# B sources

B sources are one of the most powerful components in EasyEDA. They are available as a BV voltage source and as BI current source (although in fact at the spice netlist level they are the same device just defined to have a voltage or a current output).

The function of every B source is defined by an equation.

The left hand side of the equation defines whether the output of the source is a voltage or a current.

The right hand side is an expression made up from numbers, the basic arithmetic operators and functions not only of parameters but, crucially, of dynamic voltages and currents from within the circuit being simulated. In other words, B sources can perform a range of functions in simulations that is limited only by the imagination of the simulation designer.

The syntax of the equations to define a BV source in EasyEDA is very simple:

V=expression

For example:

V=3*V(a,b)

defines a BV source that generates an output voltage equal to 3 times the difference between the voltage on the ‘a’ net (V(a)) and the voltage on the ‘b’ net (V(b)).

V=scale*uramp(V(a,b))/ABS(I(Vimon))

defines a BV source that generates an output voltage equal to the parameter, scale, multiplied by the positive difference between the voltage on the ‘a’ net (V(a)) and the voltage on the ‘b’ net (V(b)), divided by the absolute value of the current through the 0V source Vimon (I(Vimon)).

V=Vswingtanh(V(a,b)Avol)

defines a differential gain block with an small signal gain of Avol and an output voltage swing which is limited with a tanh function to +/-Vswing.

The syntax of the equations to define a BI source in EasyEDA is basically the same as for BV sources except that **V** for voltage is replaced by **I** for current:

I=expression

I=V(a)*I(Vimon)

defines a BI source that generates an output current equal to the voltage on the ‘a’ net (V(a)) multiplied by the current through the 0V source Vimon (I(Vimon)).

I=LIMIT(V(a), 3, minval^2)

defines a BI source that generates an output current equal to the voltage on the ‘a’ net (V(a)) but clamped to the value of 3 and the square of the value of the minval parameter for all values of V(a) outside the range defined by 3 and minval^2.

I=V(a,b)/Rval

when the ‘-‘ and ‘+’ terminals of the B source are named ‘a’ and ‘b’ respectively then this expression defines a resistor of value Rval.

Note that curly brackets are not used in expressions for B Sources.

There are several examples of the uses of B Sources in the following simulations.

**Note that when entered directly in a B Source value field in a schematic, expressions MUST be on a single line. When used like this, they cannot be wrapped over more than one line.**

Expressions entered into a netlist, however, such as inside a .subckt model definition, can wrap over more than one line by using the ‘+’ continuation character. Several examples of this can be found by inspecting the netlists of circuits using some of the EasyEDA .subckt models. For example in the netlist of the opamp5pEE Parameterised 5 pin opamp model there are these B sources:

Bipbias1 inp isum I=(ibias+ios)*V(supply_ok) + |

and:

Bstg1 0 stage1 I=Islew*tanh(V(indiff)*Kg) |

and in the opamp_ANF01 .subckt found elsewhere in this document, there is another example:

B1 out 0 + V=(TANH((V(inp)-V(inn))*{Avol}*2/(V(vcc)-V(vee)))*(V(vcc)-V(vee)) + +(V(vcc)+V(vee)))/2 |