Kinetic and Static Friction
Why this matters
Hey there. I'm Saavi, and we're going to tackle one of the most common forces you experience every day: friction.
Imagine you're helping your friend Maya move into a new apartment in Chicago. There's a heavy bookshelf you need to slide across the hardwood floor. You give it a small push. Nothing. You push a little harder. Still nothing. It feels like the floor is pushing back, refusing to let it budge. Finally, you give it one big shove, and it lurches into motion! And once it's moving, you might even notice it's a little easier to keep it sliding than it was to get it started.
That "stuck" feeling and the "drag" you feel while it's sliding? That's friction in a nutshell. We're about to break down exactly what's happening, why it's harder to start than to continue, and how to calculate these forces for your exam.
Diagram
Concept map
stateDiagram-v2
[*] --> AtRest
AtRest: Object is stationary
AtRest: f_s = F_app
AtRest --> Sliding: F_app > f_s,max
Sliding: Object is moving
Sliding: f_k = constant
Sliding --> AtRest: Object stops (v=0)
Core explanation
Friction might seem simple, but it has some important rules. Let's break them down so you're never caught off guard.
What Causes Friction?
On a microscopic level, no surface is perfectly smooth. Imagine zooming in on the bottom of that bookshelf and the floor. You'd see jagged peaks and valleys, like two mountain ranges grinding against each other. Friction is the force that arises from these microscopic imperfections interlocking and resisting motion.
This is also why the type of surfaces matters so much. Pushing a bookshelf on a polished wood floor is one thing; pushing it across a shaggy carpet is another entirely. The "roughness" and chemical properties of the surfaces determine how strongly they'll stick together.
Static Friction: The "Smart" Force
Static friction (f_s) is the force that prevents an object from starting to move. I call it the "smart" or "responsive" force because it only pushes back as hard as it needs to.
Think about the bookshelf again.
- If you push with 5 N of force and it doesn't move, the static friction force is pushing back with exactly 5 N. The net force is zero.
- If you increase your push to 30 N and it still doesn't move, static friction has matched you, pushing back with 30 N.
But there's a limit. Eventually, you'll push hard enough to overcome the interlocking microscopic hills and valleys. This limit is called the maximum static friction (f_s,max).
The rule for static friction is an inequality:
|F⃗_f,s| ≤ μ_s|F⃗_n|
Let's unpack this.
μ_sis the coefficient of static friction. It's a number with no units that represents the "stickiness" between two specific surfaces at rest. A higherμ_smeans more stickiness (like sneakers on a basketball court). A lowerμ_smeans less (like a puck on an air hockey table).F⃗_nis the Normal Force. This is the perpendicular force the surface exerts on the object. On a flat, horizontal surface with no other vertical forces,F_nis equal in magnitude to the object's weight (mg). But be careful! If you're pushing down on the box, or if it's on an incline,F_nwill be different.
Kinetic Friction: The Constant Drag
Once you overcome static friction and the object starts sliding, the type of friction changes to kinetic friction (f_k). This is the force that resists an object's motion when it's already moving.
Kinetic friction is simpler. It has a constant value for a given situation. As the microscopic peaks and valleys slide past each other, they don't have time to settle in and lock up as deeply. This means the kinetic friction force is almost always less than the maximum static friction force.
This is why it feels easier to keep the bookshelf moving than it was to start it!
The formula for kinetic friction is an equation, not an inequality:
|F⃗_f,k| = μ_k|F⃗_n|
μ_kis the coefficient of kinetic friction. It represents the "slipperiness" between two surfaces that are sliding against each other.- For any given pair of surfaces,
μ_kis typically less thanμ_s.
A common misconception is that friction depends on the surface area of contact. It doesn't! A wide tire and a narrow tire made of the same rubber on the same road will have the same frictional force, assuming the car's weight is the same. It's about the normal force and the nature of the surfaces, not how much area is touching.
Putting It All Together: The Friction Graph
Let's visualize the whole process with a graph. Imagine we are applying a steadily increasing force (F_app) to a heavy box and plotting the friction force that responds.
- 1Static Region (The Ramp Up)As we start pushing from 0 N, the static friction force perfectly matches our push. If we push with 2 N, it pushes back with 2 N. If we push with 8 N, it pushes back with 8 N. This is the diagonal line on the graph where
f_s = F_app. - 2The Breaking Point (The Peak)We keep pushing harder until we hit the maximum static friction,
f_s,max. In our graph's example, this happens when we apply 10 N of force. At this exact moment, the box is on the verge of moving. - 3The DropThe instant the box starts to slide, the friction switches from static to kinetic. Because
μ_k < μ_s, the friction force suddenly drops to a lower, constant value. In our example, it drops to 7 N. - 4Kinetic Region (The Plateau)As long as the box is sliding, the kinetic friction force remains constant at 7 N, no matter how much faster we push it. This is the flat, horizontal line on the graph.
