Problem 8
Question
Determine \(f(t-a)\) for the given function \(f\) and the given constant \(a\). $$f(t)=e^{-t} \sin 2 t, \quad a=\pi / 6$$.
Step-by-Step Solution
Verified Answer
The short answer to the question is:
\[f(t-a) = e^{-t} \cdot e^{\pi/6} \sin (2t - \pi/3)\]
1Step 1: Replace t with (t-a)
Replace every occurrence of the variable \(t\) with \((t-a)\) in the given function, where \(a = \pi/6\):
\[f(t-a) = e^{-(t-a)} \sin 2(t-a)\]
Step 2: Simplify the expression
2Step 2: Simplify the exponent in the exponential term
Simplify the exponent of the exponential term in the function:
\[e^{-(t-a)} = e^{-t + a} = e^{-t} \cdot e^a\]
Remembering that \(a = \pi/6\), the expression can be written as:
\[e^{-t} \cdot e^{\pi/6}\]
3Step 3: Simplify the argument in the sin term
Simplify the argument of the sin term in the function:
\[\sin 2(t-a) = \sin 2(t-\pi/6) = \sin (2t - 2\pi/6) = \sin (2t - \pi/3)\]
Step 3: Combine the simplified terms
4Step 4: Combine the simplified exponential and sin terms
Combine the simplified exponential and sin terms to obtain the final expression for \(f(t-a)\):
\[f(t-a) = e^{-t} \cdot e^{\pi/6} \sin (2t - \pi/3)\]
Key Concepts
Time ShiftingExponential FunctionsTrigonometric Functions
Time Shifting
When we talk about "Time Shifting," we are referring to adjusting the input of a function by a constant value.
This concept is commonly used in physics and engineering, especially with regard to signal processing.
This plays an essential role when dealing with Laplace transforms as it helps analyze different time-based changes to functions.
This concept is commonly used in physics and engineering, especially with regard to signal processing.
- The basic idea is to slide or "shift" the function along the time axis.
- In this context, if you have a function like \( f(t) \), a time-shifted version \( f(t-a) \) means the function happens "\( a \)" units later (or earlier if \( a \) is negative).
This plays an essential role when dealing with Laplace transforms as it helps analyze different time-based changes to functions.
Exponential Functions
Exponential functions are fundamentally structured as a constant raised to a variable power, like \( e^{-t} \).
These functions describe processes that increase or decrease rapidly; a classic example includes radioactive decay and population growth.
This transformation maintains the original behavior while accounting for the shift \( a \); when \( a = \pi/6 \), the term \( e^{\pi/6} \) becomes a multiplicative constant that will affect the function's amplitude.
These functions describe processes that increase or decrease rapidly; a classic example includes radioactive decay and population growth.
- The key characteristic of an exponential function is its constant rate of change.
- The base \( e \) (approximately 2.718) is a natural constant commonly used in these functions.
This transformation maintains the original behavior while accounting for the shift \( a \); when \( a = \pi/6 \), the term \( e^{\pi/6} \) becomes a multiplicative constant that will affect the function's amplitude.
Trigonometric Functions
Trigonometric functions like \( \sin \, \) and \( \cos \, \) describe the relations of angles on a unit circle.
They are periodic, meaning their values repeat at regular intervals, which is why they fit well into wave-like behavior in physics.
You first rewrite it as \( \sin(2t - \pi/3) \), achieving a change in the function's phase but not its periodicity.
This modification affects where the cycle starts, effectively altering the position of the wave without changing its shape.
They are periodic, meaning their values repeat at regular intervals, which is why they fit well into wave-like behavior in physics.
- They provide insights into oscillations, signals, and other waveforms.
- The argument of these functions, such as \( 2(t-a) \) in the expression \( \sin 2(t-a) \), represents a shifted angle in the trigonometric function.
You first rewrite it as \( \sin(2t - \pi/3) \), achieving a change in the function's phase but not its periodicity.
This modification affects where the cycle starts, effectively altering the position of the wave without changing its shape.
Other exercises in this chapter
Problem 8
Use \((10.10 .1)\) to determine \(L[f]\). $$f(t)=\left\\{\begin{array}{lr} 2, & 0 \leq t \leq 1 \\ t, & t > 1 \end{array}\right.$$
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Solve the given initial-value problem. $$y^{\prime \prime}-4 y^{\prime}+13 y=\delta(t-\pi / 4), \quad y(0)=3, \quad y^{\prime}(0)=0$$
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Make a sketch of the given function on \([0, \infty)\) and express it in terms of the unit step function. $$f(t)=\left\\{\begin{aligned}3, & 0 \leq t
View solution Problem 8
Use the Laplace transform to solve the given initial-value problem. \(y^{\prime \prime}+y^{\prime}-2 y=0, \quad y(0)=1, \quad y^{\prime}(0)=4\).
View solution