select and apply rail brakes

Similar documents
Selecting and Sizing Ball Screw Drives

UNIT II Robots Drive Systems and End Effectors Part-A Questions

Introduction to Accuracy and Repeatability in Linear Motion Systems

There are four types of friction, they are 1).Static friction 2) Dynamic friction 3) Sliding friction 4) Rolling friction

Fric-3. force F k and the equation (4.2) may be used. The sense of F k is opposite

Name: Partners: Period: Coaster Option: 1. In the space below, make a sketch of your roller coaster.

Motor Selection and Sizing

UltiMate Torque Arms & UltiMate Torque Tubes

Stirling Paatz of robot integrators Barr & Paatz describes the anatomy of an industrial robot.

At the skate park on the ramp

Rules of Actuator and Guide Alignment in Linear Motion Systems

BALL & ACME LEAD SCREW TECHNICAL INFORMATION

Chapter 2 Lead Screws

Acceleration due to Gravity

CNC HARDWARE & TOOLING BASICS

Physics 111: Lecture 4: Chapter 4 - Forces and Newton s Laws of Motion. Physics is about forces and how the world around us reacts to these forces.

F N A) 330 N 0.31 B) 310 N 0.33 C) 250 N 0.27 D) 290 N 0.30 E) 370 N 0.26

LINEAR ACTUATORS. Linear Actuators. Linear Actuators. Linear Actuators are Actuators that creates motion in a straight line, as contrasted

Weight The weight of an object is defined as the gravitational force acting on the object. Unit: Newton (N)

C B A T 3 T 2 T What is the magnitude of the force T 1? A) 37.5 N B) 75.0 N C) 113 N D) 157 N E) 192 N

The modular Line and Room Gantry design from SCHUNK

Forces. Definition Friction Falling Objects Projectiles Newton s Laws of Motion Momentum Universal Forces Fluid Pressure Hydraulics Buoyancy

Exam 2 is at 7 pm tomorrow Conflict is at 5:15 pm in 151 Loomis

Alternative Linear Motion Systems. Iron Core Linear Motors

Linear modules Lifting units Rotary modules Grip modules Inductive proximity switches Plug connectors

When looking at machine tools, the details of the installed drive technology usually

Unit 4 Practice Test: Rotational Motion

Suspension and Steering Systems Operation. The Steering/Suspension System (Overview)

TBG-25 OPTIONS X AXIS TRAVEL (MM) Z AXIS TRAVEL (MM) OPTIONS FOR: SPECIFICATIONS. Specifications. Configuration. Belt Type 25.

Forces. When an object is pushed or pulled, we say that a force is exerted on it.

10. CNC Hardware Basics

Choosing Between Electromechanical and Fluid Power Linear Actuators in Industrial Systems Design

Linear guide slides. For smooth and extremely accurate positioning

Serway_ISM_V1 1 Chapter 4

Work, Energy and Power Practice Test 1

Unit 24: Applications of Pneumatics and Hydraulics

Physics 125 Practice Exam #3 Chapters 6-7 Professor Siegel

Physics 201 Homework 8

Physics: Principles and Applications, 6e Giancoli Chapter 4 Dynamics: Newton's Laws of Motion

Name Period WORKSHEET: KINETIC AND POTENTIAL ENERGY PROBLEMS. 1. Stored energy or energy due to position is known as energy.

Advantages of Auto-tuning for Servo-motors

9. The kinetic energy of the moving object is (1) 5 J (3) 15 J (2) 10 J (4) 50 J

VELOCITY, ACCELERATION, FORCE

Chapter 7: Momentum and Impulse

BED TYPE MILLING CENTRE

Friction and Gravity. Friction. Section 2. The Causes of Friction

Mechanical Systems. Grade 8 Unit 4 Test. 1. A wheelbarrow is an example of what simple machine? Class 1 lever. Class 2 lever.

PS-6.2 Explain the factors that determine potential and kinetic energy and the transformation of one to the other.

Problem Set 1. Ans: a = 1.74 m/s 2, t = 4.80 s

TEPZZ 8 8 A_T EP A1 (19) (11) EP A1 (12) EUROPEAN PATENT APPLICATION. (51) Int Cl.: G01N 3/04 ( ) G01N 3/08 (2006.

Rexroth Linear Motion Technology

WORKSHEET: KINETIC AND POTENTIAL ENERGY PROBLEMS

Why Lead Screws are the Best Fit for Many Linear Motion Applications - and How to Rightly Apply Them

AP Physics - Chapter 8 Practice Test

LINEAR MOTION CONTROL

Design of a Universal Robot End-effector for Straight-line Pick-up Motion

Longitudinal and lateral dynamics

If you put the same book on a tilted surface the normal force will be less. The magnitude of the normal force will equal: N = W cos θ

Belt Drives and Chain Drives. Power Train. Power Train

Industrial Robotics. Training Objective

Lecture L2 - Degrees of Freedom and Constraints, Rectilinear Motion

Prelab Exercises: Hooke's Law and the Behavior of Springs

Lecture 17. Last time we saw that the rotational analog of Newton s 2nd Law is

Thermodynamic efficiency of an actuator that provides the mechanical movement for the driven equipments:

Fulcrum Effort or Applied Force. Fulcrum Load or Resistance. Effort or Applied Force. Load or Resistance. Other First Class Lever Examples.

