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Question: Verify Euler’s theorem for the equation \(f\left( x,y \right)=\dfrac{1}{\sqrt{{{x}^{2}}+{{y}^{2}}}}\...

Verify Euler’s theorem for the equation f(x,y)=1x2+y2f\left( x,y \right)=\dfrac{1}{\sqrt{{{x}^{2}}+{{y}^{2}}}}

Explanation

Solution

Hint: Euler’s theorem for any homogenous f(x,y)f\left( x,y \right) is given as
xfx+yfy=nf(x,y)x\dfrac{\partial f}{\partial x}+y\dfrac{\partial f}{\partial y}=nf\left( x,y \right) , where n is the degree of the homogeneous function. Determine the value of ‘n’ by expression
f(λx,λy)=λnf(x,y)f\left( \lambda x,\lambda y \right)={{\lambda }^{n}}f\left( x,y \right)
fx\dfrac{\partial f}{\partial x} means differentiate the given function w.r.t x'x' by taking as y'y' a constant and fy\dfrac{\partial f}{\partial y} means differentiation of the function w.r.t y'y' by taking x'x' as a constant. Use the relation ddxxn=nxn1\dfrac{d}{dx}{{x}^{n}}=n{{x}^{n-1}} wherever necessary.

Complete step-by-step solution -
As, we know the Euler’s theorem for any homogeneous function f(x,y)f\left( x,y \right) of degree n is given as
xfx+yfy=nf(x,y)..........(i)x\dfrac{\partial f}{\partial x}+y\dfrac{\partial f}{\partial y}=nf\left( x,y \right)..........\left( i \right)
And we can verify any function to be homogeneous or not by the relation
f(λx,λy)=λnf(x,y)........(ii)f\left( \lambda x,\lambda y \right)={{\lambda }^{n}}f\left( x,y \right)........\left( ii \right)
Where ‘n’ is the degree of a homogeneous equation.
It means if any function follows equation(ii), then it will be a homogeneous function and ‘n’ is the degree of the equation.
Now, coming to the question, we are given the function f(x,y)f\left( x,y \right) in the problem as
f(x,y)=1x2+y2.........(iii)f\left( x,y \right)=\dfrac{1}{\sqrt{{{x}^{2}}+{{y}^{2}}}}.........\left( iii \right)
Now, we can calculate value of f(λx,λy)f\left( \lambda x,\lambda y \right) from the equation (iii) as
f(λx,λy)=1(λx)2+(λy)2 f(λx,λy)=1λ2(x2+y2) f(λx,λy)=1λ1x2+y2 f(λx,λy)=λ1f(x,y) \begin{aligned} & f\left( \lambda x,\lambda y \right)=\dfrac{1}{\sqrt{{{\left( \lambda x \right)}^{2}}+{{\left( \lambda y \right)}^{2}}}} \\\ & f\left( \lambda x,\lambda y \right)=\dfrac{1}{\sqrt{{{\lambda }^{2}}\left( {{x}^{2}}+{{y}^{2}} \right)}} \\\ & f\left( \lambda x,\lambda y \right)=\dfrac{1}{\lambda }\dfrac{1}{\sqrt{{{x}^{2}}+{{y}^{2}}}} \\\ & f\left( \lambda x,\lambda y \right)={{\lambda }^{-1}}f\left( x,y \right) \\\ \end{aligned}
Now, we can compare the above relation by equation (ii) and hence, we get degree of the given function as
n = -1 ………..(iv)
Now, we have to verify the relation of equation (i), so let us calculate fx\dfrac{\partial f}{\partial x} and fy\dfrac{\partial f}{\partial y} by following approach
We have f(x,y)=1x2+y2=(x2+y2)12f\left( x,y \right)=\dfrac{1}{\sqrt{{{x}^{2}}+{{y}^{2}}}}={{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{-1}{2}}}
Now, we can calculate fx\dfrac{\partial f}{\partial x} by differentiating the above function with respect to x'x' by taking y'y' as a constant.
We know
ddxxn=nxn1........(v)\dfrac{d}{dx}{{x}^{n}}=n{{x}^{n-1}}........\left( v \right)
So, we get fx\dfrac{\partial f}{\partial x} as

