In this section, we will learn how to solve equations involving radicals. The basic strategy to solve radical equations is to isolate the radical on one side of the equation and then raise to a power on both sides to cancel the radical.
The formula \(T=2\pi\sqrt{\frac{L}{g}}\) is used to calculate the period of a pendulum and is attributed to the scientist Christiaan Huygens. In the formula, \(T\) stands for the pendulumβs period (how long one back-and-forth oscillation takes) in seconds, \(L\) stands for the pendulumβs length in meters, and \(g\) is approximately 9.8 mβs2 which is the gravitational acceleration constant on Earth.
Squaring both sides of an equation is βdangerous,βas it could create extraneous solutions, which will not make the equation true. For example, if we square both sides of \(1=-1\text{,}\) we have:
\begin{align*}
1\amp=-1\amp\amp\text{false}\\
(1)^2\amp=(-1)^2\amp\amp\text{square both sides}\ldots\\
1\amp=1\amp\amp\text{true}
\end{align*}
By squaring both sides of an equation, we can sometimes turn a false equation into a true one. This is why we must check solutions when we square both sides of an equation.
Thus, the potential solution \(-2\) is actually extraneous and we have no real solutions to the equation \(5+\sqrt{q}=3\text{.}\) The solution set is the empty set, \(\emptyset\text{.}\)
In the previous example, it would be legitimate to observe that there are no solutions at earlier stages. From the very beginning, how could \(5\) plus a positive quantity result in \(3\text{?}\) Or at the second step, since square roots are non-negative, how could a square root equal \(-2\text{?}\)
You do not have to be able to make these observations. If you follow the general steps for solving radical equations and you remember to check the possible solutions you find, then that will be enough.
Letβs look at an example of solving an equation with a cube root. There is very little difference between solving an equation with one cube root and solving an equation with one square root. Instead of squaring both sides, you cube both sides.
Unlike squaring both sides of an equation, raising both sides of an equation to the 3rd power will not create extraneous solutions. Itβs still good practice to check solution, though. This part is left as exercise.
Subsection4.6.2Solving a Radical Equation with More Than One Variable
We also need to be able to solve radical equations with other variables, like in the next example. The strategy is the same: isolate the radical, and then raise both sides to a certain power to cancel the radical.
Solve for \(L\) in the formula \(T=2\pi\sqrt{\frac{L}{g}}\text{.}\) (This is the formula for a the period \(T\) of a swinging pendulum whose length is \(L\text{,}\) on earth where the acceleration from earthβs gravity is \(g\text{.}\))
The study of black holes has resulted in some interesting mathematics. One fundamental concept about black holes is that there is a distance close enough to the black hole that not even light can escape, called the Schwarzschild radius or the event horizon radius. To find the Schwarzschild radius, \(R_s\text{,}\) we set the formula for the escape velocity equal to the speed of light, \(c\text{,}\) and we get \(c=\sqrt{\frac{2GM}{R_s}}\) which we need to solve for \(R_s\text{.}\) Note that \(G\) is a constant, and \(M\) is the mass of the black hole.
We will start by taking the equation \(c=\sqrt{\frac{2GM}{R_s}}\) and applying our standard radical-equation-solving techniques. Isolate the radical and square both sides:
What is it called when you have an equation to solve, and you use some algebra steps that lead you to having a small list of possible solutions, but one or more of them are not actually solutions?
In an electric circuit, resonance occurs when the frequency \(f\text{,}\) inductance \(L\text{,}\) and capacitance \(C\) fulfill the following equation:
A pendulum has length \(L\text{,}\) measured in feet. The amount of time that it takes to swing back and forth one full cycle is called the βperiodβ and is denoted \(T\text{.}\) The following formula from physics relates \(T\) to \(L\text{.}\)
\begin{equation*}
T = 2 \pi \sqrt{\frac{L}{32}}
\end{equation*}