Q.Solve the following differential equation: (x+y)dy+(x−y)dx=0;y=1 when x=1
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Homogeneous Differential Equations
The idea: only the ratio y/x matters
A function f(x,y) is homogeneous of degree n if scaling both variables by t scales the function by tn: f(tx,ty)=tnf(x,y). For example f(x,y)=x2+y2 gives f(tx,ty)=t2(x2+y2) — degree 2.
A first-order equation
dxdy=f(x,y)
is called homogeneous when f is homogeneous of degree 0, i.e. f(tx,ty)=f(x,y). Scaling then changes nothing, which means the slope depends only on the ratio y/x, never on the absolute sizes. So a homogeneous equation can always be recast as
dxdy=F(xy).
Quick test in the form M(x,y)dx+N(x,y)dy=0: if every term of M and N has the same total degree (sum of the powers of x and y), the equation is homogeneous. E.g. in (x2+y2)dx−2xydy=0 both M and N are degree 2.
Why we care: it becomes separable
Recognising homogeneity buys you a guaranteed method. Substitute
y=vx⇒dxdy=v+xdxdv.
Putting this into dxdy=F(v) gives
v+xdxdv=F(v)⇒xdxdv=F(v)−v,
which separates:
F(v)−vdv=xdx.
Integrate both sides, then replace v by y/x to return to the original variables. …
Concept: Homogeneous Differential Equation (degree 1 in x and y).
Step 1 – Rewrite and check homogeneity
The equation is
(x+y)dy+(x−y)dx=0⇒dxdy=−x+yx−y.
The right-hand side is a function of y/x only — homogeneous.
Step 2 – Substitute y=vx
Then dxdy=v+xdxdv. Substituting:
v+xdxdv=−1+v1−v.
Step 3 – Separate variables
xdxdv=−1+v1−v−v=−1+v1+v2.
So
1+v21+vdv=−xdx.
Step 4 – Integrate
∫1+v21dv+∫1+v2vdv=−log∣x∣+C.
This gives
tan−1v+21log(1+v2)=−log∣x∣+C.
Replace v=y/x: …
This is a homogeneous differential equation solved by substituting y=vx, separating variables, and integrating. The particular solution satisfying y(1)=1 is log(x2+y2)+2tan−1(xy)=log2+2π.
Why the homogeneous approach works
When you see a differential equation where every term in dx and dy has the same total degree — here, both (x+y) and (x−y) are degree 1 — you're looking at a homogeneous equation. The key insight: if you divide numerator and denominator by x (or y), the equation becomes a function of the ratio y/x alone. That means we can set y=vx, turning the problem into a separable one in v and x.
This is powerful because it reduces a two-variable mess into a single-variable integration.
Step-by-step solution
1. Rewrite the equation in standard form
We have:
(x+y)dy+(x−y)dx=0
Bring the dx term to the other side:
(x+y)dy=−(x−y)dx
So:
dxdy=−x+yx−y
This confirms homogeneity: the right-hand side is a function of y/x only.
2. Substitute y=vx
Let y=vx, where v is a function of x. Then:
dxdy=v+xdxdv
Substitute into the equation:
v+xdxdv=−x+vxx−vx=−x(1+v)x(1−v)=−1+v1−v
3. Separate variables
Bring v to the right:
xdxdv=−1+v1−v−v
Combine the terms on the right:
−1+v1−v−v=−1+v1−v+v(1+v)=−1+v1−v+v+v2=−1+v1+v2
So:
xdxdv=−1+v1+v2
Now separate:
1+v21+vdv=−xdx
4. Integrate both sides
Left side:
∫1+v21+vdv=∫1+v21dv+∫1+v2vdv
The first integral is tan−1v. For the second, let u=1+v2, so du=2vdv, giving 21log∣1+v2∣.
Thus:
tan−1v+21log(1+v2)=−log∣x∣+C
5. Back-substitute v=y/x
Recall v=y/x, so 1+v2=1+x2y2=x2x2+y2.
