Q.The value of ''n , such that the differential equation ππ π
π π
π = π(ππππ β ππππ + π); (π°π‘ππ«π π, π β πΉ+) is homogeneous, is
(A) 0
(B) 1
(C) 2
(D) 3
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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) β degree 2.
A first-order equation
dxdyβ=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
dxdyβ=F(xyβ).
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)dxβ2xydy=0 both M and N are degree 2.
Why we care: it becomes separable
Recognising homogeneity buys you a guaranteed method. Substitute
y=vxβdxdyβ=v+xdxdvβ.
Putting this into dxdyβ=F(v) gives
v+xdxdvβ=F(v)βxdxdvβ=F(v)βv,
which separates:
F(v)βvdvβ=xdxβ.
Integrate both sides, then replace v by y/x to return to the original variables. β¦
Concept: Homogeneous Differential Equation β an equation of the form dxdyβ=F(xyβ).
Step 1: Rewrite the given equation:
xndxdyβ=y(logyβlogx+1)=y(logxyβ+1)
Step 2: For homogeneity, the right-hand side must be expressible as a function of xyβ alone. Divide both sides by xn:
dxdyβ=xnyβ(logxyβ+1) β¦
A differential equation is homogeneous if it can be written in the form dxdyβ=F(xyβ). Here, rewriting the given equation shows that for it to be homogeneous, the power n must be 1, making option (B) correct.
We need to find n so that
xndxdyβ=y(logyβlogx+1)
is homogeneous for x,yβR+.
Why homogeneity matters: A first-order differential equation is homogeneous if it can be expressed as dxdyβ=f(xyβ). This means the right-hand side depends only on the ratio y/x, not on x and y separately. The test is: replace x with tx and y with ty; if the equation remains unchanged in form (the t cancels out), it's homogeneous.
Let's apply this step by step.
- Rewrite the equation in standard form Divide both sides by xn (valid since x>0):
dxdyβ=xny(logyβlogx+1)β
- Simplify the logarithmic term Using logyβlogx=log(xyβ), we get:
dxdyβ=xny(logxyβ+1)β
- Check homogeneity condition Replace x by tx and y by ty (with t>0). Then xyβ becomes txtyβ=xyβ, so the logarithmic part logxyβ+1 is unchanged. The numerator becomes (ty)(logxyβ+1)=tβ y(logxyβ+1). The denominator becomes (tx)n=tnxn. So the transformed right-hand side is:
tnxntβ y(logxyβ+1)β=t1βnβ xny(logxyβ+1)β
- For homogeneity, the t factor must vanish The original equation had no t factor. For the transformed equation to be identical in form to the original, we need t1βn=1 for all t>0. This forces the exponent to be zero: 1βn=0, so n=1. β¦
Method: Finding the parameter that makes a DE homogeneous
Use this when a differential equation carries an unknown power (or constant) and you must choose it so the equation becomes homogeneous β i.e. so dxdyβ can be written as a function of xyβ alone.
Steps
Step 1: Solve for the derivative
Isolate dxdyβ so the equation reads
dxdyβ=(expressionΒ inΒ x,y).
Step 2: Force every group into the ratio y/x β¦
Common Mistakes
Mistake 1: Thinking any equation with logyβlogx is automatically homogeneous
Why it's wrong: homogeneity requires the entire right side to reduce to a function of xyβ; a leftover free power of x (from xn) breaks it. Correct approach: demand the exponent of the bare x be zero. β¦
- COMEDK 2024Set 2024-A1 markMCQQ.
[!FORMULA] Β TheΒ generalΒ solutionΒ ofΒ theΒ differentialΒ equationΒ dxdyβ=x2+y2xyβΒ isΒ
(A) y=ce(2y2x2β) (B) y=ce(3y2x2β) (C) y=ce(β2y2x2β) (D) y=ce(y2x2β)βΊReveal solutionSolution
The differential equation is homogeneous, so we substitute y=vx to separate variables. Solving yields y=Ce2y2x2β, which corresponds to option (A).
