Single and Double plane pendulum - LSU

Single and Double plane pendulum Gabriela Gonz´alez 1 Introduction We will write down equations of motion for a single and a double plane pendulum, following

Plane Waves and Wave Propagation - LSU

Plane Waves and Wave Propagation Augustin Jean Fresnel (1788 - 1827) November 9, 2001 Contents 1 Plane Waves in Uniform Linear Isotropic Nonconducting Media 2

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The stability of the bicycle - Department of Physics ...

ridden model is not—it requires constant rider effort to main-tain its stability. A combination of the simple theories ac-counts neatly for all the facts.

  Physics, Of physics

Core Computing: a Foundation for Information Technology

Information technology is the outgrowth of computer science, and if LSU fails to build its program in computer science, information technology education and research at LSU will su er.

  Information, Computing, Foundations, Technology, Information technology, A foundation for information technology

Projectile Motion y(final)Projectile Motion y(final) 0

2))y p Draw a convenient coordinate s ystem and resolve forces into components. 3) Define direction of acceleration 4) Subdivide into differing systems if needed 5) S l N t ’ 2 d l ( t ) f h t5) S olve N ew ton ’s 2n d law (vec tor) for each system and use equations to find unknowns.

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Chapter 10: Superconductivity

London and London derived a phenomenological theory of su-perconductivity which correctly describes the Meissner e ect. They assumed that the electrons move in a frictionless state, so that mv_ = eE (7) or, since @j @t = en sv_, @j s @t = e2n s m E (First London Eqn.) (8) 8

  States, Theory

-2 Newton's Law of Gravitation

PROBLEMS sec. 13-2 Newton's Law of Gravitation •1 A mass M is split into two parts, m and M – m, which are then separated by a certain distance. What ratio m/M maximizes the magnitude of the gravitational force between the parts? Answer: •2 Moon effect.Some people believe that the Moon controls their activities. If the Moon moves from being directly on the opposite side of …

  Newton, S law, Gravitation

A pendulum with a moving support point

• Vertical periodic motion: Y = Y 0 cos(Ωt), X = 0. 2Y 0 cosΩt)sinθ. The motion of the support adds an oscillating component to the gravitational acceleration. This is not a driven oscillator like the previous case, because the oscillatory driving force is vertical but the natural oscillatory pendulum motion is horizontal. If Y 0Ω2 ˝ g,

  Motion, Oscillatory

Pretest-posttest designs and measurement of change

regression coefficients, ANOVA on residual scores re-sults in an inflated α-level of significance and (b) when the regression coefficient for the total sample of all groups combined is used, ANOVA on residual scores yields an inappropriately conservative test [16]. 3.4. Repeated measures ANOVA with pretest-posttest data

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Wireless and Broadband Technologies

qualified telecommunication engineers and transfer technology to industry. We envision an experimental facility with gigabit connectivity among servers, high-speed wireless interconnection and routing among nodes, with ancillary equipment to support research in communications and signal processing and to implement demanding user oriented

  Engineer

CONIC SECTIONS - NCERT

Focal distance of a point Let the equation of the parabola be y2 = 4ax and P(x, y) be a point on it. Then the distance of P from the focus (a, 0) is called the focal distance of the point, i.e., FP = ( )x a y− +2 2 = 2 ( ) 4x a ax− + = ( )x a+ 2 = | x + a | 11.1.4 Ellipse An ellipse is the set of points in a plane, the sum of whose distances

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Photo Tourism: Exploring Photo Collections in 3D

fore adding them to the scene; and using focal length information from image EXIF tags. Schaffalitzky and Zisserman [2002] present another related technique for calibrating unordered image sets, con- ... Our approach therefore uses an approximate plane-based,.)). a )) ...

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3.1.Image formation by Mirrors and Lenses

A virtual image is formed by a plane mirror at a distance q behind the mirror. q = -p. 2 Parabolic Mirrors Parallel rays reflected by a parabolic mirror are focused at a point, called the Focal Point located on the optic axis. Optic Axis Parabolic Reflector Parabolic mirrors can be used to focus incoming parallel rays to a small area

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Human Visual System

the focal length. ... • The sampling process may be viewed as partitioning the real xy plane with a grid whose vertices are elements in the Cartesian product Z x Z, where Z is the set of integers. • If ∆x and ∆y are separation of grid points in the x and y directions,

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Chapter 4 –Microscopy

focal distance measured from principal plane working distance = distance from F to physical surface of lens Entrance Pupil image of physical aperture f W Entrance Pupil = image of physical apert and entrance pupil determine numerical aperf ture i.e. resolution Chapter 4: Microscopy 10

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Reflection and Refraction

focal point, F. The distance from the focal point to the vertex of the mirror is the focal length, f. The relationship between the radius of curvature and the focal length is, R = 2f. For a concave mirror, all of the light rays that run parallel to the principal axis will reflect off of the mirror and converge at the focal point. See Figure 4 ...

  Reflections, Falco, Refraction, Reflection and refraction

The Focal Length of Lenses

Focal length of lenses 3 20 30 10 0 lens d sag (b) L (a) {Figure 1: (a) The top view of a spherometer. (b)Speherometr on a convex lens. The figure shows the definition of L, and sagittal distance dsag. screw at the lens’ center.

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