Then:
tan−1(xy)+21log(x2x2+y2)=−log∣x∣+C
Simplify the log term:
21log(x2x2+y2)=21log(x2+y2)−21log(x2)=21log(x2+y2)−log∣x∣
Plugging back:
tan−1(xy)+21log(x2+y2)−log∣x∣=−log∣x∣+C …
Method: Homogeneous initial-value problem (arctan + log)
Use this for (x+y)dy+(x−y)dx=0 with a condition; y=vx gives an inverse-tangent plus logarithm, then the point fixes the constant.
Steps
Step 1: Solve for dxdy and substitute y=vx
Rearrange to dxdy=x+yy−x, then use dxdy=v+xdxdv.
Step 2: Separate and split the numerator
You reach 1+v21+vdv=−xdx; split into 1+v21 (→ tan−1v) and 1+v2v (→ 21log(1+v2)). …
Common Mistakes
Mistake 1: Not splitting 1+v21+v
Why it's wrong: it must break into 1+v21 (→ tan−1v) and 1+v2v (→ 21log(1+v2)). Correct approach: integrate the two pieces separately.
Mistake 2: Forgetting to apply the condition y=1 at x=1
Why it's wrong: the question wants a particular solution, so C must be evaluated as log2+2π (after doubling). Correct approach: substitute the point and simplify. …
Showing the 12 most recent of 13 on this concept.
- TG EAPCET 2023Set eng-2023-05-14-AN1 markMCQQ.If the solution for the differential equation y2dx+(x2−xy−y2)dy=0 at (2,1) is x+y=k(xy2−y3), then k= (A) −3 (B) −4 (C) 4 (D) 3
›Reveal solutionSolution
This is a homogeneous differential equation solved by the substitution y=vx. After separating variables and integrating, the general solution is x+y=C(xy2−y3). Using the point (2,1) gives C=−3, so k=−3.
We are given the differential equation
y2dx+(x2−xy−y2)dy=0
and told that its solution passing through (2,1) can be written as
x+y=k(xy2−y3).
We need to find k.
Concept and intuition
The equation is homogeneous — every term in dx and dy is of degree 2. For such equations, the standard trick is to set y=vx (or x=vy), which reduces the problem to a separable one. Once we integrate, we get a family of curves. Plugging the given point pins down the constant, and matching the form reveals k.
Step-by-step solution
- Rewrite the equation in standard form
y2dx+(x2−xy−y2)dy=0
Divide through by dy (assuming dy=0):
y2dydx+x2−xy−y2=0
So
dydx=y2−x2+xy+y2.
The right-hand side is homogeneous of degree 0 (each term in numerator and denominator is degree 2). This suggests the substitution x=vy.
- Substitute x=vy Then dydx=v+ydydv. Plug into the equation:
v+ydydv=y2−(vy)2+(vy)y+y2=y2−v2y2+vy2+y2=−v2+v+1.
So
ydydv=−v2+v+1−v=−v2+1.
- Separate variables
ydydv=1−v2⇒1−v2dv=ydy.
- Integrate both sides
∫1−v2dv=∫ydy.
The left-hand side is a standard partial fractions integral:
1−v21=21(1−v1+1+v1),
so
∫1−v2dv=21log1−v1+v.
The right-hand side gives log∣y∣+C. Thus
21log1−v1+v=log∣y∣+C.
- Simplify the constant Multiply by 2:
log1−v1+v=2log∣y∣+2C=log(y2)+logC1,
where C1=e2C>0. So
log1−v1+v=log(C1y2)⇒1−v1+v=C1y2.
- Back-substitute v=x/y 1−x/y1+x/y=C1y2⇒…
- TG EAPCET 2026Set eng-2026-05-11-FN1 markMCQQ.The solution of the differential equation dxdy=3x+y−2⋅3y3x+y−2⋅3x when y(1)=2 is (A) 3y=7(3x)+12 (B) y=log3(7(3x)−14) (C) y=log3(7(3x)−12) (D) 3y=7(3x)−14
›Reveal solutionSolution
This problem involves solving a first-order differential equation by separating variables. We simplify the expression, integrate both sides, and then use the given initial condition to find the particular solution. The solution is y=log3(7(3x)−12).