We are given:
dxdyβ=x2+y2xyβ
Concept & Intuition
The right-hand side is a ratio where both numerator and denominator are homogeneous of degree 2 (each term has total power 2). This suggests the substitution y=vx (or v=y/x), which turns the equation into one where variables separate. The trick is that after substitution, the x and v parts can be isolated, leading to an implicit relation between y and x.
Step-by-step solution
- Rewrite using substitution y=vx Let v=y/x, so y=vx. Then
dxdyβ=v+xdxdvβ
Substitute into the DE:
v+xdxdvβ=x2+(vx)2x(vx)β=x2(1+v2)vx2β=1+v2vβ
- Isolate the derivative term Subtract v from both sides:
xdxdvβ=1+v2vββv=1+v2vβv(1+v2)β=1+v2vβvβv3β=β1+v2v3β
- Separate variables Multiply both sides by dx and divide by the factor involving v:
v31+v2βdv=βx1βdx
(We assume vξ =0; v=0 gives y=0, which is a trivial solution but not part of the general family.)
- Integrate both sides Left side:
β«v31+v2βdv=β«(vβ3+vβ1)dv=β2vβ2β+logβ£vβ£+C1β=β2v21β+logβ£vβ£+C1β
Right side:
β«βx1βdx=βlogβ£xβ£+C2β
Combine constants:
β2v21β+logβ£vβ£=βlogβ£xβ£+C
- Simplify using logarithms Bring the log terms together:
logβ£vβ£+logβ£xβ£=2v21β+C
That is:
logβ£vxβ£=2v21β+C
But vx=y, so:
logβ£yβ£=2v21β+C
- Replace v back in terms of x and y β¦
- KCET 2019Set A-11 markMCQQ.The equation of the curve passing through the point (1,1) such that the slope of the tangent at any point (x,y) is equal to the product of its co-ordinates is (A) 2logx=y2β1 (B) 2logy=x2+1 (C) 2logy=x2β1 (D) 2logx=y2+1
βΊReveal solutionSolution
The slope condition gives dxdyβ=xy, a separable differential equation. Solving with the initial condition (1,1) yields 2logy=x2β1, which is option (C).
The problem gives a geometric condition: at any point (x,y) on the curve, the slope of the tangent equals the product of the coordinates. That is,
dxdyβ=xβ y.
This is a first-order differential equation. The key is to recognise it as separable β we can collect all y terms on one side and all x terms on the other, then integrate.
The curve must pass through (1,1), so that fixes the constant of integration. Letβs work through it.
- Set up the differential equation The slope of the tangent at (x,y) is dxdyβ. The product of the coordinates is xy. So
dxdyβ=xy.
- Separate the variables Bring y terms to the left and x terms to the right:
ydyβ=xdx.
(We assume yξ =0; the point (1,1) ensures y>0 here.)
- Integrate both sides
β«ydyβ=β«xdx
gives
logβ£yβ£=2x2β+C.
Since y is positive near (1,1), we can drop the absolute value:
logy=2x2β+C.
- Apply the initial condition The curve passes through (1,1), so x=1, y=1:
log1=212β+Cβ0=21β+CβC=β21β.
- Write the particular solution Substitute C=β21β:
- COMEDK 2024Set 2024-E1 markMCQQ.The general solution of the differential equation xdxdyβ=y+xtan(xyβ) is (A) sin(xyβ)=xCβ (B) sin(xyβ)=Cx (C) sin(yxβ)=Cx (D) sin(yxβ)=Cy
βΊReveal solutionSolution
This is a homogeneous differential equation solved by substituting y=vx. The general solution simplifies to sin(xyβ)=Cx, which corresponds to option (B).
The key insight is that the equation is homogeneous β every term has the same degree when y and x are considered together. That means we can set y=vx (where v=y/x), which turns the equation into one that separates cleanly. The presence of tan(y/x) is a dead giveaway: itβs a function of the ratio y/x alone.
- Rewrite the equation in standard form Given:
xdxdyβ=y+xtan(xyβ)
Divide through by x (assuming xξ =0):
dxdyβ=xyβ+tan(xyβ)
This is clearly homogeneous: the right-hand side depends only on y/x.
