2.1 - Force on +z and −z Plane
Enroll to start learning
You’ve not yet enrolled in this course. Please enroll for free to listen to audio lessons, classroom podcasts and take practice test.
Interactive Audio Lesson
Listen to a student-teacher conversation explaining the topic in a relatable way.
Understanding the Traction Vector
🔒 Unlock Audio Lesson
Sign up and enroll to listen to this audio lesson
Today, we're going to explore the concept of traction vectors on the +z plane. Can anyone tell me what a traction vector represents?
Isn't it the force per unit area acting at a point on a surface?
Exactly! And in a cylindrical coordinate system, the traction vector on the +z plane can be expressed as: `t+z = σ e + τ e + τ e`. Does anyone remember what these components represent?
I think `σ` is normal stress, while `τ` represents shear stress components.
Good memory! We’ll check these components as we go deeper into the calculations.
Calculating Forces on the +z Plane
🔒 Unlock Audio Lesson
Sign up and enroll to listen to this audio lesson
Next, let’s look at how we calculate the total force on the +z plane by integrating the traction vector over the area. Can anyone describe how we approach the integration?
Do we start with an infinitesimal area element and then integrate it over the total area?
Correct! The area element on the +z plane is `dA = (r+ξ) dξ dη`. Now, can anyone explain why we use this expression for the area element?
Because `dA` needs to account for the radial distance multiplied by the small angle sweep in the direction.
Great explanation! Now we’ll use this area element to find the total force on the +z plane.
Forces on the -z Plane
🔒 Unlock Audio Lesson
Sign up and enroll to listen to this audio lesson
Now let's move to the -z plane. Who can share what changes when calculating the force on this plane compared to the +z plane?
The traction components would act in the negative direction, right?
Exactly! If the coordinates for a point on -z are `(r+ξ, θ+η, z - ∆z)`, we express the total force considering both the negative components and the integration over the area again. Always remember: the direction of the vectors matters!
So, when we do this for both planes, we can combine them to examine the overall forces, right?
Yes! That's an essential step when we derive the linear momentum balance.
Introduction & Overview
Read summaries of the section's main ideas at different levels of detail.
Quick Overview
Standard
In this section, we derive and analyze the forces acting on the upper (+z) and lower (-z) planes of a cylindrical element. It includes the definitions of traction vectors and their integration over these planes to formulate the total forces acting on them, crucial for understanding linear momentum balance in cylindrical coordinates.
Detailed
Detailed Summary
In this section, we focus on the forces acting on the +z and -z planes in a cylindrical coordinate system. The traction vector on the +z plane, represented as t+z, is defined using the stress components acting on this plane. The total force acting on the +z plane is calculated by integrating the traction vector over its defined area.
We start with the traction vector:
$$
t_{+z} = au_{zz} e_z + au_{rz} e_r + au_{ heta z} e_{ heta}$$
where σ, τ represent various stress components.
To find the total force on the +z plane, we consider an infinitesimal area element dA, factor in both the radial and angular dimensions, and subsequently perform the integration to yield the resultant force. We repeat a similar process for the -z plane, noting that the traction components will be directed negatively.
Finally, by combining forces from both planes, we set up for further derivation of the linear momentum balance. This section sets the groundwork for understanding the dynamics of cylindrical structures in applied mechanics.
Audio Book
Dive deep into the subject with an immersive audiobook experience.
Traction Vector on +z Plane
Chapter 1 of 3
🔒 Unlock Audio Chapter
Sign up and enroll to access the full audio experience
Chapter Content
On +z plane, the traction vector (t+z) is given by
$$t_{+z} = \sigma_{zz} e_z + au_{rz} e_r + au_{ heta z} e_{ heta}$$ (1)
Detailed Explanation
In this section, we start by discussing the traction vector acting on the +z plane of a cylindrical element. The notation used represents the different components of the traction vector: σ is the normal stress in the z-direction, τ represents shear stresses, and e indicates the unit basis vectors in their respective directions. Basically, this equation describes how forces act on this plane, which is essential for understanding how stress affects the material.