A differential equation relates a function to its derivatives. To solve such an equation, we aim to find the original function. One common and powerful technique for first-order differential equations is separation of variables. This method works when the equation can be rearranged such that all terms involving the dependent variable (here, y) and its differential (dy) are on one side, and all terms involving the independent variable (here, x) and its differential (dx) are on the other side. Once separated, we can integrate both sides independently to find the general solution. Finally, any given initial condition allows us to determine the specific constant of integration, leading to a particular solution.
Here's how we solve the given differential equation:
- Simplify the expression: The given differential equation is dxdy=3x+y−2⋅3y3x+y−2⋅3x. We can use the property am+n=am⋅an to rewrite 3x+y as 3x⋅3y.
dxdy=3x⋅3y−2⋅3y3x⋅3y−2⋅3x
Now, factor out common terms from the numerator and the denominator:dxdy=3y(3x−2)3x(3y−2)
- Separate the variables: Our goal is to get all terms involving y on the left side with dy, and all terms involving x on the right side with dx. Multiply both sides by 3y(3x−2) and by dx:
3y−23ydy=3x−23xdx
The variables are now successfully separated.3. Integrate both sides:
We integrate both sides of the separated equation:
∫3y−23ydy=∫3x−23xdx
To solve these integrals, we use a substitution. Consider the integral $\int \dfrac{3^t}{3^t - 2} dt$. Let $u = 3^t - 2$. Then, differentiate $u$ with respect to $t$: $du = \dfrac{d}{dt}(3^t - 2) dt = (3^t \ln 3) dt$. This means $3^t dt = \dfrac{du}{\ln 3}$. Substituting these into the integral:∫u1⋅ln3du=ln31∫u1du=ln31ln∣u∣+C
Replacing $u$ with $3^t - 2$:∫3t−23tdt=ln31ln∣3t−2∣+C
Applying this result to both sides of our separated differential equation:ln31ln∣3y−2∣=ln31ln∣3x−2∣+C′
Here, $C'$ is the constant of integration. We can multiply the entire equation by $\ln 3$ to simplify:ln∣3y−2∣=ln∣3x−2∣+C′′
Let $C'' = \ln K$ for some positive constant $K$.ln∣3y−2∣=ln∣3x−2∣+lnK
Using the logarithm property $\ln a + \ln b = \ln(ab)$: … - TG EAPCET 2024Set eng-2024-05-11-FN1 markMCQQ.If the equation of the curve which passes through the point (1,1) satisfies the differential equation dxdy=5x+2y−32x−5y+3, then the equation of that curve is (A) x2+5xy−y2+3x−3y−5=0 (B) x2+5xy−y2+3x+3y−11=0 (C) x2−5xy−y2−3x−3y+11=0 (D) x2−5xy−y2+3x+3y−1=0
›Reveal solutionSolution
The differential equation is homogeneous after shifting the origin to the intersection of the lines in the numerator and denominator; solving via the substitution Y=vX in the shifted coordinates and using the given point (1,1) yields the curve x2−5xy−y2+3x+3y−1=0, which is option (D).
The key idea: when a differential equation has the form dxdy=a′x+b′y+c′ax+by+c, it is often homogeneous after a translation that eliminates the constant terms. That translation moves the origin to the intersection point of the two lines ax+by+c=0 and a′x+b′y+c′=0. Once the constants vanish, the equation becomes homogeneous in the new variables, and we can use the substitution Y=vX in the shifted coordinates.
Here, the numerator is 2x−5y+3 and the denominator is 5x+2y−3. Their intersection is found by solving:
{2x−5y+3=05x+2y−3=0
Multiply the first by 2 and the second by 5:
4x−10y+6=0,25x+10y−15=0
Adding: 29x−9=0⇒x=299. Substituting back: 2(299)−5y+3=0⇒2918+3=5y⇒2918+87=5y⇒29105=5y⇒y=2921.
So the intersection point is (299,2921). Shift the origin there by setting:
X=x−299,Y=y−2921
Then dx=dX, dy=dY, and the differential equation becomes:
dXdY=5(X+299)+2(Y+2921)−32(X+299)−5(Y+2921)+3
Simplify numerator: 2X+2918−5Y−29105+3=2X−5Y+(2918−105+3)=2X−5Y+(−2987+3)=2X−5Y+(−3+3)=2X−5Y.
