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qualifying_exam_2
qualifying_exam_2

... component due to the fluid flow through the channel. The momentum equation given in (3) will need the addition of the dipole gradient forces, as well as an alteration of the electric field term to account for the polarization of the water in the channel. The energy terms for both electric and magnet ...
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Lec 2014 10 07

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unit 21: materials engineering learning outcome 1

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Electric Field around a Metal Disk within a Microwave Resonator
Electric Field around a Metal Disk within a Microwave Resonator

Measurement of Electromagnetic Radiation Emitted during Rapid
Measurement of Electromagnetic Radiation Emitted during Rapid

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Lecture - Galileo

... A dielectric is any material that is not a conductor, but polarizes well. Even though they don’t conduct they are electrically active – Examples. Stressed plastic or piezo-electric crystal will produce a spark. – When you put a dielectric in a uniform electric field (like in between the plates of a ...
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12.1 GaAs MESFET with Source-Connected Field Plate for High

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exam i, physics 1306

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... Two charged objects, which are small compared to the distance between them, can be modeled as point charges. The forces between point charges are proportional to the product of the charges and inversely proportional to the square of the distance between the point charges [Fe = ke q1 q2) / r2]. Probl ...
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... Just as we learnt in general physics: when a force exerts onto a spring, the spring would become extended or suppressed. The spring was described as being deformed. In the case of liquid crystal, when the external force exert and exceed a certain value, deformation will happen. The relative position ...
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Review Powerpoint (including Ex Problem Answers)

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Exam - 1 - SOLUTIONS

... The charges create an electric field at surface B that is perpendicular to the surface everywhere. Therefore no work is necessary to move a charge from one part of the surface to another. The angle between the force and the displacement (on the surface) is 90 degrees and the cosine is zero. Thus W=0 ...
Ch. 22 Gauss's Law - San Jose State University
Ch. 22 Gauss's Law - San Jose State University

Short Answer Question (6 points)
Short Answer Question (6 points)

Chapter 22 Gauss`s Law 1 Charge and Electric Flux
Chapter 22 Gauss`s Law 1 Charge and Electric Flux

... Figure 1: This is Fig. 22.2 show a positive flux (i.e., flow) out of the enclosed volume due to positive charges, and the negative flux, or flow, into the enclosed volume due to negative charge. ...
Potential Difference & Electric Potential
Potential Difference & Electric Potential

... Capacitors with Dielectrics • The molecules of the dielectric, when placed in the electric field of a capacitor, become polarized – Centers of positive and negative charges become preferentially oriented in the field (see figure below at left) – Creates a net positive (negative) charge on the left ...
Electrical Energy Potential
Electrical Energy Potential

... field is given by WAB = qExΔx J • This is valid for both +ve and -ve charges influenced by a constant electrical field. As electrical fields are vectors, direction of the field and the corresponding displacement of the charge must be indicated by a +ve or -ve sign. ...
Document
Document

Document
Document

... In principle, the electrostatic field due to a continuous charge distribution can always be found by using Coulomb’s law, but the integration required may be complex. In this chapter we present an alternative approach, base on the concept of lines of force, which, in some cases, can be much simpler. ...
Powerpoint
Powerpoint

... is always perpendicular to an equipotential surface. is always tangent to an equipotential surface. always bisects an equipotential surface. makes an angle to an equipotential surface that depends on the amount of charge. ...
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Electroactive polymers



Electroactive polymers, or EAPs, are polymers that exhibit a change in size or shape when stimulated by an electric field. The most common applications of this type of material are in actuators and sensors. A typical characteristic property of an EAP is that they will undergo a large amount of deformation while sustaining large forces.The majority of historic actuators are made of ceramic piezoelectric materials. While these materials are able to withstand large forces, they commonly will only deform a fraction of a percent. In the late 1990s, it has been demonstrated that some EAPs can exhibit up to a 380% strain, which is much more than any ceramic actuator. One of the most common applications for EAPs is in the field of robotics in the development of artificial muscles; thus, an electroactive polymer is often referred to as an artificial muscle.
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