Info on forces and strains required and produced.

Slides:



Advertisements
Similar presentations
Angular Quantities Correspondence between linear and rotational quantities:
Advertisements

Torque Chapter 8 Section 1.
Lever, Wheel and Axle, & Pulley
Newton’s Laws of Motion (and force!!) A force is a push or pull on an object.
Fluid Mechanics 2 – Hydrodynamics: Propulsion
Inverse Proportion. When a Lever is Balanced... The torques are equal F ∙ d = F ∙ d 80 g ∙ 25 cm = 100 g ∙ 20 cm 2000 g cm = 2000 g cm English: g-cm (hyphen)
Pharos University ME 352 Fluid Mechanics II
How To Build A Water Rocket
Equilibrium and Elasticity
Lesson 36 Torque and Drag Calculations
Chapter 9: Torque and Rotation
(W= weight!) W = m  g The main force acting on the body is the gravitational force! Gravitational force W applies at the center of gravity CG of the.
Torque Rotational Motion. Torque  Forces that cause objects to rotate  Two Characteristics that contribute to the effectiveness of torque: Magnitude.
DETERMINATION OF TORQUE
Causing Rotational Motion In order to make an object start rotating about an axis, a force is required However, not only the amount of force applied but.
Torque.
 Point at which all other points on the object rotate around  During motion the CM will move in the same path that a simple particle would move if subjected.
Mechanical Force Notes
Wire and rod drawing.
Warm-Up: February 17, 2015 Write down a definition for equilibrium.
In the analysis of a tilting pad thrust bearing, the following dimensions were measured: h1 = 10 mm, h2 = 5mm, L = 10 cm, B = 24 cm The shaft rotates.
Bowling Balls - Qualitative a)The ball begins by sliding; kinetic friction dissipates energy and reduces v. A small amount of rotation begins immediately.
Forces, Planes and propellers. Topic 1: Forces A force is any influence that can change the trajectory, speed or shape of a body. Effects produced by.
Mousetrap Cars Unit 11.
Mousetrap Car A mousetrap car is a vehicle designed to run on the energy that can be stored in a wound up mousetrap spring. Basic design: - Attach a string.
Levers.
Lecture 7 Rolling history, practice and categories and flat Rolling  Course Hour: 2  Basic requirements: Acquainting with rolling history, practice and.
Mechanisms Simple Machines
Bio-Mechanics Force in and on the BODY Medical Physics.
Team P14029: McKibben Muscle Robotic Fish
1 4 outline Newton’s 2 nd Law friction dynamics of falling objects RQ: 1, 2, 3, 4, 5, 6, 8, 11, 13, 14, 16, 18, 20, 21, 24, 26, 27, 30, 31, 33. Ex: 2,
General Question Test format: What types of questions should we expect? 7 multiple choice questions (5 points each) Short problems (similar to previous.
1. Objects at rest will stay at rest, and objects in motion will stay in motion in a straight line, unless acted upon by an unbalanced force.
3.3 Performance Appraisal Fluid Mechanics 2 – Hydrodynamics: Propulsion.
Physics. Simple Harmonic Motion - 3 Session Session Objectives.
Rotational Dynamics Causes of rotational motion! Analogies between linear & rotational motion continue. Newton’s 3 Laws are still valid! But, here we write.
Copyright © 2009 Pearson Education, Inc. Chapter 5 Using Newton’s Laws: Friction, Circular Motion, Drag Forces.
Unit 1: Fluid Dynamics An Introduction to Mechanical Engineering: Part Two Fluid dynamics Learning summary By the end of this chapter you should have learnt.
Rotational Motion and Equilibrium
8.2 Rotational Dynamics How do you get a ruler to spin on the end of a pencil? Apply a force perpendicular to the ruler. The ruler is the lever arm How.
Mechanisms Simple Machines Lever, Wheel and Axle, & Pulley.
Rolling Motion. Without friction, there would be no rolling motion. Assume: Rolling motion with no slipping  Can use static friction Rolling (of a wheel)
Chapter 4.2 Notes Resistance in Fluids. When one solid object slides against another, a force of friction opposes the motion. When one solid object.
 With a large perpendicular force and a small parallel force, the tendency to slide is very small. An example of this would be a 15 degree slope. The.
Rotational Motion AP Physics C. Definitions and Formulas.
Chapter Nine: Simple Machines
Airfoils, Lift and Bernoulli’s Principle
Proportionality. Direct Proportionality What is it? Direct proportionality is when one thing is directly proportional to another. Two quantities are in.
Power transmission.
What Are Gears? What Do They Do?. 1. What is a gear? A gear is a wheel with teeth that meshes together with other gears and is usually made of metal or.
How do you start the rotation of an object? How do you open an door? What did we learn about the best way to open a door? The most efficient way to open.
VEX IQ Curriculum Key Concepts Lesson 06 Lesson Materials:
CHAPTER 2 Mechanical Principles: Kinetics
Mechanisms-Simple Machines
Mechanical Systems Unit Review
Physics Section 7.4 Calculate the torque generated by a force.
How to calculate the torque due to the balance stick
Rotational Motion: Torque, Angular Inertia and Newton’s Laws
Mechanical Advantage Simple Machines.
Torque.
Chapter Nine: Simple Machines
Mechanisms-Simple Machines
Momentum, Gravity & Equilibrium
Bell Work: Centripetal Motion
VEX IQ Curriculum Key Concepts Lesson 06 Lesson Materials:
Chunk 5 Application of Newton’s Laws
Lesson 8-2 Formulas Circumference Arc Length Area Sector.
Chapter 8 Rotational Equilibrium and Dynamics
Section 8, Lecture 1, Supplemental Effect of Pressure Gradients on Boundary layer • Not in Anderson.
Torque Rotational analogue of Force Must contain Use door example
Presentation transcript:

Info on forces and strains required and produced

How much force is required? Pressure and friction drag forces act to slow the fish as it moves The muscles, in order to move the fins, must overcome: – Pressure drag of the fin due to rotation – Pressure drag on the fin due to apparent incoming fluid velocity – Reactions from the other fins – Friction drag slows the fish, but is NEGLIGIBLE as far as muscle force is concerned

Preliminary pressure drag calculations

The pressure drag force is dependent on the perpendicular velocity squared. The torque is found by integrating the drag force times distance along the fin section.

Preliminary pressure drag calculations

Muscle testing Insert picture of muscle tester setup here

1 st round of muscle testing – lessons learned Dead zone due to space between tubing and fabric mesh. 30 psi was the pressure required to take up the initial slack between the tubing and mesh. Slope inversely related to rubber stiffness, and directly related to the ratio of inner circumference over wall thickness

2 nd round of muscle testing Assembled new muscles with existing tubing and fabric mesh. Used tubing with high inner circumference to thickness ratio (it was thinner). Made sure there was no space between tubing and mesh. Tested the effect of using a slightly smaller mesh than needed, on the same tubing.

2 nd round of muscle testing Tighter mesh nearly eliminated the dead zone Obtained a force of approximately 4 pounds at 20psi

No significant difference between mesh types as long as they’re tight against the tubing 2 nd round of muscle testing

Force Feasibility Force required due to overcome pressure drag with a muscle lever arm of 4cm (1.57”): 1.83 pounds Force produced by first set of muscles: 4 pounds Reaction forces from other fin sections are significant, but also actuate out-of-phase. Are ultimately due to the drag as well, so should be on the same order. Clearly within feasibility, using a muscle assembled from a limited selection of scrap materials.

Strain feasibility Strain level of 13% at 20psi found during testing. A lever arm of 4cm, and maximum angle of 30°, requires a 30.8cm (12.2”) muscle – Has to actuate the section 30°, as well as accommodate 30° of motion in the other direction Larger muscles can be used, making it possible to move lower the lever arm length, decreasing the required muscle length.

Show pictures of fish to CAD model Side view of CAD model, and real bass Same for front view (aspect ratio) (maybe on a separate slide) Also show video of Essex fish; say that we’re going to have the muscles execute a similar motion. Same argument for forward motion at this point.