Denominator: 5X+2945+2Y+2942−3=5X+2Y+(2945+42−3)=5X+2Y+(2987−3)=5X+2Y+(3−3)=5X+2Y.
Thus the equation reduces to the homogeneous form:
dXdY=5X+2Y2X−5Y
Now set Y=vX, so dXdY=v+XdXdv. Substitute:
v+XdXdv=5X+2vX2X−5vX=5+2v2−5v
Hence:
XdXdv=5+2v2−5v−v=5+2v2−5v−v(5+2v)=5+2v2−5v−5v−2v2=5+2v2−10v−2v2
Factor 2:
XdXdv=5+2v2(1−5v−v2)
Separate variables:
1−5v−v25+2vdv=X2dX
Integrate both sides. Notice that the derivative of the denominator 1−5v−v2 is −5−2v=−(5+2v). So:
∫1−5v−v25+2vdv=−∫1−5v−v2−(5+2v)dv=−log∣1−5v−v2∣+C
Thus:
−log∣1−5v−v2∣=2log∣X∣+C
Multiply by -1:
log∣1−5v−v2∣=−2log∣X∣−C=log(X21)+constant
Exponentiate:
∣1−5v−v2∣=X2K
where K=e−C>0. Remove the absolute value by allowing K to be any nonzero constant:
1−5v−v2=X2K
Now substitute back v=Y/X:
1−5XY−X2Y2=X2K
Multiply through by X2:
X2−5XY−Y2=K
Recall X=x−299, Y=y−2921. So:
(x−299)2−5(x−299)(y−2921)−(y−2921)2=K
We determine K using the given point (1,1). Substitute x=1, y=1:
(1−299)2−5(1−299)(1−2921)−(1−2921)2=K
Compute:
1−299=2920,1−2921=298
So:
(2920)2−5⋅2920⋅298−(298)2=841400−841800−84164=841400−800−64=841−464
Thus K=−841464.
Now the equation is:
(x−299)2−5(x−299)(y−2921)−(y−2921)2=−841464
Multiply both sides by 841=292 to clear denominators:
- TG EAPCET 2026Set eng-2026-05-11-AN1 markMCQQ.If the general solution of the differential equation dxdy+x+y−52x+2y−1=0 is ax+by−9log(∣x+y+p∣)=c, and b,a,p are in GP, then the common ratio of this GP is (A) 3 (B) 2 (C) 21 (D) 31
›Reveal solutionSolution
The differential equation is reducible to a homogeneous form via substitution u=x+y, leading to a solution of the form ax+by−9log(∣x+y+p∣)=c. Matching coefficients and using the GP condition b,a,p gives the common ratio 2.
The key insight is that the equation mixes x and y in the combination x+y in both numerator and denominator. This suggests a substitution that simplifies the structure: let u=x+y. Then the equation becomes separable, and after integration we obtain a logarithmic relation. Comparing with the given general form lets us identify a, b, and p, and the geometric progression condition then fixes the common ratio.
- Rewrite the equation in terms of u=x+y. Let u=x+y. Then dxdy=dxdu−1. Substitute into
dxdy+x+y−52x+2y−1=0
to get
(dxdu−1)+u−52u−1=0.
- Simplify to a separable form. Bring terms together:
dxdu=1−u−52u−1.
Compute the right-hand side:
1−u−52u−1=u−5(u−5)−(2u−1)=u−5−u−4.
So
dxdu=−u−5u+4.
- Separate variables and integrate.
u+4u−5du=−dx.
Perform polynomial division:
u+4u−5=1−u+49.
Hence
(1−u+49)du=−dx.
Integrate:
∫(1−u+49)du=−∫dx
gives
u−9log∣u+4∣=−x+C.
- Return to x,y and match the given form. Since u=x+y, we have
x+y−9log∣x+y+4∣=−x+C.
