Q.(x) Solution of dxdy=xy+tanxy is sin(xy)=cx. (State True or False.)
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Verifying a Solution of a Differential Equation
A function y=ϕ(x) is called a solution of a differential equation if, when you substitute it and its derivatives into the equation, the two sides become equal for every x in the domain. Verification is the act of carrying out that substitution and checking that it holds as an identity.
The useful point: you do not have to solve the equation to verify a candidate. You are only checking a function that is already handed to you — which is exactly how many exam questions are phrased: "Show that … is a solution of …."
The steps
- From the given y=ϕ(x), compute exactly the derivatives that appear in the equation.
- Substitute y and those derivatives into the left-hand side.
- Simplify and check that it equals the right-hand side for all x (an identity, not just at one point).
Example 1
Verify that y=e−3x is a solution of dx2d2y+dxdy−6y=0.
Here y′=−3e−3x and y′′=9e−3x. Substituting:
9e−3x+(−3e−3x)−6e−3x=(9−3−6)e−3x=0.
The left side is 0 for every x, so y=e−3x is a solution.
Example 2 (a solution with constants)
Verify that y=acosx+bsinx satisfies dx2d2y+y=0 for any constants a,b.
Since y′′=−acosx−bsinx=−y, we get y′′+y=0. It holds for all a,b, so this two-constant family is a solution. …
The key idea is Verification of Solution — substitute the given solution into the differential equation and check if it satisfies the relation.
Step 1: Let v=xy, so y=vx and dxdy=v+xdxdv. The given solution sinv=cx implies xdxdv=sinv after differentiating:
cosv⋅dxdv=c⇒dxdv=cosvc.
Step 2: From sinv=cx, we have c=xsinv. Substitute into dxdv:
dxdv=xcosvsinv=xtanv. …
The given differential equation is a homogeneous equation solved by the substitution y=vx, which leads to the general solution sin(xy)=cx. The statement is True.
The key here is recognising the form of the equation. When you see dxdy expressed as a function of xy alone, you're looking at a homogeneous differential equation. The standard trick — substituting y=vx — turns it into a separable equation that can be integrated directly.
Let's walk through it.
- Rewrite the equation in homogeneous form The given equation is
dxdy=xy+tanxy.
The right-hand side depends only on the ratio xy, so it is homogeneous of degree zero. This tells us the substitution y=vx (where v is a function of x) will work.
- Substitute y=vx Differentiate:
dxdy=v+xdxdv.
Also, xy=v. Plugging into the equation:
v+xdxdv=v+tanv.
- Simplify to a separable form Cancel v on both sides:
xdxdv=tanv.
This is now separable. Rearrange:
tanvdv=xdx.
Since tanv=cosvsinv, we can write:
sinvcosvdv=xdx.
- Integrate both sides The left side integrates to log∣sinv∣ (because the derivative of sinv is cosv), and the right side integrates to log∣x∣+C:
∫sinvcosvdv=∫xdx
log∣sinv∣=log∣x∣+C.
- Solve for the constant Combine the logarithms:
log∣sinv∣=log∣x∣+logc(let C=logc)
log∣sinv∣=log(c∣x∣).
Removing logs (and absorbing the absolute value into the constant c): …
Method: Homogeneous Substitution for dxdy=xy+F(xy)
When the right side is a function of xy, substitute v=xy; the xy term cancels, leaving a clean separable equation in v.
Steps
Step 1: Substitute y=vx.
dxdy=v+xdxdv.
Step 2: Cancel the v term.
With dxdy=v+F(v), the equation reduces to xdxdv=F(v), so F(v)dv=xdx.
Step 3: Integrate and back-substitute v=xy. …
Common Mistakes
Mistake 1: Not substituting v=xy and trying to separate directly.
Why it's wrong: xy+tanxy is a function of the ratio, so only the homogeneous substitution untangles it. Correct approach: put y=vx, use dxdy=v+xdxdv, and the v term cancels.
Mistake 2: Integrating cotv incorrectly. …
Showing the 12 most recent of 86 on this concept.
- TG EAPCET 2021Set eng-2021-08-04-FN1 markMCQQ.The general solution of dxdy=x+sinxcosy+xcosy+sinx is (A) tan2x=2y2−cosy+C (B) tan2y=2x2−cosx+C (C) sec22y=2x2−cosx+C (D) tan2y=2x2+cosx+Cx
›Reveal solutionSolution
The given differential equation is separable after factoring. The solution is found by integrating both sides, leading to tan2y=2x2−cosx+C, which matches option (B).
