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Question

Question: The curve amongst the family of curves, represented by the differential equation, \(\left( {{x}^{2}}...

The curve amongst the family of curves, represented by the differential equation, (x2y2)dx+2xydy=0\left( {{x}^{2}}-{{y}^{2}} \right)dx+2xydy=0 which passes through the point (1,1) is
A. A circle with center on the y-axis
B. A circle with center on the x-axis
C. An ellipse with major axis along the y-axis
D. A hyperbola with transverse axis along the x-axis

Explanation

Solution

Hint: In this question, the equation of the curve is given in differential form i.e. involving dx and dy. Therefore, we should first try to solve the equation to obtain the equation of the curve involving only x and y. Then, we can match it with the curves given in the options and choose the correct answer.

Complete step-by-step answer:
The given equation of the curve is
(x2y2)dx+2xydy=0 dydx=y2x22xy...............(1.1) \begin{aligned} & \left( {{x}^{2}}-{{y}^{2}} \right)dx+2xydy=0 \\\ & \Rightarrow \dfrac{dy}{dx}=\dfrac{{{y}^{2}}-{{x}^{2}}}{2xy}...............(1.1) \\\ \end{aligned}
We find that in the RHS of equation (1.1), the degree of the terms i.e. the total power of x and y of each term in the numerator and the denominator is 2. Therefore, this is the case of a homogeneous differential equation.
Therefore, we can take y=vxy=vx for some function v. Therefore, taking derivative on both sides of y=vxy=vx, we obtain
dydx=d(vx)dx=vdxdx+xdvdx=v+xdvdx..........(1.2)\dfrac{dy}{dx}=\dfrac{d(vx)}{dx}=v\dfrac{dx}{dx}+x\dfrac{dv}{dx}=v+x\dfrac{dv}{dx}..........(1.2)
And putting y=vxy=vx in the RHS of equation (1.1), we obtain
y2x22xy=(vx)2x22x×vx=x2(v21)x2×2v=(v21)2v..............(1.3)\dfrac{{{y}^{2}}-{{x}^{2}}}{2xy}=\dfrac{{{\left( vx \right)}^{2}}-{{x}^{2}}}{2x\times vx}=\dfrac{{{x}^{2}}\left( {{v}^{2}}-1 \right)}{{{x}^{2}}\times 2v}=\dfrac{\left( {{v}^{2}}-1 \right)}{2v}..............(1.3)
Therefore, using equations (1.2) and (1.3), we can rewrite equation (1.1) as
dydx=y2x22xy v+xdvdx=v212v \begin{aligned} & \dfrac{dy}{dx}=\dfrac{{{y}^{2}}-{{x}^{2}}}{2xy} \\\ & \Rightarrow v+x\dfrac{dv}{dx}=\dfrac{{{v}^{2}}-1}{2v} \\\ \end{aligned}
Now, we can separate the terms involving v and x in the last line of the above equation to write it as
xdvdx=v212vv=v212v22v=(v2+1)2v 2vdv(v2+1)=dxx.................(1.4) \begin{aligned} & x\dfrac{dv}{dx}=\dfrac{{{v}^{2}}-1}{2v}-v=\dfrac{{{v}^{2}}-1-2{{v}^{2}}}{2v}=\dfrac{-\left( {{v}^{2}}+1 \right)}{2v} \\\ & \Rightarrow \dfrac{2vdv}{\left( {{v}^{2}}+1 \right)}=\dfrac{-dx}{x}.................(1.4) \\\ \end{aligned}
Now, we know that the integral of 1x\dfrac{1}{x} is given by
1xdx=logx+C............(1.5)\int{\dfrac{1}{x}dx}=\log x+C............(1.5)
Where C is an arbitrary constant.
Again, if we take
v2+1=s 2vdv=ds..............(1.6) \begin{aligned} & {{v}^{2}}+1=s \\\ & \Rightarrow 2vdv=ds..............(1.6) \\\ \end{aligned}
in LHS of equation (1.4), we can write it as
