Often times an object we are trying to analyze with FBDs sits atop a surface that is not parallel to the ground. This slight variation adds some noteworthy complexities that we will cover in this section.

Inclined planes can be used for mechanical advantage. It is considered a Simple Machine.

https://www.youtube.com/watch?v=igrMlzHL-qg

Pre-lecture Study Resources

Read the BoxSand Introduction and watch the pre-lecture videos before doing the pre-lecture homework or attending class. If you have time, or would like more preparation, please read the OpenStax textbook and/or try the fundamental examples provided below.

BoxSand Introduction

Forces  | Inclined Planes

Objects on a non-horizontal surface are considered to be on an inclined plane. If they slide up or down the incline their acceleration is not horizontal. Some forces acting on the object, with the normal force being an example, are off at an angle and not straight vertical (or horizontal). This presents a unique example of a system where rotating your coordinate system is beneficial to the analysis. Consider the block below and think about the direction of forces acting on it. Using a standard horizontal and vertical coordinate system (not pictured), you would have to break the tension and normal force into components. Furthermore, If the block was accelerating, without flying off the incline or falling through it, the block's acceleration would be along the incline, off at an angle from the horizontal. The acceleration would also have to be broken into components. To illustrate how cumbersome this choice of coordinate system makes the calculation, consider the case where the hanging mass is not large enough to hold the block and it is accelerating down the incline. Newton's 2nd law would look as follows with a standard positive x to the right and positive y upward. Note: the open resource diagram below doesn't use the letter F for all the forces like we encourage you do.

$\sum\overrightarrow{F}= m \overrightarrow{a} \rightarrow$      $\langle T\cos{\alpha}-N\cos{\alpha}, T\sin{\alpha}+N\sin{\alpha}-F_g\rangle = m \langle -a\cos{\alpha},-a\sin{\alpha} \rangle$

This is an image of a block on a ramp at some angle alpha that is connected by a string on the right side of the block of mass m one with a pulley system that is connected by a bucket with some mass m two. The force body diagram of the block with mass m one shows the normal force perpendicular to the surface, the force of gravity straight down broken into its x and y components and the force of tension parallel up the ramp. The x and y axis system is rotated so that the x axis is parallel to the ramp and positive x pointing down the ramp. The free body diagram of the bucket with mass m two has a tension force going up and a force of gravity going down. The x and y coordinates are rotated in a way that shows the x axis is parallel to the two forces with positive x going up.

What if instead of using a horizontal and vertical coordinate system you were to define one where the positive x direction pointed parallel to the incline, as shown in the figure. Now the tension and the normal force, are 100% in the x direction. Movement along the incline will now be along the x direction and so will the any acceleration. The only thing then that needs to be broken into components is the force of gravity. Newton's 2nd law is reduced to the following.

$\sum \overrightarrow{F} = m \overrightarrow{a} \rightarrow$      $\langle F_g\sin{\alpha}-T, N-F_g\cos{\alpha}\rangle = m \langle a,0 \rangle$

The algebra and arithmetic will be much easier using a rotated coordinate system. The biggest issue it to figure out what the new x and y components are for a rotated system. Watch my lecture video for a technique to get the components correct in a rotated coordinate system. Once you've done it a few times, I believe you'll agree the work to learn how to rotate the coordinate system is worth the savings in algebra headaches of not rotating your coordinate system. If you're still not convinced, imagine having to then do kinematics problems with the acceleration you have just calculated doing a force analysis. With a standard coordinate system it is a 2D problem and you'll have a set of kinematic equations for both the x and y directions. With a rotated coordinate system, assuming the object doesn't leave the incline, the velocity, acceleration, and change in position are zero in the direction perpendicular to the plane, making it a 1D problem.

Here's a short video to visualize the components of gravitational force (they use the letter P), and the normal force (N).

Inclined Plane Gif

Key Equations and Infographics

Now, take a look at the pre-lecture reading and videos below.