The key is to notice that the right-hand side can be grouped into terms that depend only on x and terms that depend only on y. That’s the hallmark of a separable differential equation — and once you see the pattern, the integration is straightforward.
Let’s rewrite the equation:
dxdy=x+sinxcosy+xcosy+sinx
Group the terms cleverly:
dxdy=(x+sinx)+(sinxcosy+xcosy)
Factor cosy from the last two terms:
dxdy=(x+sinx)+cosy(x+sinx)
Now factor (x+sinx) out of the whole right-hand side:
dxdy=(x+sinx)(1+cosy)
This is clearly separable: the x-part is (x+sinx) and the y-part is (1+cosy).
- Separate the variables Bring all y terms to the left and x terms to the right:
1+cosydy=(x+sinx)dx
- Integrate both sides The left side uses a standard trigonometric identity. Recall:
1+cosy=2cos22y
So:
1+cosy1=2cos22y1=21sec22y
Therefore:
∫1+cosydy=21∫sec22ydy
Let u=y/2, then dy=2du, and:
21∫sec2u⋅2du=∫sec2udu=tanu+C=tan2y+C
The right side integrates easily:
- TG EAPCET 2023Set eng-2023-05-13-AN1 markMCQQ.The general solution of the differential equation (secx+tanx)dxdy+(sec2x+secxtanx)y=1 is (A) (1+sinx)y=ncosx+c (B) (1+cosx)y=xsinx+c (C) (secx+tanx)y=xsecx+c (D) (secx+tanx)y=x+c
›Reveal solutionSolution
This is a first-order linear ODE. Rewriting it in standard form and applying the integrating factor method shows that the general solution is (secx+tanx)y=x+c, which matches option (D).
The key concept is recognizing the equation as a first-order linear differential equation of the form
dxdy+P(x)y=Q(x).
The standard method is to multiply through by an integrating factor μ(x)=e∫Pdx, which makes the left side a perfect derivative. Here, the coefficients are cleverly arranged so that the integrating factor simplifies dramatically.
- Rewrite in standard form The given equation is
(secx+tanx)dxdy+(sec2x+secxtanx)y=1.
Divide through by (secx+tanx) to isolate dxdy:
dxdy+secx+tanxsec2x+secxtanxy=secx+tanx1.
- Simplify the coefficient of y Factor the numerator: sec2x+secxtanx=secx(secx+tanx). Hence
secx+tanxsec2x+secxtanx=secx.
So the ODE becomes
dxdy+(secx)y=secx+tanx1.
- Find the integrating factor
μ(x)=e∫secxdx.
A standard integral: ∫secxdx=log∣secx+tanx∣+C.
Thus
μ(x)=elog∣secx+tanx∣=secx+tanx.
(We take the positive branch for typical intervals.)
- Multiply through by μ(x)
(secx+tanx)dxdy+(secx+tanx)(secx)y=1.
Notice the left side is exactly the derivative of (secx+tanx)y because
dxd[(secx+tanx)y]=(secx+tanx)dxdy+(secxtanx+sec2x)y, …
- TG EAPCET 2025Set eng-2025-05-02-FN1 markMCQQ.If cosxdxdy=ysinx−1, x=(2n+1)2π, n∈Z is the differential equation corresponding to the curve y=f(x) and f(0)=1 then f(x)= (A) (1−x)secx (B) (1−x)cosx (C) x+cosx (D) x+secx
›Reveal solutionSolution
This is a first-order linear ODE. Rewriting it in standard form and using an integrating factor gives f(x)=(1−x)secx, which matches option (A).
We start with the given differential equation:
cosxdxdy=ysinx−1
The goal is to find y=f(x) satisfying f(0)=1, and then match it to one of the options.
Concept and Intuition
The equation is linear in y but not yet in standard form. The standard form for a first-order linear ODE is:
dxdy+P(x)y=Q(x)
Once in this form, we multiply through by an integrating factor μ(x)=e∫P(x)dx, which lets us write the left-hand side as the derivative of μ(x)y. Then we integrate both sides.
Here, dividing by cosx will give us P(x)=−tanx and Q(x)=−secx. The integrating factor simplifies nicely because ∫tanxdx=−log∣cosx∣, so μ(x)=secx.
Step-by-step solution
- Rewrite in standard form Divide both sides by cosx (valid since x=(2n+1)2π):
dxdy=ytanx−secx
Bring the y term to the left:
dxdy−(tanx)y=−secx
So P(x)=−tanx and Q(x)=−secx.
