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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π Start your 14-day free trial to unlock the full solution βConcept understanding β Homogeneous Differential Equation
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¦
Showing the 12 most recent of 13 on this concept.
- TG EAPCET 2022Set eng-2022-07-20-FN1 markMCQQ.Assertion (A) : The degree of the differential equation yβ²β²+2xyβ²+logeβ(dxdyβ)=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
βΊReveal solutionSolution
Because of the logeβ(dy/dx) term the equation is not a polynomial in its derivatives, so its degree is not defined β 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 yβ²β², so the order is 2.
- Degree = the power to which that highest-order derivative is raised β 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(yβ²), eyβ², log(yβ²), and so on.
Step 1 β Look at the equation
yβ²β²+2xyβ²+logeβ(dxdyβ)=0
The first two terms are fine, but logeβ(yβ²) is a transcendental function of yβ². Expanding it as an infinite series would give infinitely many powers of yβ² β never a polynomial. There is no algebraic manipulation that removes the logarithm while keeping the equation polynomial in yβ² and yβ²β².
Step 2 β Verdict on the Assertion β¦
- TG EAPCET 2023Set eng-2023-05-14-AN1 markMCQQ.If the solution for the differential equation y2dx+(x2βxyβy2)dy=0 at (2,1) is x+y=k(xy2βy3), then k= (A) β3 (B) β4 (C) 4 (D) 3
βΊReveal 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(xy2βy3). Using the point (2,1) gives C=β3, so k=β3.
We are given the differential equation
y2dx+(x2βxyβy2)dy=0
and told that its solution passing through (2,1) can be written as
x+y=k(xy2βy3).
We need to find k.
Concept and intuition
The equation is homogeneous β 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+(x2βxyβy2)dy=0
Divide through by dy (assuming dyξ =0):
y2dydxβ+x2βxyβy2=0
So
dydxβ=y2βx2+xy+y2β.
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 dydxβ=v+ydydvβ. Plug into the equation:
v+ydydvβ=y2β(vy)2+(vy)y+y2β=y2βv2y2+vy2+y2β=βv2+v+1.
So
ydydvβ=βv2+v+1βv=βv2+1.
- Separate variables
ydydvβ=1βv2β1βv2dvβ=ydyβ.
- Integrate both sides
β«1βv2dvβ=β«ydyβ.
The left-hand side is a standard partial fractions integral:
1βv21β=21β(1βv1β+1+v1β),
so
β«1βv2dvβ=21βlogβ1βv1+vββ.
The right-hand side gives logβ£yβ£+C. Thus
21βlogβ1βv1+vββ=logβ£yβ£+C.
- Simplify the constant Multiply by 2:
logβ1βv1+vββ=2logβ£yβ£+2C=log(y2)+logC1β,
where C1β=e2C>0. So
logβ1βv1+vββ=log(C1βy2)β1βv1+vβ=C1βy2.
- Back-substitute v=x/y 1βx/y1+x/yβ=C1βy2ββ¦
- TG EAPCET 2026Set eng-2026-05-11-FN1 markMCQQ.The solution of the differential equation dxdyβ=3x+yβ2β 3y3x+yβ2β 3xβ when y(1)=2 is (A) 3y=7(3x)+12 (B) y=log3β(7(3x)β14) (C) y=log3β(7(3x)β12) (D) 3y=7(3x)β14
βΊReveal 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=log3β(7(3x)β12).
