GGR124H1 Lecture Notes - Frank Lloyd Wright, City Beautiful Movement, Broadacre City

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7 Apr 2011

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Colonies: particular area of city serves as port-of-entry", temporary phenomenon very short term. Enclaves: exist over several generations, congregation for functional reasons, locating there because of choice, offensive group. Ghettoes: exist over several generations, arise due to discrimination, defensive mechanism group. Influences urban development: examples of planning include, zoning, location of various facilities, community development developing, building, regenerating communities, planners are: www. notesolution. com. 2: concerned with the management of urban change. T rans-historical issues: nimbys (not in my back yard), lulus (locally undesirable land use), and bananas. March 16 (built absolutely nothing anywhere near anyone: reform, reproduction, or revolution, efficacy of planning, planning for whom, baron haussman"s paris to recreate an older version of paris. Based on these principles: each garden city would have a pop. Of 32000: city would be self supporting, diversity of activity, spacious layout, greenbelt separating the town from other towns and particular activities www. notesolution. com. Land was help in common and not individually owned.

Related Questions

Learning Goal: Understand how to determine the constants in thegeneral equation for simple harmonic motion, in terms of giveninitial conditions.
A common problem in physics is to match the particular initialconditions - generally given as an initial position x_0 andvelocity v_) at t=0 - once you have obtained the general solution.You have dealt with this problem in kinematics, where theformula

1. x(t) = x_0 + v_0t + at^2

has two arbitrary constants (technically constants of integrationthat arise when finding the position given that the acceleration isa constant). The constants in this case are the initial positionand velocity, so "fitting" the general solution to the initialconditions is very simple.

For simple harmonic motion, it is more difficult to fit the initialconditions, which we take to be

x_0, the position of the oscillator at t = 0, and
v_0, the velocity of the oscillator at t = 0.

There are two common forms for the general solution for theposition of a harmonic oscillator as a function of time t:

2. x(t) = A\cos(omega t + phi) and
3. x(t) = C\cos(omega t) + S\sin(omega t),

where A, phi, C, and S are constants, omega is the oscillationfrequency, and t is time.

Although both expressions have two arbitrary constants--parametersthat can be adjusted to fit the solution to the initialconditions--Equation 3 is much easier to use to accommodate x_0 andv_0. (Equation 2 would be appropriate if the initial conditionswere specified as the total energy and the time of the first zerocrossing, for example.)

Find C and S in terms of the initial position and velocity of theoscillator.
Give your answers in terms of x_0, v_0, and omega. Separate youranswers with a comma.

GGR124H1 Lecture Notes - Frank Lloyd Wright, City Beautiful Movement, Broadacre City

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