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Resistance. Review of Resistors. The resis tance is a n intrinsic property of a material which impedes the flow of c harge requiring a pd to be applied so that there can be current flow. Review of Resistors.
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Review of Resistors • The resistance is an intrinsic property of a material which impedes the flow of charge requiring a pd to be applied so that there can be current flow.
Review of Resistors • The resistance is an intrinsic property of a material which impedes the flow of charge requiring a pd to be applied so that there can be current flow. • From ohm’s law, the resistance of a device is the ratio of the potential difference across it to the current flowing through it.
RC Circuits • The current in the previous circuits are time independent once the emf of the source is time independent.
RC Circuits • The current in the previous circuits are time independent once the emf of the source is time independent. • However we may have circuits which are time dependent. • An example is an RC circuit.
A RC circuit consists of a resistor R connected in series with a capacitor C.
The following circuit can be use the test the charging and discharging of the capacitor through the resistor.
Consider charging: • Initially the capacitor is uncharged.
Consider charging: • Initially the capacitor is uncharged. • When in the charging position current flows and the capacitor charges. • From Kirchoff’s law:
Which can be written as: • Since • We can rewrite the equation as,
Which can be written as: • Since • We can rewrite the equation as, • Doing some algebra,
Which can be written as: • Since • We can rewrite the equation as, • Doing some algebra, • We must separate the variables so that we can integrate and find the final charge on the capacitor.
Separating variables, • Integrating,
Separating variables, • Integrating,
Separating variables, • Integrating, • Which gives,
q(t) VbatC t • Taking the antilog and simplifying we get,
The product RC in the previous equation is called the time constant. • Has units of time. • Time taken for the charge to increase from zero to 63% of its final value.
Vc Vbat t • The pd across the capacitor • Which gives
The current for the charging • Which gives I(t) Vbat/R t
Consider discharging: • For the discharge position, the battery is no longer in the circuit.
Since • We can write that
Since • We can write that • Separating variables,
Since • We can write that • Separating variables, • Which in separated form is,
Integrating, • We get • Which after simplification is,
This can be written as, , noting that the initial charge is CVbat.
This can be written as, , noting that the initial charge is CVbat. • Differentiating gives the current, • The voltage across the capacitor is,
Limiting conditions: • At t=0, q= CVbat. • At t=inf, q= 0. q CVbat t
t I(t) Vbat t
Power • The net rate of energy transfer from the source (battery) P is given by, • Power is in watts(W) or joules/second • The rate at which energy is dissipated through through the resistor is, • The energy lost is in the form of thermal energy. • The power supplied to the capacitor is,
Energy • The total energy supplied by the battery in a time t is given by, • The total energy dissipated in a time t, • The total energy supplied to the capacitor in time t,
Energy • From the conservation of energy,
From the conservation of energy, • where,
From the conservation of energy, • where,
From the conservation of energy, • where,