Newton's First Law
The Law of Inertia
Understand why objects at rest stay at rest and objects in motion keep moving: the foundational principle of inertia and net force.
What Is Inertia?
Inertia is the natural tendency of an object to resist changes in its state of motion. An object at rest wants to stay at rest, and an object moving at constant velocity wants to keep moving at that velocity.
Understanding Net Force
The net force on an object is the vector sum of all forces acting on it. When we write \(\vec{F}_{\text{net}}\), we mean the single force that would produce the same effect as all forces combined.
Why Does Newton's First Law Matter?
The Formal Statement
Mathematically, Newton's First Law states:
The converse is equally important: if an object's velocity is changing, there must be a nonzero net force acting on it.
Equilibrium in a Free-Body Diagram
Two Cases of First Law
Inertia vs. Force
| Inertia | Force | |
|---|---|---|
| Definition | Resistance to change in motion | A push or pull on an object |
| Depends on | Mass only | Interaction between objects |
| Units | kg (measured by mass) | Newtons (N) |
| Vector? | No (scalar property) | Yes (magnitude + direction) |
| Role in 1st Law | Why objects resist acceleration | What causes acceleration |
How to Apply Newton's First Law
Example 1: Book on a Table
Example 2: Constant Velocity Car
A car travels at a steady \(25 \text{ m/s}\) on a straight highway. The engine provides a forward force of \(3000 \text{ N}\). What is the total resistive force (air drag + friction)?
Example 3: Hanging Sign in Equilibrium
A \(15 \text{ kg}\) sign hangs from two cables making angles of \(30^\circ\) and \(45^\circ\) with the horizontal. Find the tension in each cable.
Inertial Reference Frames
Newton's First Law only holds in an inertial reference frame: a frame of reference that is not accelerating. If your frame accelerates, "fictitious forces" appear.
First Law vs. Second Law
| First Law | Second Law | |
|---|---|---|
| Condition | \(\sum \vec{F} = 0\) | \(\sum \vec{F} \neq 0\) |
| Result | \(\vec{a} = 0\), constant \(\vec{v}\) | \(\vec{a} = \frac{\sum \vec{F}}{m}\) |
| Tells us | What happens with no net force | How much acceleration a net force causes |
| Key use | Equilibrium problems | Dynamics problems |
Common Mistakes
Question 1 of 5
A hockey puck slides across frictionless ice at a constant speed of \(5 \text{ m/s}\). What is the net force acting on the puck?
Question 2 of 5
An astronaut floating in the International Space Station releases a ball. In the station's reference frame, the ball:
Question 3 of 5
A box sits at rest on a rough floor. A person pushes it with a horizontal force of \(40 \text{ N}\), but it does not move. What can you conclude about the friction force?
Question 4 of 5
Which of the following is an example of Newton's First Law in action?
Question 5 of 5
A skydiver reaches terminal velocity and falls at a constant \(55\) m/s. At terminal velocity, the net force on the skydiver is: