Table of Contents

    Introduction


    In the realm of mathematical analysis, especially within Laplace Transformation, the concept of Exponential Order is fundamental. This property guarantees that functions do not grow too rapidly, ensuring the convergence of integrals and the existence of Laplace transforms. By meeting the exponential order condition, a function \( f(t) \) is considered well-behaved as \( t \) approaches infinity.

    Exponential Order


    A function \( f \) is called an exponential order function if there is a constant \( a \) and positive constants \( t_0 \) and \( M \) such that:

    \[ |f(t)| \leq M e^{at} \] for all \( t \gt t_0 \) where \( f(t) \) is defined.

    In simple terms, if a function \( f \) follows this rule for some constant \( a \), we say that \( f \) is of exponential order.

    This inequality sets an upper bound on the function’s growth, thereby enabling effective analysis in various mathematical and engineering applications.

    Definition and Explanation


    The criterion for a function to be of exponential order is both simple and powerful. Essentially, it means that the absolute value of \( f(t) \) is controlled by an exponential function for sufficiently large \( t \). In other words, no matter how complex \( f(t) \) may appear, its long-term behavior is confined within the limits dictated by the exponential function \( M e^{at} \). This controlled growth is vital when solving differential equations and analyzing system stability.

    Examples-1


    \( f(t)=c \) is of exponential order where \( c \) is a constant.

    Since \( f(t)=c \), we first take the absolute value: \[ |f(t)| = |c|. \]

    We want to show that there exist constants \( M > 0 \), \( t_0 \ge 0 \), and a constant \( b \) such that \[ |f(t)| \le M e^{bt} \quad \text{for all } t > t_0. \]

    Choose \( M = |c| + 1 \) (any value greater than \( |c| \)), \( b = 0 \), and any \( t_0 > 0 \). Then, for all \( t > t_0 \): \[ \begin{align} |f(t)| &= |c| \nonumber\\ &\leq |c| + 1 \nonumber\\ &\leq (|c| + 1)e^{0\cdot t} \nonumber\\ &= Me^{0\cdot t}\nonumber \end{align} \]

    Since the condition holds for some constants \( M > 0 \), \( t_0 > 0 \), and \( b = 0 \), we conclude that \( f(t) = c \) is of exponential order.

    Examples-2


    \( f(t)=e^{at} \) is of exponential order where \(a\) is a constant.

    Since \( f(t)=e^{at} \), we first take the absolute value: \[ |f(t)| = |e^{at}| = e^{at}. \]

    We want to show that there exist constants \( M > 0 \), \( t_0 \ge 0 \), and a constant \( b \) such that \[ |f(t)| \le M e^{bt} \quad \text{for all } t > t_0. \]

    Case 1: \( a \ge 0 \)
    Choose \( M = 1 \), \( b = a \), and \( t_0 = 0 \). Then, for all \( t \ge 0 \): \[ |f(t)| = e^{at} = 1\cdot e^{at} = M e^{bt}. \]

    Case 2: \( a \lt 0 \)
    In this case, \( e^{at} \) is a decreasing function and satisfies \( e^{at} \le 1 \) for \( t \ge 0 \). Choose \( M = 1 \), \( b = 0 \), and \( t_0 = 0 \). Then, for all \( t \ge 0 \): \[ |f(t)| = e^{at} \le 1 = 1\cdot e^{0\cdot t} = M e^{bt}. \]

    Since in both cases the condition \[ |f(t)| \le M e^{bt} \quad \text{for all } t > t_0 \] is satisfied, we conclude that \( f(t)=e^{at} \) is of exponential order.

    Examples-3


    \( f(t)=t^n \) is of exponential order where \( n > 0 \).

    Since \( f(t)=t^n \), we take the absolute value: \[ |f(t)| = t^n \quad \text{for } t \ge 0. \]

    We want to show that there exist constants \( M > 0 \), \( t_0 \ge 0 \), and \( a > 0 \) such that \[ t^n \le M e^{at} \quad \text{for all } t > t_0. \]

    Let \( a > 0 \) be any positive constant. Note that \[ \lim_{t \to \infty} \frac{t^n}{e^{at}} = 0, \] which implies that for sufficiently large \( t \), the exponential \( e^{at} \) dominates the polynomial \( t^n \). In other words, there exists some \( t_0 > 0 \) such that for all \( t > t_0 \), \[ t^n \lt e^{at}. \]

    Now, choose \( M \) to be any constant satisfying \[ M \ge \max \left\{ \sup_{0 \le t \le t_0} \frac{t^n}{e^{at}},\, 1 \right\}. \] Then for all \( t > t_0 \): \[ t^n \le e^{at} \le M e^{at}. \]

    Since the condition \[ |f(t)| \le M e^{at} \] holds for some constants \( M > 0 \), \( t_0 > 0 \), and \( a > 0 \), we conclude that \( f(t)=t^n \) is of exponential order.

    Examples-4


    \( f(t)=\sin at \) is of exponential order where \( a \) is a constant.

    Since \( f(t)=\sin at \), we first take the absolute value: \[ |f(t)| = |\sin at|. \]

    We know that for all \( t \), the sine function is bounded: \[ |\sin at| \leq 1. \]

    Choose \( M = 1 \), \( b = 0 \), and \( t_0 = 0 \). Then, for all \( t \ge 0 \): \[ |f(t)| \leq 1 = Me^{0 \cdot t}. \]

    Since the condition holds for some constants \( M > 0 \), \( t_0 \ge 0 \), and \( b = 0 \), we conclude that \( f(t)=\sin at \) is of exponential order.

    Examples-5


    \( f(t)=\cos at \) is of exponential order where \( a \) is a constant.

    Since \( f(t)=\cos at \), we first consider the absolute value: \[ |f(t)| = |\cos at| \leq 1 \quad \text{for all } t. \]

    We want to show that there exist constants \( M > 0 \), \( t_0 \ge 0 \), and a constant \( b \) such that \[ |f(t)| \le M e^{bt} \quad \text{for all } t > t_0. \]

    Choose \( M = 1 \) (any value \( \geq 1 \) will work), \( b = 0 \), and any \( t_0 \ge 0 \). Then, for all \( t \ge t_0 \): \[ |f(t)| \leq 1 = 1\cdot e^{0\cdot t} = M e^{0\cdot t}. \]

    Since the condition holds for some constants \( M > 0 \), \( t_0 \ge 0 \), and \( b = 0 \), we conclude that \( f(t)=\cos at \) is of exponential order.

    Examples-6


    \( f(t)=t^{n}e^{at} \) is of exponential order, where \( n > 0 \) and \( a \) is a constant.

    Since \( f(t)=t^{n}e^{at} \), we first take the absolute value: \[ |f(t)| = |t^{n}e^{at}| = t^{n}\,|e^{at}|. \]

    We want to show that there exist constants \( M > 0 \), \( t_0 \ge 0 \), and a constant \( \alpha \) such that \[ t^{n}e^{at} \le M e^{\alpha t} \quad \text{for all } t > t_0. \]

    Case 1: \( a \ge 0 \)
    Choose any \( \delta > 0 \) and set \( \alpha = a + \delta \). Then, for large \( t \), the exponential \( e^{\delta t} \) eventually dominates the polynomial \( t^{n} \) because \[ \lim_{t \to \infty} \frac{t^n}{e^{\delta t}} = 0. \] Thus, there exists some \( t_0 > 0 \) such that for all \( t > t_0 \): \[ t^{n} \lt e^{\delta t}. \] Multiplying both sides by \( e^{at} \) gives \[ t^{n}e^{at} \lt e^{at}e^{\delta t} = e^{(a+\delta)t} = e^{\alpha t}. \] Now, choose \( M \) to be any constant satisfying \[ M \ge \max\left\{ \sup_{0 \le t \le t_0} \frac{t^{n}e^{at}}{e^{\alpha t}},\, 1 \right\}. \] Then, for all \( t > t_0 \): \[ t^{n}e^{at} \le e^{\alpha t} \le M e^{\alpha t}. \]

    Case 2: \( a \lt 0 \)
    Here, \( e^{at} \) decays as \( t \) increases, and the product \( t^{n}e^{at} \) attains a maximum at some finite \( t \). Define \[ M = \max_{t \ge 0} \{ t^{n}e^{at} \}, \] and choose \( \alpha = 0 \) and \( t_0 = 0 \). Then for all \( t \ge 0 \): \[ t^{n}e^{at} \le M = M e^{0\cdot t}. \]

    In both cases, we have found constants \( M > 0 \), \( t_0 \ge 0 \), and a constant (either \( \alpha > 0 \) or \( \alpha = 0 \)) such that \[ |f(t)| = t^{n}e^{at} \le M e^{\alpha t} \quad \text{for all } t > t_0. \] Therefore, we conclude that \( f(t)=t^{n}e^{at} \) is of exponential order.

    Examples-7


    \( f(t)=t^{n}\sin(at) \) where \( n > 0 \) and \( a \) is a constant is of exponential order.

    Since \( f(t)=t^{n}\sin(at) \), we first take the absolute value: \[ |f(t)| = |t^{n}\sin(at)| \le t^{n}, \] because \( |\sin(at)| \le 1 \) for all \( t \).