- Find the integrating factor
μ(x)=e∫P(x)dx=e∫−tanxdx
Since ∫tanxdx=−log∣cosx∣, we have:
∫−tanxdx=log∣cosx∣
Hence:
μ(x)=elog∣cosx∣=∣cosx∣
For the domain (where cosx>0 near x=0), we can take μ(x)=cosx. But it's more standard to use secx as the integrating factor when we multiply through — let's check.
Actually, careful: The standard formula is μ=e∫Pdx. With P=−tanx, we get μ=elog(cosx)=cosx (taking positive branch near 0). So the integrating factor is cosx.
- Multiply the ODE by μ(x)=cosx Original ODE in standard form:
dxdy−(tanx)y=−secx
Multiply by cosx:
cosxdxdy−ysinx=−1
Notice the left side is exactly dxd(ycosx) because:
- TG EAPCET 2026Set eng-2026-05-11-FN1 markMCQQ.The general solution of the differential equation (2xy+y2)dy=(x2−y2)dx is (A) x3−3x2y−y3=c (B) x3−3x2y+y3=c (C) x3−3xy2+y3=c (D) x3−3xy2−y3=c
›Reveal solutionSolution
This is a homogeneous differential equation. Substituting y=vx reduces it to a separable form, and integrating gives the general solution x3−3xy2−y3=c, which matches option (D).
The given equation is (2xy+y2)dy=(x2−y2)dx. Notice that every term is of degree 2 — 2xy, y2, x2, y2 — so the equation is homogeneous. For a homogeneous equation, the standard trick is to set y=vx, which turns the equation into one where variables separate cleanly.
- Rewrite in standard form Bring the dx term to the left:
(2xy+y2)dy−(x2−y2)dx=0
Or equivalently,
dxdy=2xy+y2x2−y2
- Substitute y=vx Then dxdy=v+xdxdv. The right-hand side becomes:
2x(vx)+(vx)2x2−(vx)2=x2(2v+v2)x2(1−v2)=2v+v21−v2
So the equation is:
v+xdxdv=2v+v21−v2
- Separate variables Subtract v from both sides:
xdxdv=2v+v21−v2−v=2v+v21−v2−v(2v+v2)
Simplify the numerator:
1−v2−2v2−v3=1−3v2−v3
So:
xdxdv=2v+v21−3v2−v3
Now separate:
1−3v2−v32v+v2dv=xdx
- Integrate both sides The left-hand side is set up for a simple substitution. Let u=1−3v2−v3. Then du=(−6v−3v2)dv=−3(2v+v2)dv. Notice that 2v+v2 appears in the numerator, so:
1−3v2−v32v+v2dv=−31udu
Integrating:
∫−31udu=∫xdx
−31log∣u∣=log∣x∣+C
Multiply by −3:
log∣u∣=−3log∣x∣−3C …
- TG EAPCET 2024Set eng-2024-05-10-AN1 markMCQQ.If y=sinx+Acosx is the general solution of dxdy+f(x)y=secx, then an integrating factor of the differential equation is (A) secx (B) tanx (C) cosx (D) sinx
›Reveal solutionSolution
The given general solution is y=sinx+Acosx. Differentiating and substituting into the differential equation reveals f(x)=tanx, so the integrating factor is secx, which is option (A).
We are told that y=sinx+Acosx (where A is an arbitrary constant) is the general solution of
dxdy+f(x)y=secx.
Our goal is to find the integrating factor (I.F.) of this linear first-order ODE. The standard form is y′+P(x)y=Q(x), and the integrating factor is μ(x)=e∫P(x)dx. Here P(x)=f(x).
The key insight: If we already know the general solution, we can work backwards to find f(x) by differentiating the solution and plugging it into the equation. Then we compute the integrating factor directly.
-
Differentiate the given general solution
y=sinx+Acosx
dxdy=cosx−Asinx
-
Substitute into the differential equation
The equation is dxdy+f(x)y=secx.
