Cubic equation solutions form

AI Thread Summary
The discussion focuses on the solutions to cubic equations expressed in terms of trigonometric functions and Vieta's formulas. The roots are defined using the variable t and the angle φ, leading to specific expressions for x1, x2, and x3. The equations derived from Vieta's formulas are shown to be satisfied, but the author initially struggles to solve for t and φ. A hint leads to the expansion of angles and the introduction of complex numbers to express the roots more clearly. Ultimately, relationships between the coefficients p and q are established, highlighting conditions necessary for the cubic equation's solutions.
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Homework Statement
Assume that a cubic equation has three real solutions. Show that the solutions of the cubic equation are of the form - see below.
Relevant Equations
Vieta’s formulae, discriminant.
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Let's denote ##\sqrt[3] r =t##. The three expressions above can be written as $$x_1=2t \cos \frac {\phi} 3, x_2=t (-\cos \frac {\phi} 3 -\sin \frac {\phi} 3), x_3=t (-\cos \frac {\phi} 3 +\sin \frac {\phi} 3)$$ The Vieta's formulae for the given equation are $$x_1+x_2+x_3=0$$ $$x_1 x_2+ x_2 x_3 + x_1 x_3 = p$$ $$x_1 x_2 x_3 = -q$$
The first equation is obviously satisfied by these ##x_1, x_2, x_3##. The second becomes $$t^2(2 \cos^2 \frac {\phi} 3 - 1)=p$$ and the third, $$2t^3 \cos \frac {\phi} 3 (2 \cos^2 \frac {\phi} 3 - 1)=-q$$ I hoped to see that the last two equations can be always solved for the ##t## and ##\phi## as required, but I don't.

P.S. I've got a hint and solved it. Closed.
 
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It might help to expand the angles correctly: \begin{split}<br /> \cos((\phi + 2\pi)/3) = \cos(\phi/3)\cos(2\pi/3) - \sin(\phi/3)\sin(2\pi/3) = - \tfrac12\cos(\phi/3) + \tfrac12 \sqrt{3}\sin(\phi/3) \\<br /> \cos((\phi + 4\pi)/3) = \cos(\phi/3)\cos(4\pi/3) - \sin(\phi/3)\sin(4\pi/3) = - \tfrac12\cos(\phi/3) - \tfrac12 \sqrt{3}\sin(\phi/3) \end{split}
 
Set \alpha = e^{i\phi/3} so that the roots are \begin{split}<br /> x_1 &amp;= r^{1/3}(\alpha + \bar{\alpha}) \\<br /> x_2 &amp;= r^{1/3}(\alpha\omega + \bar{\alpha}\omega^2) \\<br /> x_3 &amp;= r^{1/3}(\alpha\omega^2 + \bar{\alpha}\omega)\end{split} where \omega = e^{2\pi i/3} satisfies \omega^2 = \bar{\omega} and 1 + \omega + \omega^2 = 0. Defining \begin{split}<br /> s_0 &amp;= x_1 + x_2 + x_3 = 0\\<br /> s_1 &amp;= x_1 + \omega x_2 + \omega^2 x_3 = 3r^{1/3} \bar{\alpha} \\<br /> s_2 &amp;= x_1 + \omega^2 x_2 + \omega x_3 = 3r^{1/3}\alpha \end{split} we find that <br /> \begin{split}<br /> s_1^3 + s_2^3 &amp;= -27q = 27r(\alpha^3 + \bar{\alpha}^3) = 54r\cos \phi \\<br /> s_1^3s_2^3 &amp;= (-3p)^3 = 27^2r^2\end{split} and hence <br /> \begin{split}<br /> r^2 &amp;= -\frac{p^3}{27} \\<br /> r\cos\phi &amp;= -\frac{q}{2} \end{split} (Note that p &lt; 0 is a necesary condition for 4p^3 + 27q^2 &lt; 0.)
 
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