& \dfrac{\partial f}{\partial x}=\dfrac{\partial }{\partial x}{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{-1}{2}}} \\\ & \dfrac{\partial f}{\partial x}=-\dfrac{1}{2}{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{-1}{2}-1}}\times \dfrac{\partial }{\partial x}\left( {{x}^{2}}+{{y}^{2}} \right) \\\ \end{aligned}$$ Now, $'y'$ is acting as a constant. So, we know $\dfrac{d}{dx}\text{constant = 0}$ . Hence, we get $$\begin{aligned} & \dfrac{\partial f}{\partial x}=\dfrac{-1}{2}{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{-3}{2}}}\left( 2x \right) \\\ & \dfrac{\partial f}{\partial x}=\dfrac{-1}{2{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{3}{2}}}}\times 2x \\\ & \dfrac{\partial f}{\partial x}=\dfrac{-x}{{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{3}{2}}}}..............\left( vi \right) \\\ \end{aligned}$$ Now, we can calculate $\dfrac{\partial f}{\partial y}$ by differentiating $f\left( x,y \right)$ with respect to $y$ by taking $'x'$ as a constant. So, we get $\begin{aligned} & \dfrac{\partial f}{\partial y}=\dfrac{\partial }{\partial y}\left( \dfrac{1}{{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{1}{2}}}} \right) \\\ & \dfrac{\partial f}{\partial y}=\dfrac{\partial }{\partial y}{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{-1}{2}}} \\\ \end{aligned}$ Now, using the relation (v) , we get $\dfrac{\partial f}{\partial y}=-\dfrac{1}{2}{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{-\dfrac{1}{2}-1}}\times \dfrac{\partial }{\partial y}\left( {{x}^{2}}+{{y}^{2}} \right)$ Now as $'x'$ is acting as a constant, so we know $\dfrac{d}{dy}\text{constant}=0$ .Hence we get $$\begin{aligned} & \dfrac{\partial f}{\partial y}=\dfrac{-1}{2}{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{-3}{2}}}\times \left( 2y \right) \\\ & =\dfrac{-1}{2{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{3}{2}}}}\times 2y \\\ & \dfrac{\partial f}{\partial y}=\dfrac{-y}{{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{3}{2}}}}...........\left( vii \right) \end{aligned}$$ Now, left hand side of the equation(i) is given with the help of equation(vi) and (vii) as $\begin{aligned} & L.H.S.=x\dfrac{\partial f}{\partial x}+y\dfrac{\partial f}{\partial y} \\\ & L.H.S.=x\left( \dfrac{-x}{{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{3}{2}}}} \right)+y\left( \dfrac{-y}{{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{3}{2}}}} \right) \\\ & L.H.S.=\dfrac{-{{x}^{2}}}{{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{3}{2}}}}+\dfrac{-{{y}^{2}}}{{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{3}{2}}}} \\\ & L.H.S.=\dfrac{-1}{{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{\dfrac{3}{2}}}}\left( {{x}^{2}}+{{y}^{2}} \right) \\\ \end{aligned}$ Now, we know the property of surds $\dfrac{{{a}^{m}}}{{{a}^{n}}}={{a}^{m-n}}$ So, we get the value of L.H.S. as $\begin{aligned} & L.H.S.=-1\times {{\left( {{x}^{2}}+{{y}^{2}} \right)}^{1-\dfrac{3}{2}}} \\\ & L.H.S.=-1{{\left( {{x}^{2}}+{{y}^{2}} \right)}^{-\dfrac{1}{2}}} \\\ & L.H.S.=\dfrac{-1}{\sqrt{{{x}^{2}}+{{y}^{2}}}}..........\left( ix \right) \\\ \end{aligned}$ Now, we can get value of Right-hand side of the equation(i) as $\begin{aligned} & R.H.S.=nf\left( x,y \right) \\\ & R.H.S.=-1\times \dfrac{1}{\sqrt{{{x}^{2}}+{{y}^{2}}}} \\\ \end{aligned}$ Where, we know the value of ‘n’ is -1 from the equation(iv). So, we get $R.H.S.=\dfrac{-1}{\sqrt{{{x}^{2}}+{{y}^{2}}}}..........\left( x \right)$ Hence, we get the equation (ix) and (x) such that the RHS and LHS of the equation(i) are equal to each other. So, we get $L.H.S.=R.H.S.=\dfrac{-1}{\sqrt{{{x}^{2}}+{{y}^{2}}}}$ Therefore, the Euler theorem is verified with the given equation. Note: One may go wrong with the calculation of $\dfrac{\partial f}{\partial x}$ and $\dfrac{\partial f}{\partial y}$ . As both are confusing i.e. one needs to know where we need to differentiate the function by taking $'x'$ as a constant and where we need to take $'y'$ as a constant. So, one needs to be clear with all these concepts. One may go wrong if he/she put the degree of the given equation as ‘2’ by confusing with the powers of $'x'$ and $'y'$ in the given function i.e. $f\left( x,y \right)=\dfrac{1}{\sqrt{{{x}^{2}}+{{y}^{2}}}}$ . So, always try to verify any homogeneous relation by equation. $f\left( \lambda x,\lambda y \right)={{\lambda }^{n}}\left( f\left( x,y \right) \right)$ and get the degree of given equation by calculating the ‘n’ from above mentioned equation.