Bring x to the left:
2x+y−9log∣x+y+4∣=C. …
- TG EAPCET 2023Set eng-2023-05-13-AN1 markMCQQ.The general solution of the differential equation (3x−4y)(dx−3dy)+(6dx−4dy)=0 is (A) x−2y+log∣3x−4y+6∣=c (B) 5x−15y−4log∣15x−20y−12∣=c (C) 5x−15y+14log∣15x−20y−12∣=c (D) 8y−4x+log∣9x−12y+4∣=c
›Reveal solutionSolution
Collect dx and dy, substitute v=3x−4y; the solution is 5x−15y+14log∣15x−20y−12∣=c.
Collect terms. Expanding (3x−4y)(dx−3dy)+(6dx−4dy)=0:
(3x−4y+6)dx+(−9x+12y−4)dy=0⇒dxdy=9x−12y+43x−4y+6.
Substitution. Since 9x−12y=3(3x−4y), let v=3x−4y, giving dxdy=43−dxdv and dxdy=3v+4v+6. Equating:
43−dxdv=3v+4v+6 ⇒ dxdv=3−3v+44(v+6)=3v+45v−12.
Separate and integrate. ∫5v−123v+4dv=∫dx. Writing 3v+4=53(5v−12)+556: …
- TG EAPCET 2024Set eng-2024-05-11-FN1 markMCQQ.The general solution of the differential equation (6x2−2xy−18x+3y)dx−(x2−3x)dy=0 is (A) 2x2−x2y−9x2+3xy+c=0 (B) 4x3−2x2y−6x2+6xy+c=0 (C) 2x2−4xy−y2−x+3y+c=0 (D) 3x2+5xy−2y2−4x−2y+c=0
›Reveal solutionSolution
The differential equation is exact after rewriting, and integrating yields 2x3−x2y−9x2+3xy=c, which matches option (A).
We are given:
(6x2−2xy−18x+3y)dx−(x2−3x)dy=0
Concept & Intuition
This is a first-order differential equation. The standard approach is to check if it is exact. An equation of the form Mdx+Ndy=0 is exact if ∂y∂M=∂x∂N. If exact, we can find a function F(x,y) whose total differential equals Mdx+Ndy; then the solution is F(x,y)=c.
Here, note the minus sign: we have Mdx+Ndy=0 with M=6x2−2xy−18x+3y and N=−(x2−3x)=−x2+3x.
Step-by-step solution
- Identify M and N Write the equation as:
(6x2−2xy−18x+3y)dx+(−x2+3x)dy=0
So M=6x2−2xy−18x+3y and N=−x2+3x.
- Check exactness Compute ∂y∂M:
∂y∂M=−2x+3
Compute ∂x∂N:
∂x∂N=−2x+3
They are equal, so the equation is exact.
- Find the potential function F(x,y) We need F such that:
∂x∂F=M=6x2−2xy−18x+3y
Integrate with respect to x:
F(x,y)=∫(6x2−2xy−18x+3y)dx=2x3−x2y−9x2+3xy+g(y)
where g(y) is an arbitrary function of y alone.
- Determine g(y) Differentiate F with respect to y: ∂y∂F=−x2+3x+g′(y)…
- TG EAPCET 2022Set eng-2022-07-19-FN1 markMCQQ.The equation of any member of the family of all the ellipses whose axes are along the coordinate axes satisfies the differential equation (A) xyy′′+x(y′)2−y′=0 (B) xyy′′+x(y′)2−y=y′ (C) y′′+y(y′)2−xy=0 (D) y′′+(y′)2+x2y2=0
›Reveal solutionSolution
The family of ellipses with axes along the coordinate axes has the equation a2x2+b2y2=1. Eliminating the two arbitrary constants a and b by differentiating twice yields the differential equation xyy′′+x(y′)2−yy′=0, which matches option (A) after a sign check.
The key idea: a family of curves with two independent parameters (here a and b) requires two derivatives to eliminate them. The resulting differential equation must be free of both constants. We start from the standard ellipse equation and differentiate implicitly, then eliminate a2 and b2 algebraically.
- Write the general ellipse equation. Any ellipse with axes along the coordinate axes (centre at the origin) has the form
a2x2+b2y2=1,
where a and b are positive constants (semi-major and semi-minor axes). No other parameters appear, so the family is two-parameter.
- Differentiate once with respect to x. Treat y as a function of x. Differentiating term by term:
a22x+b22yy′=0.