Understanding this graph is crucial. It tells the entire story of friction in one picture.
Worked examples
Let's walk through a couple of problems together. The key is always to identify whether the object is moving or not first.
Will It Budge?
A 15 kg wooden crate rests on a wooden floor in a warehouse in Dallas. The coefficient of static friction μ_s between the wood surfaces is 0.5, and the coefficient of kinetic friction μ_k is 0.3. A worker, Priya, pushes horizontally on the crate with a force of 60 N.
(a) What is the magnitude of the friction force on the crate? (b) Will the crate move?
Step 1: Draw a Free-Body Diagram and Find the Normal Force. The forces acting on the crate are:
- Gravity (
F_g = mg) pulling down. - The Normal Force (
F_n) from the floor pushing up. - Priya's push (
F_app) horizontally. - Friction (
f) opposing the push.
Since the floor is horizontal and there are no other vertical forces, the upward and downward forces balance.
F_n = F_g = mg
F_n = (15 kg)(9.8 m/s²) = 147 N
Step 2: Determine the Maximum Static Friction.
Before we can know if it moves, we need to find the "breaking point."
f_s,max = μ_s * F_n
f_s,max = (0.5)(147 N) = 73.5 N
This is the most the floor can push back before the crate starts to slide.
Step 3: Compare the Applied Force to the Maximum Static Friction.
Priya is pushing with F_app = 60 N.
Our calculated maximum static friction is f_s,max = 73.5 N.
Since F_app < f_s,max (60 N is less than 73.5 N), the crate will not move.
Step 4: Answer the Question. (a) Because the crate doesn't move, the static friction force is simply matching Priya's push. Therefore, the friction force is 60 N. (b) No, the crate will not move.
Common mistake here: Many students would immediately calculate f_s,max (73.5 N) and say that's the friction force. Remember, static friction is responsive! It only uses as much force as it needs.
Calculating Acceleration
Let's say Priya gets her coworker, Carlos, to help. Together, they push the same 15 kg crate with a combined horizontal force of 90 N. What is the acceleration of the crate?
Step 1: Check if the Crate Moves.
From Example 1, we know the maximum static friction is f_s,max = 73.5 N.
Their applied force is F_app = 90 N.
Since F_app > f_s,max (90 N is greater than 73.5 N), the crate will move and accelerate.
Step 2: Calculate the Kinetic Friction Force.
As soon as the crate starts sliding, the friction switches to kinetic friction.
f_k = μ_k * F_n
f_k = (0.3)(147 N) = 44.1 N
This is the constant frictional force acting on the crate as it slides.
Step 3: Apply Newton's Second Law (ΣF = ma).
We'll look at the net force in the horizontal direction. The applied force pushes it forward, and kinetic friction pushes back.
ΣF_x = F_app - f_k = ma_x
90 N - 44.1 N = (15 kg) * a_x
45.9 N = (15 kg) * a_x
Step 4: Solve for Acceleration.
a_x = 45.9 N / 15 kg
a_x = 3.06 m/s²
The crate accelerates forward at 3.06 m/s².
Try it yourself
Ready to try a couple on your own? Don't just jump to the answer; walk through the steps we just practiced.
- 1The Stubborn File CabinetA 40 kg metal file cabinet stands on a tile floor in an office in Boston. It takes a horizontal push of at least 235 N to get the cabinet to start moving. What is the coefficient of static friction,
μ_s, between the cabinet and the floor?- Hint: The phrase "at least 235 N to get... moving" is telling you the value of the maximum static friction. Use that to work backward.
- 2Sledding in the ParkAaliyah is pulling her little brother on a sled across a snowy field in Seattle. The sled is moving at a constant velocity. The combined mass of her brother and the sled is 30 kg, and the coefficient of kinetic friction is 0.1. What is the magnitude of the force Aaliyah is pulling with?
- Hint: What does "constant velocity" tell you about the net force and acceleration? How must the pulling force relate to the kinetic friction force?
Practice — 8 questions
In simple terms, friction is a force that resists sliding between surfaces. It can be static (preventing movement) or kinetic (opposing movement).
- 2.7.A: Describe kinetic friction between two surfaces.
- 2.7.B: Describe static friction between two surfaces.
- 2.7.A.1
- Kinetic friction occurs when two surfaces in contact move relative to each other.
- 2.7.A.1.i
- The kinetic friction force is exerted in a direction opposite to the motion of each surface relative to the other surface.
- 2.7.A.1.ii
- The force of friction between two surfaces does not depend on the size of the surface area of contact.
- 2.7.A.2
- The magnitude of the kinetic friction force exerted on an object is the product of the normal force the surface exerts on the object and the coefficient of kinetic friction. Relevant equation: |F⃗_f,k| = μ_k|F⃗_n|
- 2.7.A.2.i
- The coefficient of kinetic friction depends on the material properties of the surfaces that are in contact.
- 2.7.A.2.ii
- Normal force is the perpendicular component of the force exerted on an object by the surface with which it is in contact; it is directed away from the surface.
- 2.7.B.1
- Static friction may occur between the contacting surfaces of two objects that are not moving relative to each other.
- 2.7.B.2
- Static friction adopts the value and direction required to prevent an object from slipping or sliding on a surface. Relevant equation: |F⃗_f,s| ≤ μ_s|F⃗_n|
- 2.7.B.2.i
- Slipping and sliding refer to situations in which two surfaces are moving relative to each other.
- 2.7.B.2.ii
- There exists a maximum value for which static friction will prevent an object from slipping on a given surface. Derived equation: F_f,s,max = μ_sF_n
- 2.7.B.3
- The coefficient of static friction is typically greater than the coefficient of kinetic friction for a given pair of surfaces.
stateDiagram-v2
[*] --> AtRest
AtRest: Object is stationary
AtRest: f_s = F_app
AtRest --> Sliding: F_app > f_s,max
Sliding: Object is moving
Sliding: f_k = constant
Sliding --> AtRest: Object stops (v=0)
Read what Saavi narrates
Hey there. I'm Saavi, and we're going to tackle one of the most common forces you experience every day: friction.
Imagine you're helping a friend move a heavy bookshelf. You give it a small push. Nothing. You push a little harder... still nothing. It feels like the floor is pushing back. Finally, you give it one big shove, and it lurches into motion! And once it's moving, you might notice it's a little easier to keep it sliding.
That "stuck" feeling and the "drag" you feel while it's sliding? That's friction. We're about to break down exactly what's happening. We'll explore the two main types: static friction, the stubborn force that keeps things from starting to slide, and kinetic friction, the drag force that acts on things that are already moving.
Let's try a problem. A 15 kilogram crate rests on a floor. The coefficient of static friction is 0.5. A worker, Priya, pushes horizontally with a force of 60 Newtons. Will the crate move?
First, let's find the normal force. Since it's on a flat floor, the normal force equals the weight, which is mass times gravity. So, 15 kilograms times 9.8 meters per second squared gives us 147 Newtons.
Next, let's find the maximum possible static friction... the breaking point. We multiply the coefficient of static friction, 0.5, by the normal force, 147 Newtons. That gives us 73.5 Newtons. This is the most the floor can resist.
Priya is only pushing with 60 Newtons, which is less than the maximum of 73.5. So, the crate will not move. And the friction force pushing back is exactly 60 Newtons, perfectly matching her push.
Now, here's the biggest mistake I see students make every single year. They automatically use the formula for maximum static friction for any static problem. They would have calculated 73.5 Newtons and called that the answer. But remember, static friction is responsive. It only pushes back as hard as it needs to. It's a smart force!
Keep that in mind as you practice. You've got this.
This formula calculates the *maximum* possible static friction, not the actual force. The actual static friction force is equal and opposite to the applied force, up until that maximum is reached.
First, calculate `f_s,max`. Then, compare it to the applied force. If `F_app < f_s,max`, then the actual static friction `f_s` is simply equal to `F_app`.
`F_n` is the perpendicular force from a surface. If the object is on an incline, or if there's another force pushing down or pulling up on the object, `F_n` will not be equal to `mg`.
Always draw a free-body diagram and solve for `F_n` by setting the sum of the forces perpendicular to the surface equal to zero (assuming no acceleration in that direction).
Once an object is sliding, kinetic friction takes over, which is governed by `μ_k`. Since `μ_k` is usually smaller than `μ_s`, you'll get the wrong friction force and the wrong acceleration.
If the object is moving, use `f_k = μ_k * F_n`. If it's stationary, you'll be dealing with `f_s`.
For the scope of AP Physics 1, the friction force depends only on the coefficient of friction and the normal force. A wider box doesn't have more friction than a narrow one of the same weight. Kinetic friction is also modeled as constant, regardless of speed.
Focus only on the two factors in the friction equations: the coefficient (`μ`) and the normal force (`F_n`).