Simplify Complex Roots Of Unity Expression

by Alex Johnson 43 views

When delving into the fascinating world of complex numbers, you'll inevitably encounter the concept of roots of unity. These are numbers that, when raised to a specific power, equal 1. Among these, the cubic roots of unity hold a special place, representing the solutions to the equation z3=1z^3 = 1. While 1 is one cubic root of unity, the other two are non-real and have a peculiar, yet incredibly useful, relationship. These are often denoted by ω\omega and ω2\omega^2. Understanding their properties is key to simplifying expressions involving them, like the one we're about to tackle.

Let's dive into the mathematical puzzle presented: If ω,ω2\omega, \omega^2 are the non-real cubic roots of unity, what is the value of a+bω+cω2c+aω+bω2+a+bω+cω2b+cω+aω2\frac{a+b \omega+c \omega^2}{c+a \omega+b \omega^2}+\frac{a+b \omega+c \omega^2}{b+c \omega+a \omega^2}? This problem requires us to leverage the fundamental properties of these complex roots. The first and most crucial property is that the sum of all cubic roots of unity is zero: 1+ω+ω2=01 + \omega + \omega^2 = 0. This implies that ω+ω2=−1\omega + \omega^2 = -1. Another vital property is that ω3=1\omega^3 = 1. Furthermore, ω2=1ω\omega^2 = \frac{1}{\omega} and (ω2)2=ω4=ω(\omega^2)^2 = \omega^4 = \omega. These relationships are the building blocks for simplifying any expression involving ω\omega and ω2\omega^2. Without a firm grasp of these properties, attempting to solve such problems can feel like navigating a maze blindfolded. However, with these tools at our disposal, the path to the solution becomes clear and, dare I say, quite elegant.

Unpacking the Properties of Cubic Roots of Unity

Before we fully engage with the given expression, let's reinforce our understanding of the non-real cubic roots of unity. Recall that the cubic roots of unity are the solutions to z3−1=0z^3 - 1 = 0. Factoring this equation, we get (z−1)(z2+z+1)=0(z-1)(z^2+z+1) = 0. One root is clearly z=1z=1. The other two roots come from the quadratic equation z2+z+1=0z^2+z+1 = 0. Using the quadratic formula, z=−1±12−4(1)(1)2(1)=−1±−32=−1±i32z = \frac{-1 \pm \sqrt{1^2 - 4(1)(1)}}{2(1)} = \frac{-1 \pm \sqrt{-3}}{2} = \frac{-1 \pm i\sqrt{3}}{2}. These are our ω\omega and ω2\omega^2. Let's assign ω=−1+i32\omega = \frac{-1 + i\sqrt{3}}{2} and ω2=−1−i32\omega^2 = \frac{-1 - i\sqrt{3}}{2}. If we square ω\omega, we get (−1+i32)2=1−2i3+(i3)24=1−2i3−34=−2−2i34=−1−i32(\frac{-1 + i\sqrt{3}}{2})^2 = \frac{1 - 2i\sqrt{3} + (i\sqrt{3})^2}{4} = \frac{1 - 2i\sqrt{3} - 3}{4} = \frac{-2 - 2i\sqrt{3}}{4} = \frac{-1 - i\sqrt{3}}{2}, which is indeed ω2\omega^2. Conversely, squaring ω2\omega^2 gives us ω4=ω\omega^4 = \omega. This reciprocal relationship is fundamental. More importantly, as we noted earlier, 1+ω+ω2=01 + \omega + \omega^2 = 0. This identity is incredibly powerful because it allows us to substitute −1-1 for ω+ω2\omega + \omega^2, or to express one root in terms of the others, for example, ω2=−1−ω\omega^2 = -1 - \omega. These relationships are not just abstract mathematical curiosities; they are the keys that unlock the simplification of complex algebraic expressions involving these roots.

Simplifying the First Term

Let's focus on the first term of the expression: a+bω+cω2c+aω+bω2\frac{a+b \omega+c \omega^2}{c+a \omega+b \omega^2}. Our goal is to simplify this fraction. We can try to manipulate the denominator to resemble the numerator or vice versa, using the properties we've discussed. Let's consider the denominator, c+aω+bω2c+a \omega+b \omega^2. Can we relate this to the numerator a+bω+cω2a+b \omega+c \omega^2? A common strategy when dealing with ω\omega and ω2\omega^2 is to multiply by powers of ω\omega. Let's try multiplying the denominator by ω\omega: ω(c+aω+bω2)=cω+aω2+bω3\omega(c+a \omega+b \omega^2) = c\omega + a\omega^2 + b\omega^3. Since ω3=1\omega^3 = 1, this becomes cω+aω2+bc\omega + a\omega^2 + b. This doesn't immediately look like the numerator. Let's try multiplying by ω2\omega^2: ω2(c+aω+bω2)=cω2+aω3+bω4\omega^2(c+a \omega+b \omega^2) = c\omega^2 + a\omega^3 + b\omega^4. Using ω3=1\omega^3 = 1 and ω4=ω\omega^4 = \omega, this simplifies to cω2+a+bωc\omega^2 + a + b\omega. Rearranging the terms, we get a+bω+cω2a + b\omega + c\omega^2. Eureka! The denominator, when multiplied by ω2\omega^2, becomes exactly the numerator. This means that c+aω+bω2=a+bω+cω2ω2c+a \omega+b \omega^2 = \frac{a+b \omega+c \omega^2}{\omega^2}. Therefore, the first term simplifies to a+bω+cω2a+bω+cω2ω2=ω2\frac{a+b \omega+c \omega^2}{\frac{a+b \omega+c \omega^2}{\omega^2}} = \omega^2. This is a significant simplification and shows the power of working with these roots. It's crucial to ensure that the denominator is not zero. If a+bω+cω2=0a+b \omega+c \omega^2 = 0, then a=b=c=0a = b=c=0 for the equality to hold for all cases. Assuming a,b,ca, b, c are not all zero, this simplification is valid.

