Animated Solution for Mathematics - Differential Equations: The solution of the differential equation dxdy=(x−y)2, when y(1)=1, is:
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Visualized Solution
Analyzing dxdy=(x−y)2
Given Equation: dxdy=(x−y)2
Notice the term (x−y) inside the square.
The Substitution x−y=t
This is of the form dxdy=f(ax+by+c).
Let x−y=t.
Differentiating x−y=t
Differentiating with respect to x:
dxd(x)−dxd(y)=dxdt
1−dxdy=dxdt
Expressing dxdy
Rearranging the terms:
dxdy=1−dxdt
Substitute into the original equation:
1−dxdt=t2
Separating Variables t and x
Rearrange to separate variables t and x:
dxdt=1−t2
1−t2dt=dx
Setting up ∫1−t2dt
Integrate both sides:
∫1−t2dt=∫dx
Recall the standard integral:
∫a2−x2dx=2a1lna−xa+x+C
Executing the Integration
Applying the formula with a=1 and x=t:
21ln1−t1+t=x+C
Back Substitution of t
Substitute t=x−y back into the equation:
21ln1−(x−y)1+(x−y)=x+C
21ln1−x+y1+x−y=x+C
Applying Initial Condition y(1)=1
Given initial condition: y(1)=1
This means when x=1, y=1.
Let's substitute these values to find C.
Finding the Constant C
Substitute x=1 and y=1:
21ln1−1+11+1−1=1+C
21ln(1)=1+C
Since ln(1)=0:
0=1+C⟹C=−1
Final Simplification
Substitute C=−1 back:
21ln1−x+y1+x−y=x−1
Multiply by 2:
ln1−x+y1+x−y=2(x−1)
Using property ln(ba)=−ln(ab):
−ln1+x−y1−x+y=2(x−1)
The Way Forward
Key Takeaway: For equations of type dxdy=f(ax+by+c), always substitute ax+by+c=t.
Next Challenge: Try solving dxdy=sin(x+y) using the same substitution method.
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The Sigma Insight: Variable Separable Method
Analyzing the Setup
Imagine you are standing before a complex differential equation:
dxdy=(x−y)2
At first glance, it looks intimidating. The variables x and y are locked in a tight embrace inside that square.
You might be tempted to expand it, but that only makes the mess worse. In the world of JEE Advanced, when you see a linear combination like (x−y) trapped inside a function, you are looking at an invitation to use a powerful tool: Substitution.
The Power of Substitution
We start by defining a new variable, t=x−y. This is the spark. By letting t=x−y, we are essentially simplifying the geometry of the problem.
Now, we need to see how this affects the derivative. Differentiating both sides with respect to x, we get:
dxd(x)−dxd(y)=dxdt
This simplifies to 1−dxdy=dxdt. Rearranging this, we find that:
dxdy=1−dxdt
Now, watch the magic happen. We substitute this back into our original equation:
1−dxdt=t2
Suddenly, the y has vanished! We are left with a clean, elegant equation in terms of t and x:
dxdt=1−t2
The Elegance of Separation
With the equation in the form dxdt=1−t2, we can easily separate the variables. By moving the terms, we get:
1−t2dt=dx
This is the heart of the solution. We have transformed a tangled mess into a standard integral. We know from our calculus toolkit that:
∫a2−t2dt=2a1lna−ta+t+C
Applying this with a=1, we get:
21ln1−t1+t=x+C
Finding the Unique Path
We are almost there, but we must return to our original variables. Substituting t=x−y back into our equation, we get:
21ln1−(x−y)1+(x−y)=x+C
This simplifies to:
21ln1−x+y1+x−y=x+C
Now, we use the initial condition y(1)=1. When x=1, y=1. Plugging these in, we get:
21ln1−1+11+1−1=1+C
Since ln(1)=0, we find that 0=1+C, which means C=−1.
The Final Celebration
Substituting C=−1 back into our equation, we have:
21ln1−x+y1+x−y=x−1
Multiplying by 2, we get:
ln1−x+y1+x−y=2(x−1)
To match the standard forms, we use the property ln(ba)=−ln(ab) to flip the fraction, giving us:
−ln1+x−y1−x+y=2(x−1)
This is the exact form we were looking for! You have successfully navigated the complexity and arrived at the solution. Keep this substitution trick in your arsenal—it is a classic JEE favorite.