Divide through by 2:
a2x+b2yy′=0.(1)
- Differentiate a second time. Differentiate (1) with respect to x (using the product rule on the second term):
a21+b21((y′)2+yy′′)=0.(2)
- Eliminate a2 and b2. From (1), we can write
a2x=−b2yy′⇒a21=−b2y⋅xy′.
Substitute this expression for a21 into (2):
−b2y⋅xy′+b21((y′)2+yy′′)=0.
Multiply through by b2 (which is nonzero):
- TG EAPCET 2023Set eng-2023-05-14-AN1 markMCQQ.If a and b are the arbitrary constants, then the differential equation corresponding to the family of curves given by y=x[acos(logx)+bsin(logx)] is (A) xdx2d2y+xdxdy−2y=0 (B) x2dx2d2y−xdxdy+2y=0 (C) x2dx2d2y−xdxdy−2y=0 (D) x2dx2d2y−xdxdy+y=0
›Reveal solutionSolution
The family of curves is x times a linear combination of cos(logx) and sin(logx), so it is the general solution of an Euler-Cauchy equation. Differentiating twice and eliminating a and b yields x2y′′−xy′+2y=0, which is option (B).
We are given the family of curves
y=x[acos(logx)+bsin(logx)],
where a and b are arbitrary constants. The task is to find the differential equation (DE) that all such curves satisfy, without the constants a and b.
Concept and intuition:
Since a and b are the only free parameters, the DE must be of second order (two constants → two derivatives to eliminate them). The presence of logx inside trigonometric functions, multiplied by x, is the classic signature of an Euler–Cauchy equation — terms like x2y′′, xy′, and y are the natural building blocks. Our plan: differentiate twice, then algebraically eliminate a and b.
- First derivative Write y=x⋅u, where u=acos(logx)+bsin(logx). Differentiate using the product rule:
y′=u+xu′.
Now u′=dxd[acos(logx)+bsin(logx)]. Recall dxdcos(logx)=−sin(logx)⋅x1, and dxdsin(logx)=cos(logx)⋅x1. Hence
u′=x1[−asin(logx)+bcos(logx)]=xv,where v=−asin(logx)+bcos(logx).
So
y′=u+x⋅xv=u+v.
- Second derivative Differentiate y′=u+v again. We already have u′=v/x. Differentiating v:
v′=dxd[−asin(logx)+bcos(logx)]=x1[−acos(logx)−bsin(logx)]=−xu.
So
y′′=u′+v′=xv−xu=xv−u.
- Eliminate a and b From y=xu, we get u=xy. From y′=u+v, we get v=y′−u=y′−xy. Substitute both into y′′=xv−u:
- TG EAPCET 2026Set eng-2026-05-10-AN1 markMCQQ.The differential equation corresponding to the family of curves y=ae2x+bx2, where a and b are parameters is (x−x2)dx2d2y+y(2−4x)= (A) (1−2x2)dxdy (B) (2−4x2)dxdy (C) (1−2x)dxdy (D) (2−4x)dxdy
›Reveal solutionSolution
We eliminate the two parameters a and b by differentiating twice and substituting back, obtaining a second‑order linear ODE. The right‑hand side simplifies to (2−4x)dxdy, so the correct option is (D).
Concept & Intuition
When a family of curves contains two arbitrary constants, the corresponding differential equation must be of order 2. The idea is to differentiate the given equation enough times to “free” the parameters, then eliminate them algebraically. Here y=ae2x+bx2 has a and b; we differentiate twice, solve for a and b in terms of y and its derivatives, and substitute back. The result will be a relation among y, y′, and y′′ — exactly what the question asks.