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 dxdyβ=3x+yβ2β 3y3x+yβ2β 3xβ. We can use the property am+n=amβ an to rewrite 3x+y as 3xβ 3y.
dxdyβ=3xβ 3yβ2β 3y3xβ 3yβ2β 3xβ
Now, factor out common terms from the numerator and the denominator:dxdyβ=3y(3xβ2)3x(3yβ2)β
- 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(3xβ2) and by dx:
3yβ23yβdy=3xβ23xβdx
The variables are now successfully separated.3. Integrate both sides:
We integrate both sides of the separated equation:
β«3yβ23yβdy=β«3xβ23xβdx
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:β«u1ββ ln3duβ=ln31ββ«u1βdu=ln31βlnβ£uβ£+C
Replacing $u$ with $3^t - 2$:β«3tβ23tβdt=ln31βlnβ£3tβ2β£+C
Applying this result to both sides of our separated differential equation:ln31βlnβ£3yβ2β£=ln31βlnβ£3xβ2β£+Cβ²
Here, $C'$ is the constant of integration. We can multiply the entire equation by $\ln 3$ to simplify:lnβ£3yβ2β£=lnβ£3xβ2β£+Cβ²β²
Let $C'' = \ln K$ for some positive constant $K$.lnβ£3yβ2β£=lnβ£3xβ2β£+lnK
Using the logarithm property $\ln a + \ln b = \ln(ab)$: β¦ - TG EAPCET 2026Set eng-2026-05-11-AN1 markMCQQ.If the general solution of the differential equation dxdyβ+x+yβ52x+2yβ1β=0 is ax+byβ9log(β£x+y+pβ£)=c, and b,a,p are in GP, then the common ratio of this GP is (A) 3 (B) 2 (C) 21β (D) 31β
βΊReveal solutionSolution
The differential equation is reducible to a homogeneous form via substitution u=x+y, leading to a solution of the form ax+byβ9log(β£x+y+pβ£)=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 dxdyβ=dxduββ1. Substitute into
dxdyβ+x+yβ52x+2yβ1β=0
to get
(dxduββ1)+uβ52uβ1β=0.
- Simplify to a separable form. Bring terms together:
dxduβ=1βuβ52uβ1β.
Compute the right-hand side:
1βuβ52uβ1β=uβ5(uβ5)β(2uβ1)β=uβ5βuβ4β.
So
dxduβ=βuβ5u+4β.
- Separate variables and integrate.
u+4uβ5βdu=βdx.
Perform polynomial division:
u+4uβ5β=1βu+49β.
Hence
(1βu+49β)du=βdx.
Integrate:
β«(1βu+49β)du=ββ«dx
gives
uβ9logβ£u+4β£=βx+C.
- Return to x,y and match the given form. Since u=x+y, we have
x+yβ9logβ£x+y+4β£=βx+C.
Bring x to the left:
2x+yβ9logβ£x+y+4β£=C. β¦
- TG EAPCET 2022Set eng-2022-07-18-FN1 markMCQQ.The degree of the differential equation x(dx2d2yβ)1/3+2x2(dx2d2yβ)5/3+7dxdyβ+y=0 (A) 15 (B) 5 (C) 12 (D) 3
βΊReveal 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 dx2d2yβ, 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 β it is then the exponent of the highest-order derivative present. When a derivative appears with more than one fractional power (as dx2d2yβ 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(dx2d2yβ)1/3+2x2(dx2d2yβ)5/3+7dxdyβ+y=0.
The highest-order derivative is p=dx2d2yβ (order 2), appearing with exponents 31β and 35β β both with denominator 3.
- Substitute to remove the fractional exponents Let t=p1/3 (so p=t3) and Q=7dxdyβ+y. The equation becomes
2x2t5+xt+Q=0,
which is already a genuine polynomial β 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 tΟ,Β tΟ2 (where Ο is a complex cube root of unity, Ο3=1) also satisfy (tΟ)3=(tΟ2)3=p. Multiplying the equation evaluated at t,Β tΟ,Β tΟ2 together produces an expression that depends only on p (it is symmetric in the three cube roots), via the identity a3+b3+c3β3abc=(a+b+c)(a+bΟ+cΟ2)(a+bΟ2+cΟ) with a=2x2p5/3,Β b=xp1/3,Β c=Q: 8x6p5β6x3Qp2+x3p+Q3=0. β¦
- 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) xdx2d2yβ+xdxdyββ2y=0 (B) x2dx2d2yββxdxdyβ+2y=0 (C) x2dx2d2yββxdxdyββ2y=0 (D) x2dx2d2yββxdxdyβ+y=0
βΊReveal 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 x2yβ²β²βxyβ²+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 β two derivatives to eliminate them). The presence of logx inside trigonometric functions, multiplied by x, is the classic signature of an EulerβCauchy equation β terms like x2yβ²β², xyβ², and y are the natural building blocks. Our plan: differentiate twice, then algebraically eliminate a and b.