Simplifying the Second Term

Now, let's turn our attention to the second term: a+bω+cω2b+cω+aω2\frac{a+b \omega+c \omega^2}{b+c \omega+a \omega^2}. We'll employ a similar strategy. Let the numerator be N=a+bω+cω2N = a+b \omega+c \omega^2. Consider the denominator D2=b+cω+aω2D_2 = b+c \omega+a \omega^2. Let's see what happens when we multiply D2D_2 by ω\omega: ω(b+cω+aω2)=bω+cω2+aω3\omega(b+c \omega+a \omega^2) = b\omega + c\omega^2 + a\omega^3. Using ω3=1\omega^3 = 1, this becomes bω+cω2+ab\omega + c\omega^2 + a. Rearranging, we get a+bω+cω2a + b\omega + c\omega^2, which is our numerator NN. So, b+cω+aω2=a+bω+cω2ωb+c \omega+a \omega^2 = \frac{a+b \omega+c \omega^2}{\omega}. This implies that the second term simplifies to a+bω+cω2a+bω+cω2ω=ω\frac{a+b \omega+c \omega^2}{\frac{a+b \omega+c \omega^2}{\omega}} = \omega. Again, this simplification is valid as long as the numerator is not zero. The elegance here is striking; we've managed to reduce both complex fractions to simple powers of ω\omega. This highlights the symmetric and cyclic nature of the roots of unity. The structure of the denominators is directly related to cyclic permutations of the coefficients in the numerator, a pattern that ω\omega and ω2\omega^2 are perfectly designed to simplify.

The Grand Finale: Summing the Simplified Terms

We have successfully simplified the two terms of the original expression. The first term, a+bω+cω2c+aω+bω2\frac{a+b \omega+c \omega^2}{c+a \omega+b \omega^2}, reduced to ω2\omega^2. The second term, a+bω+cω2b+cω+aω2\frac{a+b \omega+c \omega^2}{b+c \omega+a \omega^2}, reduced to ω\omega. Now, we just need to add these results together: ω2+ω\omega^2 + \omega. Recall the fundamental property of cubic roots of unity: 1+ω+ω2=01 + \omega + \omega^2 = 0. From this identity, we can directly deduce that ω+ω2=−1\omega + \omega^2 = -1. Therefore, the sum of the two simplified terms is -1. This result is independent of the values of aa, bb, and cc, provided that the denominators in the original expression are not zero. The problem elegantly resolves to a fundamental identity of the cubic roots of unity. This demonstrates how seemingly complex algebraic expressions can be unraveled using the inherent properties of mathematical constants and relationships. The beauty lies in the reduction to a simple, universally true statement about these roots.

Let's double-check our steps to ensure accuracy. We used the properties ω3=1\omega^3 = 1 and 1+ω+ω2=01 + \omega + \omega^2 = 0. For the first term, we showed that ω2(c+aω+bω2)=a+bω+cω2\omega^2 (c+a \omega+b \omega^2) = a+b \omega+c \omega^2. Thus, a+bω+cω2c+aω+bω2=ω2\frac{a+b \omega+c \omega^2}{c+a \omega+b \omega^2} = \omega^2. For the second term, we showed that ω(b+cω+aω2)=a+bω+cω2\omega (b+c \omega+a \omega^2) = a+b \omega+c \omega^2. Thus, a+bω+cω2b+cω+aω2=ω\frac{a+b \omega+c \omega^2}{b+c \omega+a \omega^2} = \omega. Summing them gives ω2+ω=−1\omega^2 + \omega = -1. The solution seems robust. This type of problem is common in algebra and complex numbers, testing a student's grasp of fundamental properties and their application in simplification. The structure of the expression is specifically designed to exploit these properties, leading to a surprisingly simple answer.

Conclusion

In conclusion, by carefully applying the fundamental properties of the non-real cubic roots of unity, namely ω3=1\omega^3 = 1 and 1+ω+ω2=01 + \omega + \omega^2 = 0, we were able to simplify the given expression. The first term a+bω+cω2c+aω+bω2\frac{a+b \omega+c \omega^2}{c+a \omega+b \omega^2} simplifies to ω2\omega^2, and the second term a+bω+cω2b+cω+aω2\frac{a+b \omega+c \omega^2}{b+c \omega+a \omega^2} simplifies to ω\omega. Adding these results, we get ω2+ω\omega^2 + \omega, which, from the identity 1+ω+ω2=01 + \omega + \omega^2 = 0, equals -1. Therefore, the value of the entire expression is -1. This problem serves as a beautiful illustration of how abstract mathematical properties can lead to elegant and straightforward solutions for seemingly intricate algebraic challenges. It underscores the importance of mastering the foundational concepts in mathematics.

For further exploration into the fascinating properties of complex numbers and roots of unity, you might find the resources at Brilliant.org to be incredibly helpful and engaging.