- Substitute y=vx Let v=y/x, so y=vx. Then differentiate:
dxdyβ=v+xdxdvβ
Substitute into the equation:
v+xdxdvβ=v+tan(v)
The v terms cancel on both sides, leaving:
xdxdvβ=tan(v)
- Separate variables Bring the v-terms to one side and x-terms to the other:
tan(v)dvβ=xdxβ
Since tan(v)=cos(v)sin(v)β, we have tan(v)1β=sin(v)cos(v)β. So:
sin(v)cos(v)βdv=xdxβ
- Integrate both sides The left side integrates to logβ£sin(v)β£ (because the derivative of sin(v) is cos(v)):
β«sin(v)cos(v)βdv=logβ£sin(v)β£+C1β
The right side gives:
β«xdxβ=logβ£xβ£+C2β
Combining constants:
logβ£sin(v)β£=logβ£xβ£+C β¦
- COMEDK 2025Set 2025-M1 markMCQQ.The general solution of the differential equation (xβy)dy=(x+y)dx is (A) tanβ1(xyβ)=cx2+y2β (B) tanβ1(xyβ)=x2+y2+c (C) etanβ1(xyβ)=xcx2+y2ββ (D) etanβ1(xyβ)=cx2+y2β
βΊReveal solutionSolution
This is a homogeneous differential equation solved by substituting y=vx, separating variables, and integrating; the general solution is etanβ1(y/x)=cx2+y2β, which matches option (D).
We start by recognizing the structure: the equation (xβy)dy=(x+y)dx is homogeneous β both coefficients are homogeneous functions of degree 1. For such equations, the substitution y=vx (or x=vy) simplifies the relationship between x and y into a separable form.
Why this works:
When we set y=vx, we get dy=vdx+xdv. The original equation becomes an equation in x and v where the variables can be separated. This is the classic method for homogeneous first-order ODEs.
- Rewrite the equation in standard form
(xβy)dy=(x+y)dx
Divide both sides by dx (assuming dxξ =0):
(xβy)dxdyβ=x+y
So
dxdyβ=xβyx+yβ
- Substitute y=vx Then dxdyβ=v+xdxdvβ. The equation becomes:
v+xdxdvβ=xβvxx+vxβ=x(1βv)x(1+v)β=1βv1+vβ
- Separate variables Subtract v from both sides:
xdxdvβ=1βv1+vββv=1βv1+vβv(1βv)β=1βv1+vβv+v2β=1βv1+v2β
So
1+v21βvβdv=xdxβ
- Integrate both sides Left side:
β«1+v21βvβdv=β«1+v21βdvββ«1+v2vβdv
The first integral is tanβ1v. For the second, let u=1+v2, du=2vdv, so β«1+v2vβdv=21βlog(1+v2).
Thus:
tanβ1vβ21βlog(1+v2)=logβ£xβ£+C
- Back-substitute v=y/x
tanβ1(xyβ)β21βlog(1+x2y2β)=logβ£xβ£+C
Simplify the log term:
1+x2y2β=x2x2+y2β
So
21βlog(x2x2+y2β)=21β[log(x2+y2)βlog(x2)]=21βlog(x2+y2)βlogβ£xβ£
Plugging back:
tanβ1(xyβ)β[21βlog(x2+y2)βlogβ£xβ£]=logβ£xβ£+C β¦
- KCET 2023Set A-21 markMCQQ.The degree of the differential equation 1+(dxdyβ)2+(dx2d2yβ)2=3dx2d2yβ+1β is (A) 3 (B) 1 (C) 2 (D) 6
βΊReveal solutionSolution
Remove the radical by cubing both sides, then read off the highest power of the highest-order derivative.
1. The definition being tested
The degree of a differential equation is the power of the highest-order derivative, after the equation has been made free of radicals and fractional powers in the derivatives. If it cannot be made polynomial in the derivatives, the degree is not defined. So the cube root here must be cleared first β you may not read the degree off the equation as printed.
2. The equation
1+(dxdyβ)2+(dx2d2yβ)2=3dx2d2yβ+1β
3. Cube both sides
[1+(dxdyβ)2+(dx2d2yβ)2]3=dx2d2yβ+1
This is now a polynomial in dxdyβ and dx2d2yβ.