So:
(cosx−Asinx)+f(x)(sinx+Acosx)=secx
- Group terms involving A and those without A Expand:
cosx−Asinx+f(x)sinx+Af(x)cosx=secx
Group constant (in A) terms: cosx+f(x)sinx
Group A terms: A(−sinx+f(x)cosx)
Since this must hold for all A (the solution is general), the coefficient of A must be zero. That gives:
−sinx+f(x)cosx=0⇒f(x)cosx=sinx⇒f(x)=tanx
- Verify the constant part With f(x)=tanx, the constant part becomes: cosx+tanx⋅sinx=cosx+cosxsin2x=cosxcos2x+sin2x=cosx1=secx …
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- TG EAPCET 2023Set eng-2023-05-12-FN1 markMCQQ.The general solution of dxdy+yf′(x)−f(x)f′(x)=0,y=f(x) is (A) y=f(x)+1+ce−f(x) (B) y=ce−f(x) (C) y=f(x)−1+ce−f(x) (D) y=f(x)+cef(x)
›Reveal solutionSolution
This is a first-order linear ODE disguised by the presence of f(x) and f′(x). By rewriting it in standard form and using an integrating factor ef(x), the general solution simplifies to y=f(x)−1+ce−f(x), which corresponds to option (C).
We start with the given differential equation:
dxdy+yf′(x)−f(x)f′(x)=0,y=f(x).
Concept & Intuition
The equation looks messy because of the f(x) and f′(x) terms, but notice that f′(x) appears as a coefficient of y and also multiplied by f(x). This suggests we can rearrange it into the standard linear form dxdy+P(x)y=Q(x), where P(x) and Q(x) are functions of x only. Once in that form, the method of integrating factor works cleanly. The key trick: treat f(x) as some known function (we don't need its explicit form), and f′(x) as its derivative.
Step-by-step solution
- Rewrite the equation in standard linear form Bring the term −f(x)f′(x) to the right-hand side:
dxdy+f′(x)y=f(x)f′(x).
This is now of the form dxdy+P(x)y=Q(x) with P(x)=f′(x) and Q(x)=f(x)f′(x).
- Find the integrating factor The integrating factor μ(x) is given by e∫P(x)dx. Here:
∫P(x)dx=∫f′(x)dx=f(x)+C.
We only need one integrating factor, so take μ(x)=ef(x).
- Multiply through by the integrating factor
ef(x)dxdy+ef(x)f′(x)y=ef(x)f(x)f′(x).
The left-hand side is the derivative of yef(x) with respect to x (by the product rule, since dxdef(x)=ef(x)f′(x)). So we have:
dxd(yef(x))=ef(x)f(x)f′(x).
- Integrate both sides
yef(x)=∫ef(x)f(x)f′(x)dx.
Notice that the integrand is set up for a substitution: let u=f(x), then du=f′(x)dx, so:
∫euudu.
This is a standard integral. Use integration by parts: let w=u, dv=eudu, then dw=du, v=eu. So:
∫ueudu=ueu−∫eudu=ueu−eu+C=eu(u−1)+C. …
- TG EAPCET 2025Set eng-2025-05-03-FN1 markMCQQ.If the differential equation having y=Aex+Bsinx as its general solution is f(x)dx2d2y+g(x)dxdy+h(x)y=0, then f(x)+g(x)+h(x)= (A) cosx−sinx (B) 4sinx (C) 2cosx (D) 0
›Reveal solutionSolution
Eliminating A,B from y=Aex+Bsinx gives (cosx−sinx)y′′+2sinxy′−(sinx+cosx)y=0, so f+g+h=0 — option (D).
Concept. A two‑parameter family y=Aex+Bsinx satisfies a second‑order ODE obtained by eliminating A and B from y,y′,y′′. The Wronskian‑style determinant of {y,ex,sinx} vanishing is exactly that eliminant.
Solution.
- Differentiate:
y=Aex+Bsinx,y′=Aex+Bcosx,y′′=Aex−Bsinx.
- A non‑trivial (A,B) exists iff yy′y′′exexexsinxcosx−sinx=0. …
- TG EAPCET 2026Set eng-2026-05-11-AN1 markMCQQ.The integrating factor of the linear differential equation in x given by dxdy=3x+y+21 is (A) e−3x (B) e−x (C) e−3y (D) e−y
›Reveal solutionSolution
The given equation is not linear in y, but rewriting it as dydx=3x+y+2 makes it linear in x with integrating factor e−3y, so the correct option is (C).
We are given
dxdy=3x+y+21.
At first glance, this looks like a first-order differential equation in y as a function of x. But it is not linear in y because the right-hand side is a rational function containing y in the denominator. However, we can flip the relationship: treat x as a function of y instead.
The key insight: if dxdy is given, then dydx=1/dxdy (provided the derivative is nonzero). This often turns a nonlinear equation in y into a linear equation in x.
- Rewrite the equation in terms of x(y) Since dydx=dxdy1, we have
dydx=3x+y+2.
This is now a linear first-order differential equation in x with independent variable y.
