Numerical methods for solving ordinary differential equations (ODEs) can be classified as single-step or multistep methods.
Let's analyze the options:
(a) Successive approximation method (e.g., Picard's iteration): This is an iterative method for solving ODEs or integral equations, generally considered single-step in its basic form of progression.
(b) Adams-Bashforth method: This is a family of explicit multistep methods for solving ODEs. For example, the two-step Adams-Bashforth method uses \(y_n\) and \(y_{n-1}\) (and their derivatives) to find \(y_{n+1}\).
(c) Runge-Kutta method: This is a family of single-step methods. They achieve higher accuracy by evaluating the derivative function \(f(t,y)\) at multiple intermediate points within a single step.
(d) Euler's method: This is the simplest single-step method: \(y_{n+1} = y_n + h f(t_n, y_n)\). Therefore, the Adams-Bashforth method is a multistep method. (Note: While some methods listed can be adapted for BVPs, multistep methods are primarily developed for IVPs of ODEs. The question wording is a bit broad.) \[ \boxed{\text{Adams - Bashforth method}} \]
When the enable data input \( D = 1 \), select inputs \( S_1 = S_0 = 0 \) in the 1×4 Demultiplexer, then the outputs \( Y_0, Y_1, Y_2, Y_3 \) are
The \( Z \) parameter \( Z_{21} \) of the following circuit is
The \( h \) parameters of the following circuit is
For an input voltage \( v = 10 \sin 1000t \), the Thevenin's impedance at the terminals X and Y for the following circuit is