for constant acceleration, and how to split a vector into two perpendicular components. You should be able to use sine and cosine for a given angle.
Lessons
Read in order. The small labels are the topics of each lesson. They take your colour as you answer the checks.
Glossary
The key words of this chapter, with the meaning this chapter gives them.
- action-reaction pair
- The two forces of one interaction: the force of A on B and the force of B on A. They are equal, opposite, of the same kind, and act on different bodies.
- contact force
- A force that acts only while two bodies touch, such as a push, the normal force, tension or friction.
- extension
- The change in length of a spring from its natural length. A compression is a negative extension.
- force
- A push or a pull exerted by one body on another. It is a vector, measured in newtons.
- free-body diagram
- A drawing of one body alone with an arrow for every force acting on it, and for nothing else.
- friction
- The force a rough surface exerts parallel to itself, opposing the sliding of a body along it. It has its own chapters later in this unit.
- inertia
- The tendency of a body to keep its velocity, at rest or in uniform motion. It is a property of the body, not a force.
- inertial frame
- A frame of reference in which Newton's first law holds; a frame that is not accelerating. The ground is one, to a very good approximation.
- mass
- The measure of a body's inertia, in kilograms. It is a scalar and does not depend on where the body is.
- net force
- The vector sum of all the forces acting on a body, \(\sum \vec F\).
- newton
- The SI unit of force. One newton gives a mass of one kilogram an acceleration of one metre per second squared: \(1\,\text{N} = 1\,\text{kg·m/s}^2\).
- non-contact force
- A force that acts across space without contact. In mechanics the only one is gravity.
- normal force
- The push of a surface on a body in contact with it, perpendicular to the surface. A surface can push but never pull.
- spring constant
- The force needed per unit extension of a spring, \(k = F/x\), in N/m. A stiff spring has a large \(k\).
- spring force
- The force a stretched or compressed spring exerts on whatever holds its end, directed towards its natural length.
- tension
- The pull of a string or rope on a body tied to it, along the string and away from the body.
- weight
- The gravitational pull of the Earth on a body, \(W = mg\), directed vertically downward.