The equation for the instantaneous voltage across a discharging capacitor is given by π£ = πππ β π‘ π , where ππ is the initial voltage and π is the time constant of the circuit. The tasks are to: a) Draw a graph of voltage against time for ππ = 12π and π = 2π , between π‘ = 0π and π‘ = 10π . b) Calculate the gradient at π‘ = 2π and π‘ = 4π . c) Differentiate π£ = 12π β π‘ 2 and calculate the value of ππ£ ππ‘ at π‘ = 2π and π‘ = 4π . d) Compare your answers for part b and part c. e) Calculate the second derivative of the instantaneous voltage ( π 2 π£ ππ‘2 ).
Solution
The voltage across a discharging capacitor is given by
"v = {V_0}\\,e - \\tau t\\"
Using
"{V_0}=12 \\ V" and "\\tau = 2\\ s"
We have
"v = 12\\,e - 2 t\\"
This is a linear equation and its plot is shown below (graph of "v = {V_0}\\,e - \\tau t\\" voltage against time for "{V_0}=12 \\ V" and "\\tau = 2\\ s" , between "\ud835\udc61 = 0 \\ \ud835\udc60" and "\ud835\udc61 = 10\\ \ud835\udc60" .
Solution (b)
The above plot is a straight line. It means it has a constant gradient. From the equation "v = 12\\,e - 2 t\\" , the gradient is "m=-2".
Therefore, the gradient at π‘ = 2π is "m=-2" and π‘ = 4π is "m=-2".
Solution (c)
"v = 12\\,e - 2 t\\"
Its derivative is
"\\frac{dv}{dt} = -2"
Therefore, "\\frac{dv}{dt}" at π‘ = 2π and π‘ = 4π , is "\\frac{dv}{dt} = -2"
Solution (d)
From part (b) and part (c), we can say that "\\frac{dv}{dt}" gives the gradient of the curve/ line "v = 12\\,e - 2 t\\" , which is constant "m=-2" for all values of "t" .
Solution (e)
"v = 12\\,e - 2 t\\"
Its first derivative is
"\\frac{dv}{dt} = -2"
And the second derivative is
"\\frac{{{d^2}v}}{{d{t^2}}} = 0\\"
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