Examples & Analogies
Imagine pressing down on a sponge with your hand. The pressure you apply creates a force (the traction vector) in the vertical direction (upwards or downwards). In our case, the sponge represents the cylindrical element, where your hand applies force in different directions, similar to how stress vectors interact within the element.
Calculating Total Force on +z Plane
Chapter 2 of 3
🔒 Unlock Audio Chapter
Sign up and enroll to access the full audio experience
Chapter Content
The total force due to this traction can be obtained by integrating it over +z plane. The difference between the outer and inner radius of this face is \( \Delta r \) and the total angle subtended by the face at the center is \( \Delta \theta \). The coordinates of a general point on the top surface is denoted by \( (r + \xi, \theta + \eta, z) \) (where r and θ coordinates vary while the z coordinate remains fixed). Thus, the area of the infinitesimal element is:
$$dA = d\xi \times (r + \xi) d\eta = (r + \xi) d\xi d\eta$$ (2)
Detailed Explanation
Next, we calculate the total force acting on the +z plane by integrating the traction vector over the area of the plane. To do this, we need to specify how the coordinates change across the top surface of the cylinder and define an infinitesimal area (dA). This area is calculated based on the radial and angular changes, represented by dξ and dη, giving us a clear geometric representation of how we consider the area for our force calculations.
Examples & Analogies
Think about a pizza cutter slicing through a pizza. The area where the cutter applies pressure (traction) can be thought of as dA. As you move the cutter (analogous to integrating over the area), you compute the total force exerted on the pizza (total force on +z plane). As the cutter moves, it exposes more area for the pressure to act upon—this is similar to how we compute total force over the cylindrical element.
Total Force on −z Plane
Chapter 3 of 3
🔒 Unlock Audio Chapter
Sign up and enroll to access the full audio experience
Chapter Content
For −z plane, all the traction components act along negative basis directions but an arbitrary point on −z plane will have coordinates \( (r + \xi, \theta + \eta, z - \Delta z) \). Thus, the total force on −z plane will be...
Detailed Explanation
On the −z plane, the situation is similar, but the traction components act in the opposite direction. The coordinates of a point on this plane are adjusted to reflect the change in the z component, indicating we're effectively looking at the forces acting downwards, as the negative basis directions come into play. Although the tensions and coordinates are transformed, they are analyzed similarly to those on the +z plane.
Examples & Analogies
Returning to our sponge analogy, if you now pull the sponge in an upward motion, the force applied from below (like your fingers) creates a different effect than if you apply downward pressure. The angle and direction of those forces change significantly, similar to how we analyze different planes in cylindrical coordinates.
Key Concepts
-
Traction Vector: A force per unit area acting on the surface.
-
Integration over Area: The process to calculate total force by summing contributions from infinitesimal area elements.
-
Cylindrical Coordinate System: A system useful for analyzing objects with cylindrical geometry.
Examples & Applications
A force distributed across the cross-section of a pipe, calculated using integration over the cylindrical surface area.
Forces on the +z plane of a cylindrical structure, derived using the traction vector integrated over defined area.
Memory Aids
Interactive tools to help you remember key concepts
Rhymes
Traction vector's the force we collect, on surfaces it's what we detect.
Stories
Imagine a cylindrical tin. On the top, the force acts strong. On the bottom, it’s just as wrong. Forces accumulate, as we integrate, making movement, we illustrate.
Memory Tools
To remember the steps: T-I-F — Traction, Integrate, Force!
Acronyms
T-FAC
Traction For Area Calculation for radial and angular contributions.
Flash Cards
Glossary
- Cylindrical Coordinate System
A three-dimensional coordinate system defined by the distance from a fixed axis and the angle around that axis.
- Traction Vector
A vector that represents the force per unit area acting on a surface.
- Infinitesimal Area Element
A differential element of area used in calculus to perform integration over a surface.
- Stress Components
Components of stress, including normal stress and shear stress, that describe the internal forces acting within a material.
Reference links
Supplementary resources to enhance your learning experience.