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- Fourier Series
- Fourier Series
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- Fourier Transform
- Fourier Transforms
- Fourier Transforms Properties
- Fourier Transform – Representation and Condition for Existence
- Properties of Continuous-Time Fourier Transform
- Table of Fourier Transform Pairs
- Linearity and Frequency Shifting Property of Fourier Transform
- Modulation Property of Fourier Transform
- Time-Shifting Property of Fourier Transform
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- Parseval’s Theorem & Parseval’s Identity of Fourier Transform
- Fourier Transform of Complex and Real Functions
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- Analysis of LTI System with Fourier Transform
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- Convolution and Correlation
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- Laplace Transform
- Laplace Transforms
- Common Laplace Transform Pairs
- Laplace Transform of Unit Impulse Function and Unit Step Function
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- Laplace Transforms Properties
- Linearity Property of Laplace Transform
- Time Shifting Property of Laplace Transform
- Time Scaling and Frequency Shifting Properties of Laplace Transform
- Time Differentiation Property of Laplace Transform
- Time Integration Property of Laplace Transform
- Time Convolution and Multiplication Properties of Laplace Transform
- Initial Value Theorem of Laplace Transform
- Final Value Theorem of Laplace Transform
- Parseval's Theorem for Laplace Transform
- Laplace Transform and Region of Convergence for right sided and left sided signals
- Laplace Transform and Region of Convergence of Two Sided and Finite Duration Signals
- Circuit Analysis with Laplace Transform
- Step Response and Impulse Response of Series RL Circuit using Laplace Transform
- Step Response and Impulse Response of Series RC Circuit using Laplace Transform
- Step Response of Series RLC Circuit using Laplace Transform
- Solving Differential Equations with Laplace Transform
- Difference between Laplace Transform and Fourier Transform
- Difference between Z Transform and Laplace Transform
- Relation between Laplace Transform and Z-Transform
- Relation between Laplace Transform and Fourier Transform
- Laplace Transform – Time Reversal, Conjugation, and Conjugate Symmetry Properties
- Laplace Transform – Differentiation in s Domain
- Laplace Transform – Conditions for Existence, Region of Convergence, Merits & Demerits
- Z Transform
- Z-Transforms (ZT)
- Common Z-Transform Pairs
- Z-Transform of Unit Impulse, Unit Step, and Unit Ramp Functions
- Z-Transform of Sine and Cosine Signals
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- Z-Transforms Properties
- Properties of ROC of the Z-Transform
- Z-Transform and ROC of Finite Duration Sequences
- Conjugation and Accumulation Properties of Z-Transform
- Time Shifting Property of Z Transform
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- Differentiation in z Domain Property of Z Transform
- Initial Value Theorem of Z-Transform
- Final Value Theorem of Z Transform
- Solution of Difference Equations Using Z Transform
- Long Division Method to Find Inverse Z Transform
- Partial Fraction Expansion Method for Inverse Z-Transform
- What is Inverse Z Transform?
- Inverse Z-Transform by Convolution Method
- Transform Analysis of LTI Systems using Z-Transform
- Convolution Property of Z Transform
- Correlation Property of Z Transform
- Multiplication by Exponential Sequence Property of Z Transform
- Multiplication Property of Z Transform
- Residue Method to Calculate Inverse Z Transform
- System Realization
- Cascade Form Realization of Continuous-Time Systems
- Direct Form-I Realization of Continuous-Time Systems
- Direct Form-II Realization of Continuous-Time Systems
- Parallel Form Realization of Continuous-Time Systems
- Causality and Paley Wiener Criterion for Physical Realization
- Discrete Fourier Transform
- Discrete-Time Fourier Transform
- Properties of Discrete Time Fourier Transform
- Linearity, Periodicity, and Symmetry Properties of Discrete-Time Fourier Transform
- Time Shifting and Frequency Shifting Properties of Discrete Time Fourier Transform
- Inverse Discrete-Time Fourier Transform
- Time Convolution and Frequency Convolution Properties of Discrete-Time Fourier Transform
- Differentiation in Frequency Domain Property of Discrete Time Fourier Transform
- Parseval’s Power Theorem
- Miscellaneous Concepts
- What is Mean Square Error?
- What is Fourier Spectrum?
- Region of Convergence
- Hilbert Transform
- Properties of Hilbert Transform
- Symmetric Impulse Response of Linear-Phase System
- Filter Characteristics of Linear Systems
- Characteristics of an Ideal Filter (LPF, HPF, BPF, and BRF)
- Zero Order Hold and its Transfer Function
- What is Ideal Reconstruction Filter?