Step‑by‑step derivation
- Write the given family and its first two derivatives
y=ae2x+bx2
Differentiate:
dxdy=2ae2x+2bx
Differentiate again:
dx2d2y=4ae2x+2b
- Eliminate the constant b From y′′=4ae2x+2b, we can solve for b:
2b=y′′−4ae2x⇒b=2y′′−4ae2x
But it’s cleaner to eliminate b by combining y′ and y′′. Notice:
y′=2ae2x+2bx
Multiply y′′ by x:
xy′′=4axe2x+2bx
Subtract xy′′ from y′:
y′−xy′′=(2ae2x+2bx)−(4axe2x+2bx)=2ae2x−4axe2x=2ae2x(1−2x)
So we have:
y′−xy′′=2ae2x(1−2x)(1)
- Eliminate the constant a From the original equation y=ae2x+bx2, we can also express ae2x:
ae2x=y−bx2
But we already have b from y′′: b=2y′′−4ae2x. Substituting that back would reintroduce a. Instead, use equation (1) to solve for ae2x:
2ae2x=1−2xy′−xy′′⇒ae2x=2(1−2x)y′−xy′′
Now plug this into the expression for b from y′′:
y′′=4ae2x+2b⇒2b=y′′−4ae2x=y′′−4⋅2(1−2x)y′−xy′′
Simplify:
2b=y′′−1−2x2(y′−xy′′)
Multiply both sides by (1−2x):
2b(1−2x)=y′′(1−2x)−2(y′−xy′′)
Expand the right side:
y′′(1−2x)−2y′+2xy′′=y′′−2xy′′−2y′+2xy′′=y′′−2y′
So:
2b(1−2x)=y′′−2y′⇒b=2(1−2x)y′′−2y′(2)
- Substitute ae2x and b back into the original equation The original y=ae2x+bx2 becomes:
y=2(1−2x)y′−xy′′+2(1−2x)y′′−2y′⋅x2
Multiply both sides by 2(1−2x):
2y(1−2x)=(y′−xy′′)+x2(y′′−2y′)
Expand the right side:
y′−xy′′+x2y′′−2x2y′=y′−2x2y′+(−xy′′+x2y′′)=y′(1−2x2)+y′′(x2−x)
So:
2y(1−2x)=y′(1−2x2)+y′′(x2−x)
- Rearrange to match the question’s form Bring the y′′ term to the left:
- TG EAPCET 2024Set eng-2024-05-10-FN1 markMCQQ.If A and B are arbitrary constants, then the differential equation having y=Ae−x+Bcosx as its general solution is (A) (sinx−cosx)dx2d2y+2cosxdxdy−(sinx+cosx)y=0 (B) (cosx−sinx)dx2d2y+2cosxdxdy+(sinx+cosx)y=0 (C) (cosx+sinx)dx2d2y+2sinxdxdy−(sinx−cosx)y=0 (D) (cosx−sinx)dx2d2y−2sinxdxdy+(cosx+sinx)y=0
›Reveal solutionSolution
The key idea is to eliminate the arbitrary constants A and B from y=Ae−x+Bcosx by differentiating twice and solving the resulting linear system. The correct differential equation is option (B).
We start with the given general solution:
y=Ae−x+Bcosx, where A and B are arbitrary constants.
To find the differential equation that has this as its general solution, we need to eliminate A and B. Since there are two constants, we will need up to the second derivative.
Concept & Intuition
A general solution with two arbitrary constants corresponds to a second‑order linear ODE. The constants are “hidden” in the expression; differentiating gives us equations that involve them. By treating A and B as unknowns, we can solve for them from the first two derivatives and substitute back, or directly combine the equations to eliminate them. The trick is to notice that e−x and cosx are linearly independent, so the elimination will yield a unique linear relation among y, y′, and y′′ with coefficients that may depend on x.
Step‑by‑step elimination
- Write down the function and its first two derivatives.
