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Mathematical Methods for Physicists: A concise introduction - Site Map

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PROBLEMS<br />

Figure 2.3.<br />

RC circuit.<br />

2.4 RC circuits: A typical RC circuit is shown in Fig. 2.3. Find current ¯ow I…t†<br />

in the circuit, assuming E…t† ˆE 0 .<br />

Hint: the voltage drop across the capacitor is given Q/C, with Q(t) the<br />

charge on the capacitor at time t.<br />

2.5 Find a constant such that …x ‡ y† is an integrating factor of the equation<br />

…4x 2 ‡ 2xy ‡ 6y†dx ‡…2x 2 ‡ 9y ‡ 3x†dy ˆ 0:<br />

What is the solution of this equation?<br />

2.6 Solve dy=dx ‡ y ˆ y 3 x:<br />

2.7 Solve:<br />

(a) the equation …D 2 D 12†y ˆ 0 with the boundary conditions y ˆ 0,<br />

Dy ˆ 3 when t ˆ 0;<br />

(b) the equation …D 2 ‡ 2D ‡ 3†y ˆ 0 with the boundary conditions y ˆ 2,<br />

Dy ˆ 0 when t ˆ 0;<br />

(c) the equation …D 2 2D ‡ 1†y ˆ 0 with the boundary conditions y ˆ 5,<br />

Dy ˆ 3 when t ˆ 0.<br />

2.8 Find the particular integral of …D 2 ‡ 2D 1†y ˆ 3 ‡ t 3 .<br />

2.9 Find the particular integral of …2D 2 ‡ 5D ‡ 7† ˆ3e 2t .<br />

2.10 Find the particular integral of …3D 2 ‡ D 5†y ˆ cos 3t:<br />

2.11 Simple harmonic motion of a pendulum (Fig. 2.4): Suspend a ball of mass m<br />

at the end of a massless rod of length L and set it in motion swinging back<br />

and <strong>for</strong>th in a vertical plane. Show that the equation of motion of the ball is<br />

d 2 <br />

dt 2 ‡ g sin ˆ 0;<br />

L<br />

where g is the local gravitational acceleration. Solve this pendulum equation<br />

<strong>for</strong> small displacements by replacing sin by .<br />

2.12 Forced oscillations with damping: If we allow an external driving <strong>for</strong>ce F…t†<br />

in addition to damping (Example 2.12), the motion of the oscillator is<br />

governed by<br />

y 00 ‡ b m y 0 ‡ k m y ˆ F…t†;<br />

97

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