Name Class Date. You do twice as much work. b. You lift two identical books one meter above the ground.

B) 286 m C) 325 m D) 367 m Answer: B

Chapter 3.8 & 6 Solutions

Resistance in the Mechanical System. Overview

Airplane wing test stand for simulating the airstream. Airbus Deutschland GmbH

F f v 1 = c100(10 3 ) m h da 1h 3600 s b =

Lesson 2 - Force, Friction

Machine tool optimization

Configured Linear Motion Assemblies Reduce Engineering and Assembly Costs and Leadtime

Chapter 4: Newton s Laws: Explaining Motion

DUGARD. Machine Tools Since Dugard 700L Series Heavy Duty CNC Lathes.

Profile rail guides LLR

A Determination of g, the Acceleration Due to Gravity, from Newton's Laws of Motion

GRAVITATIONAL FIELDS PHYSICS 20 GRAVITATIONAL FORCES. Gravitational Fields (or Acceleration Due to Gravity) Symbol: Definition: Units:

8. Potential Energy and Conservation of Energy Potential Energy: When an object has potential to have work done on it, it is said to have potential

GANTRY ROBOTIC CELL FOR AUTOMATIC STORAGE AND RETREIVAL SYSTEM

Multi-Axis Systems. zcs01

Lecture L22-2D Rigid Body Dynamics: Work and Energy

Design Aspects of Robot Manipulators

Steps to Solving Newtons Laws Problems.

Introduction to Linear Actuators: Precision Linear Motion Accomplished Easily and Economically

Roanoke Pinball Museum Key Concepts

Robotic Collision Sensor and/ Axial Compliance Device Protector

Belt Tensioning Methods for Small Package Conveyors What s the best solution?

LAB 6: GRAVITATIONAL AND PASSIVE FORCES

Chapter 6 Work and Energy

Plastic Injection Molding

[ means: Save time, money and space! MAXXMILL 500. Vertical milling center for 5-side machining

State Newton's second law of motion for a particle, defining carefully each term used.

TEACHER ANSWER KEY November 12, Phys - Vectors

WORK DONE BY A CONSTANT FORCE

TOP VIEW. FBD s TOP VIEW. Examination No. 2 PROBLEM NO. 1. Given:

Technical News Bulletin

v v ax v a x a v a v = = = Since F = ma, it follows that a = F/m. The mass of the arrow is unchanged, and ( )

Section 1 Gravity: A Force of Attraction

Transcription:

select and apply rail brakes Alex Thell Mechanical Engineer Nexen Group

L i n e a r M o t i o n Linear guide rail brakes play a critical role in many linear motion applications by ensuring that the guide carriage and payload do not move under load. Precision linear motion is an important requirement for a range of machinery such as packaging machines, metal-cutting machine tools, woodworking machines and medical systems, among others. Many linear motion applications require the ability to stop the motion at various points while work is performed. Rail brakes provide an efficient method of stopping linear motion by providing holding force on profile rail guides in a package small enough to work alongside linear bearing blocks. Rail brakes must be capable of providing reliable, high holding force while ensuring low backlash for accurate positioning. One very popular design uses a series of spring engaged/pneumatic released pistons to apply a clamping force. The design uses a wedge and roller mechanism on the non-bearing contacurface of the guide rail. Selecting the correct rail brake for a particular application begins with calculating the maximum holding force required by the application. Next, select a brake, or brakes, that will deliver that force while ensuring that the brake fits the profile rail. Typical components of a linear motion system are the structural supporystem, bearing guides, profile rail slides and drive system. Linear profile rails are designed into the structural support with a carriage attached to the bearing guides. Actuation of the carriage moves the payload along the linear system to provide the required motion. Plain bearing linear guides rely on low-friction, sliding surfaces running directly on the profile rails to provide smooth, linear motion. Rolling element guides use sets of balls or cylindrical rollers to support the guides. In a recirculating element guide, the balls or rollers circulate within the guide whenever the guide moves with respect to the rail. The payload of the linear motion system rides on the carriage, which is typically driven by an electric motor through a rack and pinion, ball screw, leacrew or belt drive, which converts the rotary motion