- First derivative Write y=xβ u, where u=acos(logx)+bsin(logx). Differentiate using the product rule:
yβ²=u+xuβ².
Now uβ²=dxdβ[acos(logx)+bsin(logx)]. Recall dxdβcos(logx)=βsin(logx)β x1β, and dxdβsin(logx)=cos(logx)β x1β. Hence
uβ²=x1β[βasin(logx)+bcos(logx)]=xvβ,whereΒ v=βasin(logx)+bcos(logx).
So
yβ²=u+xβ xvβ=u+v.
- Second derivative Differentiate yβ²=u+v again. We already have uβ²=v/x. Differentiating v:
vβ²=dxdβ[βasin(logx)+bcos(logx)]=x1β[βacos(logx)βbsin(logx)]=βxuβ.
So
yβ²β²=uβ²+vβ²=xvββxuβ=xvβuβ.
- Eliminate a and b From y=xu, we get u=xyβ. From yβ²=u+v, we get v=yβ²βu=yβ²βxyβ. Substitute both into yβ²β²=xvβuβ:
- TG EAPCET 2023Set eng-2023-05-13-AN1 markMCQQ.The general solution of the differential equation (3xβ4y)(dxβ3dy)+(6dxβ4dy)=0 is (A) xβ2y+logβ£3xβ4y+6β£=c (B) 5xβ15yβ4logβ£15xβ20yβ12β£=c (C) 5xβ15y+14logβ£15xβ20yβ12β£=c (D) 8yβ4x+logβ£9xβ12y+4β£=c
βΊReveal solutionSolution
Collect dx and dy, substitute v=3xβ4y; the solution is 5xβ15y+14logβ£15xβ20yβ12β£=c.
Collect terms. Expanding (3xβ4y)(dxβ3dy)+(6dxβ4dy)=0:
(3xβ4y+6)dx+(β9x+12yβ4)dy=0βdxdyβ=9xβ12y+43xβ4y+6β.
Substitution. Since 9xβ12y=3(3xβ4y), let v=3xβ4y, giving dxdyβ=43βdxdvββ and dxdyβ=3v+4v+6β. Equating:
43βdxdvββ=3v+4v+6βΒ βΒ dxdvβ=3β3v+44(v+6)β=3v+45vβ12β.
Separate and integrate. β«5vβ123v+4βdv=β«dx. Writing 3v+4=53β(5vβ12)+556β: β¦
- TG EAPCET 2024Set eng-2024-05-11-FN1 markMCQQ.The general solution of the differential equation (6x2β2xyβ18x+3y)dxβ(x2β3x)dy=0 is (A) 2x2βx2yβ9x2+3xy+c=0 (B) 4x3β2x2yβ6x2+6xy+c=0 (C) 2x2β4xyβy2βx+3y+c=0 (D) 3x2+5xyβ2y2β4xβ2y+c=0
βΊReveal solutionSolution
The differential equation is exact after rewriting, and integrating yields 2x3βx2yβ9x2+3xy=c, which matches option (A).
We are given:
(6x2β2xyβ18x+3y)dxβ(x2β3x)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 βyβMβ=βxβNβ. 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=6x2β2xyβ18x+3y and N=β(x2β3x)=βx2+3x.
