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Welcome to electron line now let's take a look at inductance in graphical form here we look at the equation V equals L times DI DT that equates the voltage across an inductor to the inductance and the rate of change that are currently respect to time, but that equation has the form like the algebra equation y equals MX plus B where m is the slope and B is the y-intercept now for a moment imagine B to be 0 now we can see that V equals L DI DT is like the equation y equals MX where m is the slope since M is the slope here that then indicates that L would be the slope of this equation V would be the dependent variable and the DT would represent the independent variable so when we draw the graph here on the vertical axis we have the voltage across the inductor on the horizontal axis we have the rate of change that a current respect to time, and then we would draw a straight line like this the slope of this line represents the inductance of the inductor that represents the relationship between the voltage across the inductor and the rate of change the current with respect to time through the inductor now if the inductance is large with other words into physical properties of the inductor such that you have a large inductance then you would have a slope that looks like this you would have a steeper slope, so this is a larger inductance and if you have a smaller inductor with smaller inductance down the slope would look something like this but in other words with the rate of change that the current it would then cause a small change in the voltage where in this case the rate of change the current would create a large voltage across the inductor, so this would be a small inductor or small inductance and that would then represent a larger inductance, but again you can see how this simply represents the size of the inductor or the inductance of the inductor relative to the proportion of the change in the current to the voltage across the inductor and that's how we do that graphically
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