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480 DIFFERENTIAL EQUATIONS<br />

Thus 4 = A + B (1)<br />

Velocity,<br />

dx<br />

dt =−2Ae−2t − 4Be −4t<br />

dx<br />

dt<br />

= 8 cm/s when t = 0,<br />

thus 8 =−2A − 4B (2)<br />

From <strong>equation</strong>s (1) and (2),<br />

A = 12 and B =−8<br />

Hence the particular solution is<br />

x = 12e −2t − 8e −4t<br />

i.e. displacement, x = 4(3e −2t − 2e −4t )cm<br />

Now try the following exercise.<br />

Exercise 189 Further problems on second<br />

order <strong>differential</strong> <strong>equation</strong>s of the form<br />

a d2 y<br />

dx 2 + b dy<br />

dx + cy = 0<br />

1. The charge, q, on a capacitor in a certain electrical<br />

circuit satisfies the <strong>differential</strong> <strong>equation</strong><br />

d2 q<br />

dt 2 + 4dq + 5q = 0. Initially (i.e. when<br />

dt<br />

t = 0), q = Q and dq = 0. Show that the<br />

dt<br />

charge in the circuit can be expressed as:<br />

q = √ 5 Qe −2t sin (t + 0.464)<br />

2. A body moves in a straight line so that its<br />

distance s metres from the origin after time<br />

t seconds is given by d2 s<br />

dt 2 + a2 s = 0, where a<br />

is a constant. Solve the <strong>equation</strong> for s given<br />

that s = c and ds<br />

dt = 0 when t = 2π a<br />

[s = c cos at]<br />

3. The motion of the pointer of a galvanometer<br />

about its position of equilibrium is represented<br />

by the <strong>equation</strong><br />

I d2 θ<br />

dt 2 + K dθ + Fθ = 0.<br />

dt<br />

If I, the moment of inertia of the pointer about<br />

its pivot, is 5 × 10 −3 , K, the resistance due to<br />

friction at unit angular velocity, is 2 × 10 −2<br />

and F, the force on the spring necessary to<br />

produce unit displacement, is 0.20, solve the<br />

<strong>equation</strong> for θ in terms of t given that when<br />

t = 0, θ = 0.3 and dθ<br />

dt = 0.<br />

[θ = e −2t (0.3 cos 6t + 0.1 sin 6t)]<br />

4. Determine an expression for x for a <strong>differential</strong><br />

<strong>equation</strong> d2 x<br />

dt 2 + 2ndx dt + n2 x = 0 which<br />

represents a critically damped oscillator,<br />

given that at time t = 0, x = s and dx<br />

dt = u.<br />

[x ={s + (u + ns)t}e −nt ]<br />

5. L d2 i<br />

dt 2 + R di<br />

dt + 1 i = 0 is an <strong>equation</strong> representing<br />

current i in an electric circuit. If<br />

C<br />

inductance L is 0.25 henry, capacitance C<br />

is 29.76 × 10 −6 farads and R is 250 ohms,<br />

solve the <strong>equation</strong> for i given the boundary<br />

conditions that when t = 0, i = 0 and di<br />

[<br />

dt = 34.<br />

i = 1 (<br />

e −160t − e −840t)]<br />

20<br />

6. The displacement s of a body in a damped<br />

mechanical system, with no external forces,<br />

satisfies the following <strong>differential</strong> <strong>equation</strong>:<br />

2 d2 s<br />

dt 2 + 6ds dt + 4.5s = 0<br />

where t represents time. If initially, when<br />

t = 0, s = 0 and ds = 4, solve the <strong>differential</strong><br />

dt<br />

<strong>equation</strong> for s in terms of t. [s = 4te − 2 3 t ]

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