Electric Current – Understanding Delays in Electrical Current

This is an electronics design forum. You could use a current sense resistor (shunt) and a current sense amplifier, and feed the output to a comparator. This will cover the current detection part of the circuit. Then it is just a matter of timing the excursion.

If you don't want to program a microcntroller, you could have the comparator output enable a digital timer (and reset the timer on falling edge). The timer can be set up to stop counting when it reaches a certain count (the timeout count).

If you don't mind programming a microcontroller, you could just feed the comparator output to an input on the microcontroller.

I do see a problem in your specification, however. Suppose the TX button is stuck. The timer starts counting, then at some point it cuts power to the radio. Now the current drops below 1A, and the timer resets, turning the radio back on. But the TX button is still stuck, so you immediately jump right back into the same problem.

Give it some thought.

Lets look at this circuit in a slightly clearer topology - below is exactly the same circuit, but rearranged to put all the elements in a way that height is signifying voltage - the higher up in the diagram, the higher the voltage. (It's a nice analogy which helps visualise what is going on).

^{simulate this circuit – Schematic created using CircuitLab}

So, at the top of the diagram is \$20 + 10 = 30 \mathrm{V}\$. At the bottom is \$0 \mathrm{V}\$. So lets see if we can work out the currents \$I_r\$ and \$I_d\$. I should note that the direction I have drawn the current arrows is the direction that conventional current would have to flow (positive to negative).

Well, for \$I_r\$ it is fairly easy. Ohm's law tells us for a resistor (or any device with 'Ohmic' behaviour), that \$V=I\times R\$, so from this we can work out:

$$I_r = \frac{V}{R} = \frac{30}{50} = 0.6 \mathrm{A}$$

Why? Well, at the top of the diagram is \$30\mathrm{V}\$, and at the bottom is \$0\mathrm{V}\$, so there must be that much voltage across the resistor.

Now lets look at the diode. For a diode to conduct the voltage at the Anode must be higher than the voltage at the cathode ^(*). Now in this diagram we can see that the Anode is at \$20\mathrm{V}\$, and the cathode is at \$30\mathrm{V}\$, so this means the voltage across the diode \$V_ak = 20 - 30 = -10\mathrm{V}\$. So from this we can see that the diode is reverse biased - the voltage at the anode is negative with respect to the cathode. So we know then that \$I_d = 0 \mathrm{A}\$.

The current can't 'split down the parallel branch', because the diode is reverse biased so is blocking the flow of current - it's acting essentially as an open circuit.

If the diode was placed the other way around (not a good idea!), then current could flow down that branch. But the current that flows would not reduce the amount of current that flows through the resistor. Instead it increases the amount of current drawn from the 10V supply ^(**).

_{(*) There is some 'reverse leakage current' for a diode, basically the amount of current that it conducts when reverse biased, but this is pretty small so for simplicity we say it is \$0\$.}

_{(**) Assuming an ideal power supply - one which has no limit on how much current you can draw.}