BoxSand Videos

OpenStax Reading

OpenStax Section 4.5  |  Normal, Tension, and Other Examples of Forces

Openstax College Textbook Icon

Fundamental examples


1. Consider consider a $1.5 \, kg$ object on a frictionless incline as shown in the image below. If the magnitude of $\vec{F}^A$ is equal to $8 \, N$ and the angled labeled is $60^{\circ}$, what is the acceleration of the object?

This image shows a block with mass m on a ramp with angle theta and an applied force that pushes the block up the ramp.

2. Lombard Street in San Francisco, uses a curvy road to help mitigate the steep hill that cars must travel down. If approximated as an incline plane, Lombard Street roughly makes a $27^{\circ}$ incline with respect to the horizontal.

a) Find the force of static friction if the coefficient of static ($\mu_s$) friction between Lombard Street and a car's tires is $0.70$. The car has a mass of $1381 \, kg$.

b) What is the minimum value that $\mu_s$ can be before your car starts to slip down the street?

CLICK HERE for solutions.

Short foundation building questions, often used as clicker questions, can be found in the clicker questions repository for this subject.

Clicker Questions Icon


 

Post-Lecture Study Resources

Use the supplemental resources below to support your post-lecture study.

Practice Problems

BoxSand's Quantitative Practice Problems

BoxSand's Multiple Select Problems

 

Recommended example practice problems 

BoxSand Practice Problems

Solutions to BoxSand Practice Problems

Set 1: Normal Forces interactive set/quiz

Set 2: SledSled 2: The Friction Strikes BackMountain Road

For additional practice problems and worked examples, visit the link below. If you've found example problems that you've used please help us out and submit them to the student contributed content section.

For additional practice problems and worked examples, visit the link below. If you've found example problems that you've used please help us out and submit them to the student contributed content section.

Example Problems Icon

Additional Boxsand Study Resources

Additional BoxSand Study Resources

Learning Objectives

Summary

Inclined planes are a physical situation where students must wrestle with a non-traditional coordinate system and the vector components in that system.

Atomistic Goals

Students will be able to...

  1. Identify the direction of acceleration and weigh the value of aligning your coordinate system with that direction as opposed to choosing one that minimizes the number of force components.
  2. Orient the forces in a FBD in the direction they are applied and not rotated to align with a horizontal or vertical direction.
  3. Translate a given angle in the physical representation to all like angles in a FBD, which may require geometry.

 

Equations, definitions, and notation icon Concept Map Icon
Key Terms Icon Student Contributed Content Icon

Additional Study Resources

Use the supplemental resources below to support your post-lecture study.

YouTube Videos


Khan Academy explains inclined plan force components you may see when solving inclined plane problems:

https://www.youtube.com/watch?v=TC23wD34C7k

This is a simple introduction to motion on an inclined plane with no friction:

https://www.youtube.com/watch?v=Mz2nDXElcoM

Doc Schuster describes techniques for solving inclined plane problems

https://www.youtube.com/watch?v=BEyWcYG5g68

This a short video lecture by APlusPhysics on Ramp and Inclines;

https://www.youtube.com/watch?v=j8R9PS_sVP8

https://www.youtube.com/watch?v=vQqB_MBVPXw

Simulations


This phet simulation highlights the physics when working with inclined planes.

Phet Interactive Simulations Icon

For additional simulations on this subject, visit the simulations repository.

Simulation Icon

Demos


 For additional demos involving this subject, visit the demo repository

Demos Icon

History


Oh no, we haven't been able to write up a history overview for this topic. If you'd like to contribute, contact the director of BoxSand, KC Walsh (walshke@oregonstate.edu).

Physics Fun


Oh no, we haven't been able to post any fun stuff for this topic yet. If you have any fun physics videos or webpages for this topic, send them to the director of BoxSand, KC Walsh (walshke@oregonstate.edu).

Other Resources


Physics Classroom: Inclined planes

The Physics Classroom Icon

In addition to the textbook above be sure to read the EasyPhysics Inclined Plane with Gravity section which describes decomposed forces on an inclined plane a little differently.

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Resource Repository

This link will take you to the repository of other content on this topic.

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Problem Solving Guide

Use the Tips and Tricks below to support your post-lecture study.