- Identify the standard linear form The standard form for a linear ODE in x is
dydx+P(y)x=Q(y).
Our equation is
dydx−3x=y+2.
So P(y)=−3 and Q(y)=y+2.
- Recall the integrating factor formula For a linear ODE dydx+P(y)x=Q(y), the integrating factor is
μ(y)=e∫P(y)dy.
Here P(y)=−3, so
μ(y)=e∫(−3)dy=e−3y.
- Interpret the result …
- TG EAPCET 2022Set eng-2022-07-20-AN1 markMCQQ.If l and m are respectively the order and the degree of the differential equation f(x)y′′+g(x)y′=x4y whose general solution is y=ax2+blogx, then f(m)+g(m)= (A) 2l (B) l (C) 3m (D) 1+m
›Reveal solutionSolution
The key idea is to find the differential equation from its given general solution, then identify its order l and degree m, and finally evaluate f(m)+g(m) — the answer is l.
We are told that the general solution of the differential equation
f(x)y′′+g(x)y′=x4y
is y=ax2+blogx, where a and b are arbitrary constants. The functions f(x) and g(x) are not given explicitly — they are to be determined from the fact that this y satisfies the equation for all a,b.
The problem asks for f(m)+g(m), where l is the order and m is the degree of this differential equation. So we first need to find the differential equation itself.
- Find the derivatives of the given solution.
y=ax2+blogx
Differentiate:
y′=2ax+xb
Differentiate again:
y′′=2a−x2b
-
Eliminate the arbitrary constants a and b.
We have three equations: y, y′, y′′ in terms of a and b. We need one equation relating y, y′, y′′ and x alone — that is the differential equation.
From y′′=2a−x2b, we can solve for a and b in terms of y′′ and something else. But a cleaner way:
From y′=2ax+xb, multiply by x:
xy′=2ax2+b
From y=ax2+blogx, we have ax2=y−blogx. Substitute into xy′:
xy′=2(y−blogx)+b=2y−2blogx+b
This still has b. Instead, let's use y′′ directly.
From y′′=2a−x2b, multiply by x2:
x2y′′=2ax2−b
But 2ax2=2(y−blogx) from y=ax2+blogx. So:
x2y′′=2y−2blogx−b
This still contains b. We need another relation to eliminate b.
From y′=2ax+xb, multiply by x:
xy′=2ax2+b
And 2ax2=2(y−blogx). So:
xy′=2y−2blogx+b
Now subtract the x2y′′ equation from this? Let's do it systematically.
We have:
xy′=2y−2blogx+b(1)
x2y′′=2y−2blogx−b(2)
Subtract (2) from (1):
xy′−x2y′′=(2y−2blogx+b)−(2y−2blogx−b)=2b
So b=21(xy′−x2y′′).
Now add (1) and (2):
xy′+x2y′′=(2y−2blogx+b)+(2y−2blogx−b)=4y−4blogx
Substitute b:
xy′+x2y′′=4y−4(21(xy′−x2y′′))logx
xy′+x2y′′=4y−2(xy′−x2y′′)logx
Bring terms together:
xy′+x2y′′+2(xy′−x2y′′)logx=4y
Factor:
- TG EAPCET 2026Set eng-2026-05-10-FN1 markMCQQ.If y=(x+x2+1)5 then 25y= (A) (x2+1)y2−xy1 (B) (x2+1)y2+xy1 (C) (x2+1)y2−2xy1 (D) (x2+1)y2+2xy1
›Reveal solutionSolution
The function y=(x+x2+1)5 is a power of an inverse hyperbolic sine, so its derivatives satisfy a simple recurrence. Differentiating twice and rearranging gives 25y=(x2+1)y2+xy1, which is option (B).
We have y=(x+x2+1)5. The expression inside the parentheses is the standard form for the inverse hyperbolic sine: sinh−1x=log(x+x2+1), so x+x2+1=esinh−1x. That means y=e5sinh−1x. This is a composition that makes differentiation clean: the derivative of sinh−1x is x2+11, and the chain rule will produce a pattern that eliminates the square root.
The key insight: instead of brute-force expanding, we can find a relation between y, y1=dxdy, and y2=dx2d2y by differentiating the defining equation. Notice that x+x2+1 satisfies a neat property: its reciprocal is x2+1−x. This will help us isolate derivatives.
- First derivative. Let u=x+x2+1. Then y=u5, and dxdu=1+x2+1x=x2+1x2+1+x=x2+1u. So by the chain rule:
y1=5u4⋅dxdu=5u4⋅x2+1u=x2+15u5=x2+15y.