Step-by-step solution
- Identify M and N Write the equation as:
(6x2β2xyβ18x+3y)dx+(βx2+3x)dy=0
So M=6x2β2xyβ18x+3y and N=βx2+3x.
- Check exactness Compute βyβMβ:
βyβMβ=β2x+3
Compute βxβNβ:
βxβNβ=β2x+3
They are equal, so the equation is exact.
- Find the potential function F(x,y) We need F such that:
βxβFβ=M=6x2β2xyβ18x+3y
Integrate with respect to x:
F(x,y)=β«(6x2β2xyβ18x+3y)dx=2x3βx2yβ9x2+3xy+g(y)
where g(y) is an arbitrary function of y alone.
- Determine g(y) Differentiate F with respect to y: βyβFβ=βx2+3x+gβ²(y)β¦
- 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) xyyβ²β²+x(yβ²)2βyβ²=0 (B) xyyβ²β²+x(yβ²)2βy=yβ² (C) yβ²β²+y(yβ²)2ββxyβ=0 (D) yβ²β²+(yβ²)2+x2y2=0
βΊReveal solutionSolution
The family of ellipses with axes along the coordinate axes has the equation a2x2β+b2y2β=1. Eliminating the two arbitrary constants a and b by differentiating twice yields the differential equation xyyβ²β²+x(yβ²)2βyyβ²=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
a2x2β+b2y2β=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:
a22xβ+b22yβyβ²=0.
Divide through by 2:
a2xβ+b2yβyβ²=0.(1)
- Differentiate a second time. Differentiate (1) with respect to x (using the product rule on the second term):
a21β+b21β((yβ²)2+yyβ²β²)=0.(2)
- Eliminate a2 and b2. From (1), we can write
a2xβ=βb2yβyβ²βa21β=βb2yββ xyβ²β.
Substitute this expression for a21β into (2):
βb2yββ xyβ²β+b21β((yβ²)2+yyβ²β²)=0.
Multiply through by b2 (which is nonzero):
- 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 dxdyβ=5x+2yβ32xβ5y+3β, then the equation of that curve is (A) x2+5xyβy2+3xβ3yβ5=0 (B) x2+5xyβy2+3x+3yβ11=0 (C) x2β5xyβy2β3xβ3y+11=0 (D) x2β5xyβy2+3x+3yβ1=0
βΊReveal 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 x2β5xyβy2+3x+3yβ1=0, which is option (D).
The key idea: when a differential equation has the form dxdyβ=aβ²x+bβ²y+cβ²ax+by+cβ, 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 aβ²x+bβ²y+cβ²=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 2xβ5y+3 and the denominator is 5x+2yβ3. Their intersection is found by solving:
{2xβ5y+3=05x+2yβ3=0β
Multiply the first by 2 and the second by 5:
4xβ10y+6=0,25x+10yβ15=0
Adding: 29xβ9=0βx=299β. Substituting back: 2(299β)β5y+3=0β2918β+3=5yβ2918+87β=5yβ29105β=5yβy=2921β.
So the intersection point is (299β,2921β). Shift the origin there by setting:
X=xβ299β,Y=yβ2921β
Then dx=dX, dy=dY, and the differential equation becomes:
dXdYβ=5(X+299β)+2(Y+2921β)β32(X+299β)β5(Y+2921β)+3β
Simplify numerator: 2X+2918ββ5Yβ29105β+3=2Xβ5Y+(2918β105β+3)=2Xβ5Y+(β2987β+3)=2Xβ5Y+(β3+3)=2Xβ5Y.
Denominator: 5X+2945β+2Y+2942ββ3=5X+2Y+(2945+42ββ3)=5X+2Y+(2987ββ3)=5X+2Y+(3β3)=5X+2Y.