Assumptions

Remember that inclined plane problems are just tilted standard problems, so the same rules apply, i.e. draw a FBD, sum forces, set equal to ma, solve for forces/acceleration and analyze motion.

In these problems, it is often useful to align your axes with your inclined plane, this will result in the normal force and friction force (if any) will be on axis, but gravitational force and other forces will often need to be decomposed into vectors that point along our new axes.

Checklist

 

Misconceptions & Mistakes

  • Oftentimes in physics the angle given is not the angle you need to use in the problem. Do not assume, check the angle is correct, especially on exams.

 

  • Position and velocity have no bearing on acceleration, which takes its cues from forces on the system. Forces tell objects how to accelerate, acceleration tells velocity how to change, velocity tells position how to change. Acceleration is the ultimate root of motion, brought about by force interactions.

 

 

Pro Tips

  • Remember that all equations you can derive on an inclined plane should reduce to a flat plane if you set the angle of the plan to 0. Oftentimes they will also reduce to free fall if you set the angle of the plane to 90 degrees we well! Use these types of checks to see if your equations make sense!.
  • Often one of the most challenging parts of an inclined plane is translating the angle given into your equations. One of the best ways to make this easier is to find the angle of the incline as it relates to one of your vectors, then draw a traditional horizontal axis and a vertical axis. Then, draw axes that align with your inclined plan, one along the inclined plane and normal  (pointing directly perpendicular) to it. Now, using these two sets of lines, you can say that every OTHER angle between those lines is the same (so only 2 unique angles are found between the lines). You can easily fill in the angles from there after knowing only 1. This is known as the pizza wedge tick, take a look below:
  • You still want to align your sum of forces to point in the direction of acceleration, which is usually pointing down or up the inclined plane (and acceleration is usually 0 perpendicular to the plane), so generally speaking you'll usually tilt your axes the same angle that the inclined plane is at, expect in a few notable cases where acceleration is NOT along these axes (uniform circular motion has some instances of this that will come later!).

 

Multiple Representations

Multiple Representations is the concept that a physical phenomena can be expressed in different ways. 

Physical


Physical Representations describes the physical phenomena of the situation in a visual way.

 This image shows two scenarios of an object moving. Each image shows a variety of forces acting on the object denoted as arrows and the kind of force and the direction that it acts on the object. There is also an arrow showing the direction of the net force which also shows the direction of acceleration. Each image shows a free body diagram of all of the forces that is acting on the object to show a physical representation of all of the forces as well as their magnitudes and direction.

Mathematical


Mathematical Representation uses equation(s) to describe and analyze the situation.

The main mathematical representation for forces will be applying Newton's Second Law to a physical problem. You will need to analyze the motion of an object and create a free body diagram of the relative forces in order to derive the force equations. We learned in the kinematics section how to analyze motion without any concern about the forces that caused the motion. The infographic below describes the relationship between force and acceleration. Thus, we may now analyze the forces acting on an object to determine the relative acceleration.

A representation with the words newton's second law (n.two.l) on the top. There is an equation that shows that the sum of all of the forces external to the system, acting on the system, is equal to the mass of the system multiplied by the acceleration of the center of mass of the system. This is also written in words below with the note that says that this equation contains vector and scalar quantities.

 

Graphical


Graphical Representation describes the situation through use of plots and graphs.

An image that shows the position over time, velocity over time and acceleration over time graphs of three scenarios of a stationary object, uniform motion (constant velocity) and motion with a constant acceleration. This is to show that we can use different situations of changing position, velocity or acceleration to show the movement of an object over time. .

Descriptive


Descriptive Representation describes the physical phenomena with words and annotations.

 A spaceship, deep in space, has ran out of fuel. Since nothing is there to act on the ship, it will continue to move at the speed it is moving and in the direction it is moving. It will do this until something acts on it, something like the pull from a nearby star that becomes no longer negligible as the ship passes near the star.

Experimental


Experimental Representation examines a physical phenomena through observations and data measurement.

 

Here is a great video of an experiment where a pen cap is dropped into a bottle using Newton's first law

https://www.youtube.com/watch?v=uOSBC0SXVR4