    We want to show that there exist constants \( M > 0 \), \( t_0 \ge 0 \), and a constant \( b \) such that \[ |f(t)| \le M e^{bt} \quad \text{for all } t > t_0. \]

    Notice that \( t^n \) is a polynomial and grows slower than any exponential function \( e^{bt} \) when \( b > 0 \). In fact, for any fixed \( b > 0 \), \[ \lim_{t \to \infty}\frac{t^n}{e^{bt}} = 0. \] This implies that there exists some \( t_0 \ge 0 \) such that for all \( t > t_0 \), \[ t^n \le e^{bt}. \]

    Thus, if we choose \( M \ge 1 \) (for example, \( M = 1 \)) and any \( b > 0 \) along with the corresponding \( t_0 \), then for all \( t > t_0 \) we have: \[ |f(t)| \le t^n \le M e^{bt}. \]

    Since the condition holds for some constants \( M > 0 \), \( t_0 \ge 0 \), and \( b > 0 \), we conclude that \( f(t)=t^{n}\sin(at) \) is of exponential order.

    Examples-8


    \( f(t)=t^{n}\cos at \) where \(n \gt 0\) and \(a\) is a constant.

    Since \( f(t)=t^{n}\cos(at) \), we first take the absolute value: \[ |f(t)| = |t^{n}\cos(at)| \le t^{n}, \] because \( |\cos(at)| \le 1 \) for all \( t \).

    We want to show that there exist constants \( M > 0 \), \( t_0 \ge 0 \), and a constant \( b \) such that \[ |f(t)| \le M e^{bt} \quad \text{for all } t \gt t_0. \]

    Notice that \( t^n \) is a polynomial and grows slower than any exponential function \( e^{bt} \) when \( b > 0 \). In fact, for any fixed \( b > 0 \), \[ \lim_{t \to \infty}\frac{t^n}{e^{bt}} = 0. \] This implies that there exists some \( t_0 \ge 0 \) such that for all \( t > t_0 \), \[ t^n \le e^{bt}. \]

    Thus, if we choose \( M \ge 1 \) (for example, \( M = 1 \)) and any \( b > 0 \) along with the corresponding \( t_0 \), then for all \( t > t_0 \) we have: \[ |f(t)| \le t^n \le M e^{bt}. \]

    Since the condition holds for some constants \( M > 0 \), \( t_0 \ge 0 \), and \( b > 0 \), we conclude that \( f(t)=t^{n}\cos(at) \) is of exponential order.

    Examples-9


    \( f(t)=e^{bt}\sin at \) is of exponential order, where \(a\) and \(b\) are constants.

    Since \( f(t)=e^{bt}\sin at \), we first take the absolute value: \[ |f(t)| = |e^{bt}\sin at| \le e^{bt} \, |\sin at| \le e^{bt}, \] because \( |\sin at| \le 1 \) for all \( t \).

    We want to show that there exist constants \( M > 0 \), \( t_0 \ge 0 \), and a constant \( \alpha \) such that \[ |f(t)| \le M e^{\alpha t} \quad \text{for all } t > t_0. \]

    Case 1: \( b \ge 0 \)
    Choose \( M = 1 \), \( \alpha = b \), and \( t_0 = 0 \). Then for all \( t \ge 0 \): \[ |f(t)| \le e^{bt} = 1\cdot e^{bt} = M e^{\alpha t}. \]

    Case 2: \( b \lt 0 \)
    In this case, since \( e^{bt} \) is a decreasing function and satisfies \( e^{bt} \le 1 \) for \( t \ge 0 \), choose \( M = 1 \), \( \alpha = 0 \), and \( t_0 = 0 \). Then for all \( t \ge 0 \): \[ |f(t)| \le e^{bt} \le 1 = 1\cdot e^{0\cdot t} = M e^{\alpha t}. \]

    Since in both cases the condition \[ |f(t)| \le M e^{\alpha t} \quad \text{for all } t > t_0 \] is satisfied, we conclude that \( f(t)=e^{bt}\sin at \) is of exponential order.

    Examples-10


    \( f(t)=e^{bt}\cos at \) is of exponential order, where \(a\) and \(b\) are constants.

    Since \( f(t)=e^{bt}\cos at \), we first take the absolute value: \[ |f(t)| = |e^{bt}\cos at| \le e^{bt} \, |\cos at| \le e^{bt}, \] because \( |\cos at| \le 1 \) for all \( t \).

