MHB Can you solve these quadruple equations with real numbers?

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The discussion presents a problem involving quadruple equations that need to be solved for real numbers, specifically focusing on the equations involving variables a, b, c, and d. It also notes that this problem has been previously used in a past Problem of the Week, prompting an apology from the poster. Following this, a new physics problem is introduced regarding a rotating rod with beads that slide outward, requiring calculations of angular speeds at different stages. Despite the introduction of the new problem, no responses were received for the original quadruple equations. The thread emphasizes the importance of following guidelines for participation in the forum.
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Hello, MHB Community! (Wave)

anemone has asked for me to fill in for her while she's away on holiday. :)

Here is this week's POTW:


Find all quadruples $(a,b,c,d)$ of real numbers that simultaneously satisfy the following equations:$$\left\{\begin{array}{rcl}a^3+c^3 & = & 2 \\ a^2b+c^2d & = & 0 \\ b^3+d^3 & = & 1 \\ ab^2+cd^2 & = & -6 \end{array}\right.$$
Remember to read the http://www.mathhelpboards.com/showthread.php?772-Problem-of-the-Week-%28POTW%29-Procedure-and-Guidelines to find out how to http://www.mathhelpboards.com/forms.php?do=form&fid=2!
 
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Hello, MHB Community! (Wave)

It has been brought to my attention that the problem posted this week has been used in the past, found here:

https://mathhelpboards.com/potw-secondary-school-high-school-students-35/problem-week-277-aug-28th-2017-a-22196.html

I apologize for that...here is the solution with which I was provided:

Consider the polynomial $P(x)=(ax+b)^3+(cx+d)^3=\left(a^3+b^3\right)x^3+3\left(a^2b+c^2d\right)x^2+3\left(ab^2+cd^2\right)x+b^3+d^3$. By the conditions of the problem, $P(x)=2x^3-18x+1$. Clearly $P(0)>0,\,P(1)<0$ and $P(3)>0$. Thus $P$ has three distinct zeroes. But $P(x)=0$ implies $ax+b=-(cx+d)$ or $(a+c)x+b+d=0$. This equation has only one solution, unless $a=-c$ and $b=-d$. But since the conditions of the problem do not allow this, we infer that the system of equations in the problem has no solution.
So, I am going to post another problem, from my old physics homework.


A uniform rod of mass $M$ and length $d$ rotates in a horizontal plane about a fixed, vertical, frictionless pin through its center. Two small beads, each of mass $m$, are mounted on the rod such that they are able to slide without friction along its length. Initially the beads are held by catches st positions $x$ (where $x<d/2$) on each side of the center, at which time the system rotates with an angular speed $\omega$.

Suddenly the catches are released and the small beads slide outward along the rod. Find:

  • (a) the angular speed of the system at the instant the beads reach the ends of the rod
  • (b) the angular speed of the rod after the beads fly off the ends

Remember to read the http://www.mathhelpboards.com/showthread.php?772-Problem-of-the-Week-%28POTW%29-Procedure-and-Guidelines to find out how to http://www.mathhelpboards.com/forms.php?do=form&fid=2!
 
No one answered this weeks POTW...my solution follows:

(a) Apply conservation of angular momentum (subscripts of $R$ pertain to the rod, while those of $B$ pertain to the beads, and $\omega_i=\omega$):

Recall angular momentum $L$ is the product of the moment of interia $I$ and the angular speed $\omega$.

$$I_R\omega_i+2I_{B_i}\omega_i=I_R\omega_f+2I_{B_f}\omega_f$$

Solve for $\omega_f$:

$$\omega_f=\omega_i\frac{I_R+2I_{B_i}}{I_R+2I_{B_f}}$$

Now the moment of inertia for a point mass (which we can use for the small beads where no radius is given) of mass $m$ and distance from the axis of rotation $r$ is:

$$I=mr^2$$

And the moment of rotation for a rod of mass $m$ and length $L$ is:

$$I=\frac{1}{12}mL^2$$

And so, there results:

$$\omega_f=\omega_i\frac{\frac{1}{12}Md^2+2mx^2}{\frac{1}{12}Md^2+2m\left(\frac{d}{2}\right)^2}=\omega_i\frac{Md^2+24mx^2}{Md^2+6md^2}$$​

(b) We can equate the momentum of the system when the beads are at the ends of the rod to when the beads have flown off the rod as follows:

$$d^2\omega_f\left(\frac{1}{12}M+2m\right)=I_R\omega_R+2mv_B$$

Now, observing that $$v_B=\frac{d}{2}\omega_f$$, and substituting for the moment of inertia for the rod, we have:

$$d^2\omega_f\left(\frac{1}{12}M+2m\right)=\frac{1}{12}Md^2\omega_R+md\omega_f$$

Solve for $\omega_R$:

$$\omega_R=\frac{\omega_f}{Md}\left(d\left(M+24m\right)-12m\right)$$​
 
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