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$$f ( t ) = \frac { t ^ { 2 } - 3 t + 2 } { t ^ { 2 } - 4 }$$

Short Answer

Expert verified
The simplified function is \( f(t) = \frac { t-1 } { t+2 } \) and the function is undefined at \( t = -2 \).

Step by step solution

01

- Factor the polynomials

In the numerator, the function \( t^{2} - 3t +2 \) can be factored into \( (t-1)(t-2) \). The denominator \( t^{2} - 4 \) can be factored into \( (t-2)(t+2) \), using the difference of squares.
02

- Simplify the function

Now that we have factored the polynomials, the function \( f(t) = \frac { (t-1)(t-2) } { (t-2)(t+2) } \). As you can see, \( t-2 \) terms in the numerator and denominator can be cancelled out, simplifying the function to \( f(t) = \frac { t-1 } { t+2 } \) .
03

- Identify the undefined values

For a function to be undefined, the denominator of the function has to be equal to zero. So, we find the values of \( t \) that make \( t+2 =0 \), which gives \( t = -2 \) . This value is excluded from the domain of the function as it makes the denominator of the function (and hence the function itself) undefined.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Polynomial Factorization
Polynomial factorization involves breaking down a polynomial into simpler factors that, when multiplied together, give back the original polynomial. This is similar to how we can factor numbers, like 12 into 2 and 6. For polynomials, the process often involves finding numbers (or expressions) that can be multiplied to reach the respective terms in the polynomial.

In our exercise, we dealt with the polynomial in the numerator:
  • \( t^{2} - 3t + 2 \), which can be factored as \((t-1)(t-2)\).
This is achieved by finding two numbers that multiply to the constant term (2 in this case), and add up to the coefficient of the linear term (-3 here).

Similarly, the polynomial in the denominator,
  • \( t^2 - 4 \), is factored as \((t-2)(t+2)\).
This uses the difference of squares formula which is particularly useful for any expression in the form of \(a^2 - b^2\) resulting in \((a-b)(a+b)\). Learning to recognize these patterns will make factorization quicker and easier.
Simplifying Rational Expressions
Simplification of rational expressions is the process of making these expressions as simple as possible. Rational expressions, like the one in our exercise, are fractions where the numerator and the denominator are polynomials.

After factoring both the numerator and the denominator, you can cancel out any common factors. In our exercise, both the numerator and the denominator had \(t-2\) as a factor:
  • Original form: \( \frac{(t-1)(t-2)}{(t-2)(t+2)} \).
Since \(t-2\) appears in both parts of the fraction, it can be canceled out, simplifying the expression to:
  • \(\frac{t-1}{t+2}\).
Simplifying helps in evaluating the functions more easily and also reveals more about their behaviors and properties. Remember to not cancel factors directly without ensuring they are indeed factors of both parts of the fraction.
Domain of a Function
The domain of a function consists of all the possible values of the variable that make the function work without any issues. In rational functions, we particularly focus on the values that make the denominator zero, as these are the points where the function becomes undefined.

In our example, the denominator \(t+2\) becomes zero when \(t = -2\), making our function undefined at this value. Thus, \(t = -2\) is not included in the domain of the function.

The domain of \(f(t)\), then, is all real numbers except \(t = -2\). Checking the domain is crucial since it indicates where the function can be smoothly evaluated without running into mathematical problems. Always look for values that might make any part of the expression undefined and exclude those from the domain.

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Most popular questions from this chapter

Figure 7.29 shows a beam of length 2\(\lambda\) that is imbed- ded in a support on the left side and free on the right. The vertical deflection of the beam a distance \(x\) from the support is denoted by \(y(x) .\) If the beam has a concen- trated load L acting on it in the center of the beam, then the deflection must satisfy the symbolic boundary value problem $$E I y^{(4)}(x)=L \delta(x-\lambda)$$ $$y(0)=y^{\prime}(0)=y^{\prime \prime}(2 \lambda)=y^{\prime \prime \prime}(2 \lambda)=0$$ where \(E,\) the modulus of elasticity, and \(I,\) the moment of inertia, are constants. Find a formula for the dis- placement \(y(x)\) in terms of the constants \(\lambda, L, E,\) and I. [Hint: Let \(y^{\prime \prime}(0)=A\) and \(y^{\prime \prime \prime}(0)=B .\) First solve the fourth-order symbolic initial value problem and then use the conditions \(y^{\prime \prime}(2 \lambda)=y^{\prime \prime \prime}(2 \lambda)=0\) to determine \(A\) and \(B . ]\)

$$f ( t ) = \frac { t ^ { 2 } - t - 20 } { t ^ { 2 } + 7 t + 10 }$$

\(\begin{array}{ll}{x^{\prime}-2 x+y^{\prime}=-(\cos t+4 \sin t) ;} & {x(\pi)=0} \\ {2 x+y^{\prime}+y=\sin t+3 \cos t ;} & {y(\pi)=3}\end{array}\)

$$\begin{array}{l}{y^{\prime \prime}+y=-\delta(t-\pi)+\delta(t-2 \pi)} \\\ {y(0)=0, \quad y^{\prime}(0)=1}\end{array}$$

Thanks to Euler's formula (page 166) and the algebraic properties of complex numbers, several of the entries of Table 7.1 can be derived from a single formula; namely, (6) $$\quad \mathscr{L}\left\\{e^{(a+i b) t}\right\\}(s)=\frac{s-a+i b}{(s-a)^{2}+b^{2}}, \quad s>a$$ (a) By computing the integral in the definition of theLaplace transform on page 353 with \(f(t)=e^{(a+i b) t}\)show that $$\mathscr{L}\left\\{e^{(a+i b) t}\right\\}(s)=\frac{1}{s-(a+i b)}, \quad s>a$$ (b) Deduce (6) from part (a) by showing that$$\frac{1}{s-(a+i b)}=\frac{s-a+i b}{(s-a)^{2}+b^{2}}$$ (c) By equating the real and imaginary parts in formula (6), deduce the last two entries in Table 7.1.

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