We encounter friction in our daily lives; take the wearing-off of your slipper soles for example. Or even the grip between your bike tyres and the road, which is required for the wheel to rotate and for you to cycle forward.
There are also fluid friction (e.g. swimming through water and slowing down when you stop propelling yourself) and internal friction (e.g. a swinging pendulum stopping by itself eventually). In statics, we will be focusing on dry friction.
Dry friction is caused by the contact between 2 surfaces, due to the unevenness of the surface at the micro-scale. Even 2 pieces of glass (which might seem smooth) have friction if you put them together
We encounter friction in our daily lives; take the wearing-off of your slipper soles for example. Or even the grip between your bike tyres and the road, which is required for the wheel to rotate and for you to cycle forward.
There are also fluid friction (e.g. swimming through water and slowing down when you stop propelling yourself) and internal friction (e.g. a swinging pendulum stopping by itself eventually). In statics, we will be focusing on dry friction.
Dry friction is caused by the contact between 2 surfaces, due to the unevenness of the surface at the micro-scale. Even 2 pieces of glass (which might seem smooth) have friction if you put them together
There are two types of dry friction:
Static friction – this friction applies when an object is stationary. It is calculated using:
μs is the coefficient of static friction and N is the normal force acting on the friction contact surface. The “≤” sign means that it can go up to a maximum value of Ff,max = μsN.
It is presented this way because the static friction force only serves to counter the action force to prevent motion, and in some cases a force of less than μsN is adequate. However when the action force exceeds μsN then we have kinetic friction instead.
Kinetic friction – this is the frictional resistive force that acts on the object as long as it is in motion and in contact with the friction surface. It is calculated using:
μk is the coefficient of kinetic friction and N is the same normal force. Typically μk is less than μs.
Are there only two simple equations in this topic? Is this too good to be true? Yes and no… =(
The key to this topic is constructing the correct FBD with all forces identified, and determining whether the frictional force is Ff = μsN or Ff < μsN, or whether it switches to kinetic friction (Ff = μkN).
Let’s look at an example now.
There are two types of dry friction:
Static friction – this friction applies when an object is stationary. It is calculated using:
μs is the coefficient of static friction and N is the normal force acting on the friction contact surface. The “≤” sign means that it can go up to a maximum value of Ff,max = μsN.
It is presented this way because the static friction force only serves to counter the action force to prevent motion, and in some cases a force of less than μsN is adequate. However when the action force exceeds μsN then we have kinetic friction instead.
Kinetic friction – this is the frictional resistive force that acts on the object as long as it is in motion and in contact with the friction surface. It is calculated using:
μk is the coefficient of kinetic friction and N is the same normal force. Typically μk is less than μs.
Are there only two simple equations in this topic? Is this too good to be true? Yes and no… =(
The key to this topic is constructing the correct FBD with all forces identified, and determining whether the frictional force is Ff = μsN or Ff < μsN, or whether it switches to kinetic friction (Ff = μkN).
Let’s look at an example now.