Hence
x2+1y1=5y.(1)
- Second derivative. Differentiate (1) with respect to x. The left side is a product:
dxd(x2+1y1)=x2+1xy1+x2+1y2.
The right side differentiates to 5y1. So: …
- TG EAPCET 2022Set eng-2022-07-19-AN1 markMCQQ.Assertion (A): The curves y2=4x and x2=−2y intersect at (1,2) orthogonally. Reason (R): If the product of the slopes of the tangents drawn to two curves at their point of intersection is −1, then the curves are said to cut each other orthogonally. 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
The assertion claims the curves intersect orthogonally at (1,2), but (1,2) is not an intersection point of the curves. The reason correctly defines orthogonal intersection. Thus, Assertion (A) is false, and Reason (R) is true.
When we talk about two curves intersecting orthogonally, we mean that at their point of intersection, the tangents to each curve are perpendicular to each other. The condition for two lines to be perpendicular is that the product of their slopes is −1.
Let's analyze the given assertion and reason.
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Analyze Assertion (A): The curves y2=4x and x2=−2y intersect at (1,2) orthogonally.
First, we must verify if the point (1,2) is indeed a point of intersection for both curves. A point of intersection must satisfy the equations of both curves.
-
For the curve y2=4x:
Substitute x=1 and y=2:
22=4(1)
4=4
This is true, so (1,2) lies on the curve y2=4x.
-
For the curve x2=−2y:
Substitute x=1 and y=2:
12=−2(2)
1=−4
This is false. The point (1,2) does not lie on the curve x2=−2y.
Since (1,2) does not lie on both curves, it cannot be a point of intersection. Therefore, the assertion that the curves intersect at (1,2) is false.
Watch outIt is crucial to first check if the given point is an actual point of intersection. If it's not, then any claim about the nature of intersection (like orthogonality) at that point is automatically false, regardless of what the slopes might suggest if we were to calculate them there.
Even though the assertion is already false, for a complete understanding, let's briefly check the orthogonality condition if (1,2) were an intersection point.
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Slope of tangent to y2=4x at (1,2):
Differentiate y2=4x implicitly with respect to x:
2ydxdy=4
dxdy=2y4=y2
At (1,2), the slope m1=22=1.
-
Slope of tangent to x2=−2y at (1,2):
Differentiate x2=−2y implicitly with respect to x:
2x=−2dxdy
dxdy=−22x=−x
At (1,2), the slope m2=−1. …
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- TG EAPCET 2025Set eng-2025-05-02-AN1 markMCQQ.Consider the following statements Assertion (A): When x,y,z are positive numbers, then
[!FORMULA] tan−1(yzx(x+y+z))+tan−1(xzy(x+y+z))+tan−1(xyz(x+y+z))=π
Reason (R): tan−1a+tan−1b=tan−1(1−aba+b) if a>0 & b>0 The correct answer is (A) Both (A) and (R) are true, (R) is the correct explanation of (A) (B) Both (A) and (R) are true, (R) is not the correct explanation of (A) (C) (A) is true, but (R) is false (D) (A) is false, but (R) is true›Reveal solutionSolution
The three inverse tangents really do add to π, because their tangents satisfy a+b+c=abc. But the Reason omits the essential restriction ab<1, so it is false as printed. (A) true, (R) false — option (C).
The concept first
If A+B+C=π then tanA+tanB+tanC=tanAtanBtanC; and conversely, if a,b,c>0 satisfy
a+b+c=abc,
then tan−1a+tan−1b+tan−1c=π (each term lies in (0,π/2), so the sum lies in (0,3π/2) and π is the only multiple of π available).
The second-hand tool, tan−1a+tan−1b=tan−11−aba+b, is where students lose marks. For a,b>0 the true statement is
tan−1a+tan−1b=⎩⎨⎧tan−11−aba+b,π+tan−11−aba+b,ab<1,ab>1,
because the left side can exceed π/2, whereas tan−1 can never return more than π/2.
Step 1 — Test the Assertion
Put s=x+y+z and
a=yzxs,b=zxys,c=xyzs.
Then
abc=x2y2z2xyzs3=xyzs3/2,
a+b+c=xyzs(x+y+z)=xyzs3/2.
They are equal, so a+b+c=abc and therefore the sum of the three inverse tangents is π. (A) is true. Quick check with x=y=z=1: each term is tan−13=3π, and 3×3π=π. ✓
Step 2 — Test the Reason …
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