    We want to show that there exist constants \( M > 0 \), \( t_0 \ge 0 \), and a constant \( \alpha \) such that \[ |f(t)| \le M e^{\alpha t} \quad \text{for all } t > t_0. \]

    Case 1: \( b \ge 0 \)
    Choose \( M = 1 \), \( \alpha = b \), and \( t_0 = 0 \). Then for all \( t \ge 0 \): \[ |f(t)| \le e^{bt} = 1\cdot e^{bt} = M e^{\alpha t}. \]

    Case 2: \( b \lt 0 \)
    In this case, since \( e^{bt} \) is a decreasing function and satisfies \( e^{bt} \le 1 \) for \( t \ge 0 \), choose \( M = 1 \), \( \alpha = 0 \), and \( t_0 = 0 \). Then for all \( t \ge 0 \): \[ |f(t)| \le e^{bt} \le 1 = 1\cdot e^{0\cdot t} = M e^{\alpha t}. \]

    Since in both cases the condition \[ |f(t)| \le M e^{\alpha t} \quad \text{for all } t > t_0 \] is satisfied, we conclude that \( f(t)=e^{bt}\cos at \) is of exponential order.

    Examples-11


    \( f(t)=\sinh at \) is of exponential order, where \( a \) is a constant.

    Since \( f(t)=\sinh at \), recall that \[ \sinh at = \frac{e^{at} – e^{-at}}{2}. \] Taking the absolute value gives \[ |f(t)| = |\sinh at| \le \frac{e^{at} + e^{-at}}{2}. \]

    Notice that for any real \( a \) and for all \( t \ge 0 \), \[ e^{at} \le e^{|a|t} \quad \text{and} \quad e^{-at} \le e^{|a|t}. \] Therefore, \[ |f(t)| \le \frac{e^{|a|t} + e^{|a|t}}{2} = e^{|a|t}. \]

    Choose \( M = 1 \), \( \alpha = |a| \), and \( t_0 = 0 \). Then, for all \( t \ge 0 \), \[ |f(t)| \le e^{|a|t} = M e^{\alpha t}. \]

    Since we have found constants \( M > 0 \), \( t_0 \ge 0 \), and \( \alpha > 0 \) such that \[ |f(t)| \le M e^{\alpha t}, \] we conclude that \( f(t)=\sinh at \) is of exponential order.

    Examples-12


    \( f(t)=\cosh at \) is of exponential order, where \( a \) is a constant.

    Since \( f(t)=\cosh at \), recall that \[ \cosh at = \frac{e^{at}+e^{-at}}{2}. \]

    Taking the absolute value (noting that \(\cosh at \ge 0\) for all \(t\)), we have: \[ |f(t)| = \cosh at = \frac{e^{at}+e^{-at}}{2}. \]

    For any real \(a\) and all \(t \ge 0\), observe that \[ e^{at} \le e^{|a|t} \quad \text{and} \quad e^{-at} \le e^{|a|t}. \] Hence, \[ |f(t)| \le \frac{e^{|a|t}+e^{|a|t}}{2} = e^{|a|t}. \]

    Choose \( M = 1 \), \( \alpha = |a| \), and \( t_0 = 0 \). Then, for all \( t \ge 0 \): \[ |f(t)| \le e^{|a|t} = M e^{\alpha t}. \]

    Since the condition \[ |f(t)| \le M e^{\alpha t} \] holds for some constants \( M > 0 \), \( t_0 \ge 0 \), and \( \alpha > 0 \), we conclude that \( f(t)=\cosh at \) is of exponential order.

    Conclusion


    In summary, mastering the concept of exponential order is essential for anyone working with Laplace Transformation. Every function discussed in the examples conforms to the exponential order condition by exhibiting a controlled rate of growth. This fundamental property not only ensures the convergence of Laplace integrals but also facilitates the analysis and solution of differential equations.

    As you explore the detailed solutions linked above, you will develop a stronger grasp of this critical mathematical concept. Embrace these examples as stepping stones toward a deeper understanding of mathematical preliminaries in Laplace Transformation. Happy learning and continued exploration in mathematics!

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      A group is a set equipped with a binary operation that satisfies four fundamental properties: closure, associativity, the existence of an identity element, and the existence of inverses for every element.

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      The four main properties are:

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      The identity element is a unique element in the group that, when combined with any other element using the group operation, leaves that element unchanged. It is commonly denoted by e or 1.

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      A normal subgroup is a subgroup that is invariant under conjugation by any element of the original group. This means for every element n in the normal subgroup N and every element g in the group, gng⁻¹ is still in N. Normal subgroups allow the construction of quotient groups, where the group is partitioned into cosets of the normal subgroup.

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      Lagrange's theorem states that for any finite group, the order (number of elements) of every subgroup divides the order of the entire group. This theorem is a fundamental result in the study of finite groups.

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