4. Identify order and degree
- Order = 2 (the highest derivative present is dx2d2yβ). β¦
- COMEDK 2024Set 2024-M1 markMCQQ.Which of the following is not a homogenous function of x and y (A) sinxβcosy (B) cos2(xyβ)+xyβ (C) x2+2xy (D) 2xβy
βΊReveal solutionSolution
A homogeneous function satisfies f(tx,ty)=tnf(x,y) for some n. Checking each option shows that sinxβcosy fails this test, so it is not homogeneous.
Concept & Intuition
A function of two variables is homogeneous of degree n if scaling both inputs by the same factor t multiplies the output by tn. This is a powerful symmetry property: the functionβs form depends only on the ratio of the variables (like y/x) when n=0, or more generally on powers of t times that ratio. To test homogeneity, replace x with tx and y with ty, then see if you can factor out a single power of t. If you cannot β because the function involves non-polynomial terms like sin or cos of the original variables (not their ratio) β it is not homogeneous.
Step-by-step reasoning
- Option (A): f(x,y)=sinxβcosy Replace x with tx and y with ty:
f(tx,ty)=sin(tx)βcos(ty)
There is no way to factor out a common power of t because sin(tx)ξ =tnsinx for any constant n (except trivially t=1). The function does not scale uniformly. Hence, this is not homogeneous.
- Option (B): f(x,y)=cos2(xyβ)+xyβ Replace:
f(tx,ty)=cos2(txtyβ)+txtyβ=cos2(xyβ)+xyβ
The t cancels completely, so f(tx,ty)=t0f(x,y). This is homogeneous of degree 0.
- Option (C): f(x,y)=x2+2xy Replace: f(tx,ty)=(tx)2+2(tx)(ty)=t2x2+2t2xy=t2(x2+2xy)=t2f(x,y) β¦
- COMEDK 2021Set 2021-B1 markMCQQ.The differential equation xdx+ydy=xdyβydx has solution (A) x2+y2=2ktanβ1xyβ (B) x2+y2=ke2tanβ1xyβ (C) log(x2+y2)=2tanβ1xyβ+c (D) log(x2+y2)=tanβ1xyβ+c
βΊReveal solutionSolution
[!TLDR]
Recognise the two sides as exact differentials of x2+y2 and tanβ1(y/x); separating and integrating gives log(x2+y2)=2tanβ1(y/x)+c.
Concept
This CBSE Class 12 differential-equations problem is solved fastest by spotting standard exact-differential combinations: d(x2+y2)=2(xdx+ydy) and d(tanβ1xyβ)=x2+y2xdyβydxβ.
Solution
Start from
xdx+ydy=xdyβydx.
Write each side as a differential:
21βd(x2+y2)=(x2+y2)d(tanβ1xyβ).
Divide both sides by x2+y2:
21ββ x2+y2d(x2+y2)β=d(tanβ1xyβ).
Integrate:
21βlog(x2+y2)=tanβ1xyβ+c1β. β¦
- COMEDK 2021Set 20211 markMCQQ.The solution of the differential equation ydxdyβ=xβx2y2β+Οβ²(x2y2β)Ο(x2y2β)ββ is (where, C is a constant) (A) Ο(x2y2β)=Cx (B) xΟ(x2y2β)=C (C) Ο(x2y2β)=Cx2 (D) x2Ο(x2y2β)=C
βΊReveal solutionSolution
Integrate: log|phi(v)| = 2 log|x| + log C => phi(v) = C x^2 => phi(y^2/x^2) = C x^2.
Concept: substitute v = y^2/x^2 to reduce to a separable equation.
Given: y dy/dx = x [ y^2/x^2 + phi(v)/phi'(v) ], where v = y^2/x^2.
From v = y^2/x^2 we get y^2 = v x^2. Differentiate with respect to x:
2y (dy/dx) = x^2 (dv/dx) + 2vx
=> y (dy/dx) = (x^2/2)(dv/dx) + vx.
Substitute into the given equation:
(x^2/2)(dv/dx) + vx = xv + x * phi(v)/phi'(v)
=> (x^2/2)(dv/dx) = x * phi(v)/phi'(v) β¦
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