into linear motion. Once the payload has been delivered to the proper position, there is often a requirement for the payload to be heltationary. This is normally required in order to provide stability and accuracy while work is being done. A typical example is a linear motion system that carries a robot arm used in pick-and-place assembly operations. The linear axis must be fixed in position in order to accurately maintain the position of the robot arm and ensure that reaction forces generated by the robot do not move the carriage on the rail. Fixing the position of the linear axis is critical since any movement of the carriage would interfere with the assembly operations. How they work Rail brakes ride under the carriage and are attached between the bearing blocks. The rail brake holds the carriage in position by applying friction to the profile rails. Rail brakes are carefully designed not to brake on the rail surfaces that engage with the bearings to ensure no reduction of bearing life. Most rail brakes are designed primarily for static load holding applications since the motor itself can be used to stop the payload dynamically. The rail brake provides rigidity and accurate positioning required to achieve high levels of quality and throughput in a range of operations such as CNC machining and precision assembly among others. A popular rail brake design uses springs to apply clamping force through friction pads onto the profile rails, thus locking the payload of the linear motion system in position. The springs continuously deliver clamping force while pneumatic pistons provide the force needed to release the brake when they are actuated. In order to securely grip the rails, the friction facings on the rail brakes need to be designed to match the size and geometry of the rails. The larger the rails used in the application, the greater the holding force that the brakes are able to apply. The spring engaged/pneumatic released approach previously mentioned provides consistent holding force by tightly pressing the friction facings against the rail. This approach provides low backlash (typically within 0.002 in.). Braking systems integral with the motor or drive system produce higher backlash because the backlash includes not only the backlash of the brakes, but also the backlash of the drive system. The spring engaged/pneumatic released design also uses a low volume cylinder so it doesn t require as much compressed air as typical brakes.

Rail brake applications Rail brakes are used in three primary applications. The first and most common is holding accurate machine position during normal machine operations, such as CNC machining, pick and place gantry machines, and robotic welding and assembly. The second common application is power-off holding, which is needed when the power supply is disconnected from the machine. This is typically required during maintenance or when the linear motion system is turned off between shifts. The third common rail brake application is emergency stop braking. Rail brakes are intended for holding applications with limitemergency stops. They should not be used for cyclic, dynamic braking activity in order to preserve the life of the friction facings. One key advantage of the spring engaged/pneumatic released braking approach is that it automatically stops the payload if the power shouluddenly fail. Selecting rail brakes The firstep in selecting the right rail brake is to determine the maximum holding force required by the application. In static holding, where the carriage comes to a stop before the brake is applied, heat buildup and wear on the brake are minimal. For applications where the rail is oriented horizontally, and therefore the payload is noubjected to gravitational forces, the minimum requiretatic holding force is equal to the force exerted on the carriage by the operation that is performed by the payload of the linear motion device. When the rail is oriented other than horizontally, the brake must also be able to absorb the gravitational forces acting on the carriage. These forces can be determined with the following formula: F m g (sin θ) where F forces in Newtons m mass of the payload, carriage, and motor moving parts in kilograms g acceleration due to gravity θ angle of the rail with respect to horizontal axis In emergency stops, the brake also has to absorb the kinetic energy built up by the carriage and payload of the linear motion device. In many such applications, a predetermined maximum allowable stopping distance has been determined. The formulas below can be used to predict horizontal or vertical stopping distance based on the holding force of the brake. Sample calculations are also provided based on the data below. Brake model RB25 Brake force (F) 1000 N (225 lb) Brake engagement time (t e ) 0.050 sec Acceleration due to gravity (g) 9.8 m/sec 2 Mass of load (m) 45.4 kg Load velocity (V) RB25 0.50 m/sec Sample data Horizontal Travel (X and Y axis) Stopping time at full brake force: m V 45.4 0.50 0.023 sec F 1000 Total time elapsed during emergency stop: t e + 0.05 + 0.023 0.073 sec Distance of travel during brake engagement: V t e (0.5) (0.050) 0.025 m Distance of travel at full brake force: 0.5 m V 2 F 0.006 m (0.5) 45.4 (0.5)2 1000 Total travel distance during emergency stop: + 0.006 + 0.025 0.031 m (31 mm) In this example, the load will travel 31 mm (1.22 in.) from the time the RB25 engages until the system is brought to a complete stop 0.073 seconds later.

Vertical Travel (downward) (Z axis) Stopping time at full brake force: m (g t e + V) F - (m g) (45.4) (9.8 0.05 + 0.5) 0.081 sec 1000 (45.4 9.8) Total elapsed time during emergency stop: t e + 0.05 + 0.081 0.131 sec Distance of travel during brake engagement: (0.5 g) t 2 e ) + V t e 0.5 (9.8) (0.05) 2 + (0.5) (0.05) 0.037 m These equations will help determine the maximum holding force required by the application. Choose a rail brake model with the required holding force that will also fit the guide rail used in the application. If the desired rail brake is not capable of providing the required force, the size of the rail must be increased, or multiple rail brakes must be used to hold the load. DW Nexen Group www.nexengroup.com Distance of travel at full brake force: 0.5 [t e g + V] 0.5 [(0.05) (9.8) + 0.5] 0.081 0.040 m Total travel distance during emergency stop: + 0.037 + 0.040 0.077 sec In this example, the load will travel down 77 mm (3.03 in.) from the time the RB25 engages until the system is brought to a complete stop 0.131 seconds later. www.nexengroup.com 800-843-7445 651-484-5900