y=Ae−x+Bcosx
Differentiate:
y′=−Ae−x−Bsinx
Differentiate again:
y′′=Ae−x−Bcosx
- Notice a pattern: we can isolate Ae−x and Bcosx. From y and y′′ we have:
y=Ae−x+Bcosx
y′′=Ae−x−Bcosx
Adding these two equations gives:
y+y′′=2Ae−x⇒Ae−x=2y+y′′
Subtracting the second from the first gives:
y−y′′=2Bcosx⇒Bcosx=2y−y′′
- Now use the first derivative to link these. From y′=−Ae−x−Bsinx, substitute the expressions we found:
y′=−2y+y′′−Bsinx
But we also have Bcosx=2y−y′′, so B=2cosxy−y′′ (provided cosx=0, but the final ODE will hold everywhere by continuity). Then:
y′=−2y+y′′−2cosxy−y′′⋅sinx
Simplify:
y′=−2y+y′′−2(y−y′′)tanx
- Clear denominators and rearrange. Multiply through by 2:
2y′=−(y+y′′)−(y−y′′)tanx
2y′=−y−y′′−ytanx+y′′tanx
Group terms involving y′′ and y:
2y′=−y(1+tanx)+y′′(tanx−1)
Multiply both sides by cosx to eliminate the tangent (since tanx=sinx/cosx):
2y′cosx=−y(cosx+sinx)+y′′(sinx−cosx) …
- TG EAPCET 2022Set eng-2022-07-18-FN1 markMCQQ.The degree of the differential equation x(dx2d2y)1/3+2x2(dx2d2y)5/3+7dxdy+y=0 (A) 15 (B) 5 (C) 12 (D) 3
›Reveal solutionSolution
The degree of a differential equation is the power of the highest-order derivative once the equation is rewritten as a polynomial in the derivatives (no fractional or negative powers on any derivative). Here the highest-order derivative is dx2d2y, and after the fractional exponents 1/3 and 5/3 are cleared, its highest surviving power is 5. So the degree is 5, option (B).
Concept and intuition
The degree of a differential equation is defined only once the equation is free of radicals and fractional/negative powers of the derivatives — it is then the exponent of the highest-order derivative present. When a derivative appears with more than one fractional power (as dx2d2y does here, with exponents 1/3 and 5/3), we clear the fractions by substitution and algebraic elimination, then read off the resulting integer power.
Step-by-step solution
- Identify the highest-order derivative and its exponents
x(dx2d2y)1/3+2x2(dx2d2y)5/3+7dxdy+y=0.
The highest-order derivative is p=dx2d2y (order 2), appearing with exponents 31 and 35 — both with denominator 3.
- Substitute to remove the fractional exponents Let t=p1/3 (so p=t3) and Q=7dxdy+y. The equation becomes
2x2t5+xt+Q=0,
which is already a genuine polynomial — but in t, not yet in p.
- Eliminate t to get a polynomial purely in p Since t is a real cube root of p, the two other cube roots tω, tω2 (where ω is a complex cube root of unity, ω3=1) also satisfy (tω)3=(tω2)3=p. Multiplying the equation evaluated at t, tω, tω2 together produces an expression that depends only on p (it is symmetric in the three cube roots), via the identity a3+b3+c3−3abc=(a+b+c)(a+bω+cω2)(a+bω2+cω) with a=2x2p5/3, b=xp1/3, c=Q: 8x6p5−6x3Qp2+x3p+Q3=0. …
- TG EAPCET 2022Set eng-2022-07-20-FN1 markMCQQ.Assertion (A) : The degree of the differential equation y′′+2xy′+loge(dxdy)=0 is 2. Reason (R) : The degree of a differential equation is the highest degree of the highest order derivative occurring in the equation, after the equation is expressed in the form of a polynomial in differential coefficients. The correct option among the following is: (A) (A) is true (R) is true and (R) is the correct explanation for (A) (B) (A) is true (R) is true but (R) is not the correct explanation for (A) (C) (A) is true but (R) is false (D) (A) is false but (R) is true
›Reveal solutionSolution
Because of the loge(dy/dx) term the equation is not a polynomial in its derivatives, so its degree is not defined — the Assertion (degree =2) is false. The Reason states the definition correctly and is true. Option (D).
The concept: order versus degree
- Order = the order of the highest derivative present. Here the highest is y′′, so the order is 2.
- Degree = the power to which that highest-order derivative is raised — but only after the equation has been written as a polynomial in the derivatives. If it cannot be so written, the degree is not defined.
The degree is undefined whenever a derivative appears inside a transcendental function: sin(y′), ey′, log(y′), and so on.
Step 1 — Look at the equation
y′′+2xy′+loge(dxdy)=0
The first two terms are fine, but loge(y′) is a transcendental function of y′. Expanding it as an infinite series would give infinitely many powers of y′ — never a polynomial. There is no algebraic manipulation that removes the logarithm while keeping the equation polynomial in y′ and y′′.
Step 2 — Verdict on the Assertion …
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