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ZEYNEP KIZILIRMAK

ZEYNEP K.

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Two masses $m_{1}$ and $m_{2}$ rest on a horizontal frictionless plane. The masses are attached to fixed walls by springs whose spring constants are $k_{1}$ and $k_{3}$. (See Figure $9.7 .5 .$ The masses are connected by a spring whose spring constant is $k_{2}$. Determine a first-order system of differential equations that governs the motion of the system. (FIGURE CAN'T COPY)

Two masses $m_{1}$ and $m_{2}$ rest on a horizontal frictionless plane. The masses are attached to fixed walls by springs whose spring constants are $k_{1}$ and $k_{3}$. (See Figure $9.7 .5 .$ The masses are connected by a spring whose spring constant is $k_{2}$. Determine a first-order system of differential equations that governs the motion of the system. (FIGURE CAN'T COPY)

Differential Equations and Linear Algebra

Systems of Differential Equations

Some Applications of Linear Systems of…

Two equal masses $m$ are connected to three identical springs (spring constant $k$ ) on a frictionless horizontal surface (see figure). One end of the system is fixed; the other is driven back and forth with a displacement $X=X_{0} \cos \omega t .$ Find and sketch graphs of the resulting displacements of the two masses.

Two equal masses $m$ are connected to three identical springs (spring constant $k$ ) on a frictionless horizontal surface (see figure). One end of the system is fixed; the other is driven back and forth with a displacement $X=X_{0} \cos \omega t .$ Find and sketch graphs of the resulting displacements of the two masses.

Vibrations and Waves

Two particles as in one dimension at the junction of there springs, as shown in the figure The springs all have unstretched lengths equal to $a$ and the force constants and masses are shown. Find the eigenfrequencies and normal modes of the system.

Classical Mechanics

A particle is thrown up vertically with initial speed to. reaches a maximum heir,ht and falls brick to ground. Show that the Coriolis deflection when it again reaches the ground is opposite in direction, and four times greater in magnitude. than the Coriolis deflection when it is dropped at rest from the same maximum height.

Classical Mechanics

Questions asked

INSTANT ANSWER

5.6.1 (a) Using the two spin functions \( \varphi_{1}=\alpha \) and \( \varphi_{2}=\beta \) as an orthonormal basis (so \( \langle\alpha \mid \alpha\rangle=\langle\beta \mid \beta\rangle=1,\langle\alpha \mid \beta\rangle=0) \), and the relations \[ S_{x} \alpha=\frac{1}{2} \beta, \quad S_{x} \beta=\frac{1}{2} \alpha, \quad S_{y} \alpha=\frac{1}{2} i \beta, \quad S_{y} \beta=-\frac{1}{2} i \alpha, \quad S_{z} \alpha=\frac{1}{2} \alpha, \quad S_{z} \beta=-\frac{1}{2} \beta, \] construct the \( 2 \times 2 \) matrices of \( S_{x}, S_{y} \), and \( S_{z} \). (b) Taking now the basis \( \varphi_{1}^{\prime}=C(\alpha+\beta), \varphi_{2}^{\prime}=C(\alpha-\beta) \) : (i) Verify that \( \varphi_{1}^{\prime} \) and \( \varphi_{2}^{\prime} \) are orthogonal, (ii) Assign \( C \) a value that makes \( \varphi_{1}^{\prime} \) and \( \varphi_{2}^{\prime} \) normalized, (iii) Find the unitary matrix for the transformation \( \left\{\varphi_{i}\right\} \rightarrow\left\{\varphi_{i}^{\prime}\right\} \). (c) Find the matrices of \( S_{x}, S_{y} \), and \( S_{z} \) in the \( \left\{\varphi_{i}^{\prime}\right\} \) basis.

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Sam Stansfield verified

Numerade educator

Consider a Hilbert space whose members are functions defined on the surface of the unit sphere, with a scalar product of the form [ langle f | g angle = int d Omega f^* g, ] where ( dOmega ) is the element of solid angle. Note that the total solid angle of the sphere is ( 4pi ). We work here with the three functions ( varphi_1 = Cx/r ), ( varphi_2 = Cy/r ), ( varphi_3 = Cz/r ), with ( C ) assigned a value that makes the ( varphi_i ) normalized. (a) Find ( C ), and show that the ( varphi_i ) are also mutually orthogonal. (b) Form the ( 3 imes 3 ) matrices of the angular momentum operators [ L_x = -ileft(y frac{partial}{partial z} - z frac{partial}{partial y} ight), quad L_y = -ileft(z frac{partial}{partial x} - x frac{partial}{partial z} ight), ] [ L_z = -ileft(x frac{partial}{partial y} - y frac{partial}{partial x} ight). ]

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Newtons law in daily life questions

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Yujie Wang verified

Numerade educator

a person approaching a vehicle moving at hogh speed is pushed towards the vehicle reason

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Yujie Wang verified

Numerade educator

Q.1. A donkey is attached to a cart. a) It pulls on a cart but the car does not move. Explain the reason considering the Newton's Law. (5 pt) b) Under what conditions does the system (donkey+cart) accelerate? Describe your response with reference to Newton's Law. (5 pt)

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Luke Humphrey verified

Numerade educator

for the vibration of a linear triatomic molecule is it possible to have their rotational motion while they are shifting to the right or to the left slightly all together

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