Thus the equation reduces to the homogeneous form:
dXdYβ=5X+2Y2Xβ5Yβ
Now set Y=vX, so dXdYβ=v+XdXdvβ. Substitute:
v+XdXdvβ=5X+2vX2Xβ5vXβ=5+2v2β5vβ
Hence:
XdXdvβ=5+2v2β5vββv=5+2v2β5vβv(5+2v)β=5+2v2β5vβ5vβ2v2β=5+2v2β10vβ2v2β
Factor 2:
XdXdvβ=5+2v2(1β5vβv2)β
Separate variables:
1β5vβv25+2vβdv=X2βdX
Integrate both sides. Notice that the derivative of the denominator 1β5vβv2 is β5β2v=β(5+2v). So:
β«1β5vβv25+2vβdv=ββ«1β5vβv2β(5+2v)βdv=βlogβ£1β5vβv2β£+C
Thus:
βlogβ£1β5vβv2β£=2logβ£Xβ£+C
Multiply by -1:
logβ£1β5vβv2β£=β2logβ£Xβ£βC=log(X21β)+constant
Exponentiate:
β£1β5vβv2β£=X2Kβ
where K=eβC>0. Remove the absolute value by allowing K to be any nonzero constant:
1β5vβv2=X2Kβ
Now substitute back v=Y/X:
1β5XYββX2Y2β=X2Kβ
Multiply through by X2:
X2β5XYβY2=K
Recall X=xβ299β, Y=yβ2921β. So:
(xβ299β)2β5(xβ299β)(yβ2921β)β(yβ2921β)2=K
We determine K using the given point (1,1). Substitute x=1, y=1:
(1β299β)2β5(1β299β)(1β2921β)β(1β2921β)2=K
Compute:
1β299β=2920β,1β2921β=298β
So:
(2920β)2β5β 2920ββ 298ββ(298β)2=841400ββ841800ββ84164β=841400β800β64β=841β464β
Thus K=β841464β.
Now the equation is:
(xβ299β)2β5(xβ299β)(yβ2921β)β(yβ2921β)2=β841464β
Multiply both sides by 841=292 to clear denominators:
- 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 (xβx2)dx2d2yβ+y(2β4x)= (A) (1β2x2)dxdyβ (B) (2β4x2)dxdyβ (C) (1β2x)dxdyβ (D) (2β4x)dxdyβ
βΊReveal solutionSolution
We eliminate the two parameters a and b by differentiating twice and substituting back, obtaining a secondβorder linear ODE. The rightβhand side simplifies to (2β4x)dxdyβ, 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 βfreeβ 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, yβ², and yβ²β² β exactly what the question asks.
Stepβbyβstep derivation
- Write the given family and its first two derivatives
y=ae2x+bx2
Differentiate:
dxdyβ=2ae2x+2bx
Differentiate again:
dx2d2yβ=4ae2x+2b
- Eliminate the constant b From yβ²β²=4ae2x+2b, we can solve for b:
2b=yβ²β²β4ae2xβb=2yβ²β²β4ae2xβ
But itβs cleaner to eliminate b by combining yβ² and yβ²β². Notice:
yβ²=2ae2x+2bx
Multiply yβ²β² by x:
xyβ²β²=4axe2x+2bx
Subtract xyβ²β² from yβ²:
yβ²βxyβ²β²=(2ae2x+2bx)β(4axe2x+2bx)=2ae2xβ4axe2x=2ae2x(1β2x)
So we have:
yβ²βxyβ²β²=2ae2x(1β2x)(1)
- Eliminate the constant a From the original equation y=ae2x+bx2, we can also express ae2x:
ae2x=yβbx2
But we already have b from yβ²β²: b=2yβ²β²β4ae2xβ. Substituting that back would reintroduce a. Instead, use equation (1) to solve for ae2x:
2ae2x=1β2xyβ²βxyβ²β²ββae2x=2(1β2x)yβ²βxyβ²β²β
Now plug this into the expression for b from yβ²β²:
yβ²β²=4ae2x+2bβ2b=yβ²β²β4ae2x=yβ²β²β4β 2(1β2x)yβ²βxyβ²β²β
Simplify:
2b=yβ²β²β1β2x2(yβ²βxyβ²β²)β
Multiply both sides by (1β2x):
2b(1β2x)=yβ²β²(1β2x)β2(yβ²βxyβ²β²)
Expand the right side:
yβ²β²(1β2x)β2yβ²+2xyβ²β²=yβ²β²β2xyβ²β²β2yβ²+2xyβ²β²=yβ²β²β2yβ²
So:
2b(1β2x)=yβ²β²β2yβ²βb=2(1β2x)yβ²β²β2yβ²β(2)
- Substitute ae2x and b back into the original equation The original y=ae2x+bx2 becomes:
y=2(1β2x)yβ²βxyβ²β²β+2(1β2x)yβ²β²β2yβ²ββ x2
Multiply both sides by 2(1β2x):
2y(1β2x)=(yβ²βxyβ²β²)+x2(yβ²β²β2yβ²)
Expand the right side:
yβ²βxyβ²β²+x2yβ²β²β2x2yβ²=yβ²β2x2yβ²+(βxyβ²β²+x2yβ²β²)=yβ²(1β2x2)+yβ²β²(x2βx)
So:
2y(1β2x)=yβ²(1β2x2)+yβ²β²(x2βx)
- Rearrange to match the questionβs form Bring the yβ²β² 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=Aeβx+Bcosx as its general solution is (A) (sinxβcosx)dx2d2yβ+2cosxdxdyββ(sinx+cosx)y=0 (B) (cosxβsinx)dx2d2yβ+2cosxdxdyβ+(sinx+cosx)y=0 (C) (cosx+sinx)dx2d2yβ+2sinxdxdyββ(sinxβcosx)y=0 (D) (cosxβsinx)dx2d2yββ2sinxdxdyβ+(cosx+sinx)y=0
βΊReveal solutionSolution
The key idea is to eliminate the arbitrary constants A and B from y=Aeβx+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=Aeβx+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 secondβorder linear ODE. The constants are βhiddenβ 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 eβx and cosx are linearly independent, so the elimination will yield a unique linear relation among y, yβ², and yβ²β² with coefficients that may depend on x.
Stepβbyβstep elimination
- Write down the function and its first two derivatives.
y=Aeβx+Bcosx
Differentiate:
yβ²=βAeβxβBsinx
Differentiate again:
yβ²β²=AeβxβBcosx
- Notice a pattern: we can isolate Aeβx and Bcosx. From y and yβ²β² we have:
y=Aeβx+Bcosx
yβ²β²=AeβxβBcosx
Adding these two equations gives:
y+yβ²β²=2AeβxβAeβx=2y+yβ²β²β
Subtracting the second from the first gives:
yβyβ²β²=2BcosxβBcosx=2yβyβ²β²β
- Now use the first derivative to link these. From yβ²=βAeβxβBsinx, substitute the expressions we found:
yβ²=β2y+yβ²β²ββBsinx
But we also have Bcosx=2yβyβ²β²β, so B=2cosxyβyβ²β²β (provided cosxξ =0, but the final ODE will hold everywhere by continuity). Then:
yβ²=β2y+yβ²β²ββ2cosxyβyβ²β²ββ sinx
Simplify:
yβ²=β2y+yβ²β²ββ2(yβyβ²β²)tanxβ
- Clear denominators and rearrange. Multiply through by 2:
2yβ²=β(y+yβ²β²)β(yβyβ²β²)tanx
2yβ²=βyβyβ²β²βytanx+yβ²β²tanx
Group terms involving yβ²β² and y:
2yβ²=βy(1+tanx)+yβ²β²(tanxβ1)
Multiply both sides by cosx to eliminate the tangent (since tanx=sinx/cosx):
2yβ²cosx=βy(cosx+sinx)+yβ²β²(sinxβcosx) β¦
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