- What is the Frequency Response of Discrete Time Systems?
- Basic Elements to Construct the Block Diagram of Continuous Time Systems
- BIBO Stability Criterion
- BIBO Stability of Discrete-Time Systems
- Distortion Less Transmission
- Distortionless Transmission through a System
- Rayleigh’s Energy Theorem
Laplace Transform - Conditions for Existence, Region of Convergence, Merits & Demerits
Laplace Transform
The Laplace transform is a mathematical tool which is used to convert the differential equations in time domain into the algebraic equations in the frequency domain or s-domain.
Mathematically, if x(t) is a time domain function, then its Laplace transform is defined as −
$$\mathrm{L[x(t)]\:=\:X(s)\:=\:\int_{-\infty}^{\infty}\:x(t)\:e^{-st} \: dt \quad \dotso\: (1)}$$
Where, s is a complex variable and it is given by,
$$\mathrm{s\:=\:\sigma\:+\:j\omega}$$
And the operator L is called the Laplace transform operator which transforms the time domain function into the s-domain function.
Since a linear time invariant (LTI) system is described by differential equations and the response of the system for a given input is obtained by solving the differential equations relating its input and output. But the solution of higher order differential equations is very tedious and time consuming, so the Laplace transform is used to solve these differential equations. The Laplace transform converts the time domain differential equations into the algebraic equations in s-domain, get the solution in s-domain and then the solution in time domain can be obtained by the taking inverse Laplace transform of the solution.
Conditions for Existence of Laplace Transform
The Laplace transform of a function x(t), i.e., function X(s) exists only if
$$\mathrm{\int_{-\infty}^{\infty}\: \left| x(t) e^{-\sigma t} \right| \: dt\: \lt \:\infty}$$
Or, only if,
$$\mathrm{\lim_{t \to \infty}\: x(t) e^{-st} \:=\: 0}$$
Therefore, the necessary and sufficient conditions for the existence of the Laplace transform are −
- The function x(t) should be piece-wise continuous in the given closed interval and must be of exponential order.
- The function $\mathrm{x(t)e^{-st}}$ should be absolutely integrable
Region of Convergence of Laplace Transform
The region of convergence (ROC) is defined as the set of points in the s-plane for which the Laplace transform of function x(t) (i.e., the function X(s)) converges.
Explanation − For a given function x(t), the Laplace transform as given by the equation (1) may not converge for all values of the complex variable s. Since every value of the variable (s) corresponds to a particular point in the s-plane. If there is no value corresponding to the variable (s), i.e., no point on the splane for which the Laplace integral converges. Then, the function x(t) does not have a region of convergence (ROC) and hence it is not Laplace transformable.
Properties of Region of Convergence of Laplace Transform
Following are the properties of the ROC of Laplace transform −
- The ROC of Laplace transform does not contain any poles.
- The ROC of the Laplace transform of x(t), i.e., function X(s) is bounded by poles or extends up to infinity.
- The ROC of the sum of two or more signals is equal to the intersection of the ROCs of those signals.
- The ROC of Laplace transform must be a connected region.
- If the function x(t) is a right-sided function, then the ROC of X(s) extends to the right of the right most pole and no-pole is located inside the ROC.
- If the signal x(t) is a left-sided signal, then the ROC of Laplace transform X(s) extends to the left of the left most pole and no pole is located inside the ROC.
- If the signal x(t) is a two-sided signal, then the ROC of the Laplace transform X(s) is a strip in the s-plane bounded by the poles and nopole is located inside the ROC.
- The impulse signal is the only signal for which the ROC is the entire splane.
- The imaginary axis of the s-plane is contained by the ROC of a stable LTI system.
Merits and Demerits of Laplace Transform
Following are some of the merits of using the Laplace transform technique −
- The Laplace transform has a convergence factor and hence it is more general than Fourier transform. That means, the signals which are not convergent in Fourier transform are convergent in the Laplace transform.
- Using Laplace transform, the differential equations describing a system can be converted into simple algebraic equations. Hence, the analysis of the LTI systems using Laplace transform becomes easier.
- The Laplace transform can be used to analyse the unstable systems.
- The convolution operation in time domain can be converted into multiplication in s-domain.
- s = jω is used only for steady-state sinusoidal analysis.
- Using Laplace transform technique, the frequency response of the system cannot be drawn or estimated. Only the pole-zero plot can be drawn.