Related Formula
∫ (1)/(x) dx = ln|x| + C$$\int \frac{1}{x} dx = \ln|x| + C$$
Core Logic
Solving the first differential equation:
(dx)/(dt) + ax = 0 ⇒ (dx)/(x) = -a dt$$\frac{dx}{dt} + ax = 0 \Rightarrow \frac{dx}{x} = -a dt$$
Integrating both sides:
ln|x| = -at + c₁$$\ln|x| = -at + c_1$$
Given x(0) = 2$x(0) = 2$, we find c₁ = ln 2$c_1 = \ln 2$. Thus:
ln(x) = -at + ln 2 ⇒ x(t) = 2e-at$$\ln(x) = -at + \ln 2 \Rightarrow x(t) = 2e^{-at}$$
Step 1: Solving for y(t)
Solving the second differential equation:
(dy)/(dt) + by = 0 ⇒ (dy)/(y) = -b dt$$\frac{dy}{dt} + by = 0 \Rightarrow \frac{dy}{y} = -b dt$$
Integrating both sides:
ln|y| = -bt + c₂$$\ln|y| = -bt + c_2$$
Given y(0) = 1$y(0) = 1$, we find c₂ = 0$c_2 = 0$. Thus:
y(t) = e-bt$y(t) = e^{-bt}$
Step 2: Applying the condition
We are given 3y(1) = 2x(1)$3y(1) = 2x(1)$. Substituting our solutions at t=1$t=1$:
3(e-b) = 2(2e-a) ⇒ 3e-b = 4e-a$$3(e^{-b}) = 2(2e^{-a}) \Rightarrow 3e^{-b} = 4e^{-a}$$
Rearranging to group exponential terms:
e-be-a = (4)/(3) ⇒ ea-b = (4)/(3)$$\frac{e^{-b}}{e^{-a}} = \frac{4}{3} \Rightarrow e^{a-b} = \frac{4}{3}$$
Step 3: Finding t for x(t) = y(t)
Set the two trajectory solutions equal:
x(t) = y(t) ⇒ 2e-at = e-bt$$x(t) = y(t) \Rightarrow 2e^{-at} = e^{-bt}$$
Rearranging gives:
2 = e-bte-at ⇒ 2 = e(a-b)t$$2 = \frac{e^{-bt}}{e^{-at}} \Rightarrow 2 = e^{(a-b)t}$$
Substitute ea-b = (4)/(3)$e^{a-b} = \frac{4}{3}$ from Step 2:
2 = ((4)/(3))^t$$2 = \left(\frac{4}{3}\right)^t$$
Taking (4)/(3)$\log_{\frac{4}{3}}$ on both sides yields:
t = (4)/(3)2$$t = \log_{\frac{4}{3}}2$$
Pattern Recognition
For (dz)/(dt) + kz = 0$\frac{dz}{dt} + kz = 0$, the solution is always an exponential decay z = z₀ e-kt$z = z_0 e^{-kt}$. Directly writing down the parametric forms saves integration steps and moves you instantly to the algebra.
Chapter Mix
Class 12 Maths: Differential Equations