2vdv(v2+1)=dss.................(1.7)\dfrac{2vdv}{\left( {{v}^{2}}+1 \right)}=\dfrac{ds}{s}.................(1.7)
Therefore, we can rewrite equation (1.4) using (1.7) as
dss=dxx\dfrac{ds}{s}=-\dfrac{dx}{x}
Taking integral on both sides and using equation (1.5), we obtain
dss=dxx logs+C1=logx+C2 logs=logx+C3 \begin{aligned} & \int{\dfrac{ds}{s}}=-\int{\dfrac{dx}{x}} \\\ & \Rightarrow \log s+{{C}_{1}}=-\log x+{{C}_{2}} \\\ & \Rightarrow \log s=-\log x+{{C}_{3}} \\\ \end{aligned}
Where C1{{C}_{1}} and C2{{C}_{2}} are arbitrary constants and C3=C2C1{{C}_{3}}={{C}_{2}}-{{C}_{1}} which is also a constant. Taking exponentials on both sides and using the fact that logx=log(1x)-\log x=\log \left( \dfrac{1}{x} \right) and elogx=x{{e}^{\log x}}=x for any value of x, we have
logs=logx+C3=log(1x)+C3 elogs=elog(1x)+C3=elog(1x)×eC3 s=1x×C4...................(1.8) \begin{aligned} & \log s=-\log x+{{C}_{3}}=\log \left( \dfrac{1}{x} \right)+{{C}_{3}} \\\ & \Rightarrow {{e}^{\log s}}={{e}^{\log \left( \dfrac{1}{x} \right)+{{C}_{3}}}}={{e}^{\log \left( \dfrac{1}{x} \right)}}\times {{e}^{{{C}_{3}}}} \\\ & \Rightarrow s=\dfrac{1}{x}\times {{C}_{4}}...................(1.8) \\\ \end{aligned}
Where C4=eC3{{C}_{4}}={{e}^{{{C}_{3}}}} is another constant. Now, rewriting the value of s as s=v2+1s={{v}^{2}}+1 and v=yxv=\dfrac{y}{x}, we can rewrite equation (1.8) as
s=1x×C4 (yx)2+1=C4x...................(1.9) \begin{aligned} & s=\dfrac{1}{x}\times {{C}_{4}} \\\ & \Rightarrow {{\left( \dfrac{y}{x} \right)}^{2}}+1=\dfrac{{{C}_{4}}}{x}...................(1.9) \\\ \end{aligned}
Which is the equation of the curve. As it passes through (1,1), x=1 and y=1 should satisfy equation (1.9), therefore, we should have
(11)2+1=C41 C4=2 \begin{aligned} & {{\left( \dfrac{1}{1} \right)}^{2}}+1=\dfrac{{{C}_{4}}}{1} \\\ & \Rightarrow {{C}_{4}}=2 \\\ \end{aligned}
Therefore, we can use this value of C4{{C}_{4}} in equation (1.9) to obtain
(yx)2+1=2x x2+y22x=0...................(1.10) \begin{aligned} & {{\left( \dfrac{y}{x} \right)}^{2}}+1=\dfrac{2}{x} \\\ & \Rightarrow {{x}^{2}}+{{y}^{2}}-2x=0...................(1.10) \\\ \end{aligned}
Now, we see that the degree and the coefficient of the terms with highest degree of both x and y in (1.10) is same. Therefore, it represents a circle. Comparing (1.10) with the general equation of a circle with center at (-g,-f) is given by
x2+y2+2gx+2fy+c=0{{x}^{2}}+{{y}^{2}}+2gx+2fy+c=0
Comparing it with equation (1.10), we find that g=-1 and f=0. Therefore, the center of the circle represented by (1.10) should lie at (-1,0) and thus on the x-axis as the y-coordinate is 0.
Therefore, option (b) is the correct answer.

Note: We should note that in equation (1.8), we put all the constant terms on one side and renamed it as C4{{C}_{4}}. We could do it because as C1{{C}_{1}}, C2{{C}_{2}} and C3{{C}_{3}} were arbitrary constants and their values were not determined and in the final equations just C4{{C}_{4}} appeared, therefore, we could find the equation of the curve using C4{{C}_{4}} only and not C1,C2{{C}_{1}},{{C}_{2}} or C3{{C}_{3}}.