differential equation
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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 ]