The total resistance in the circuit with resistors connected

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1
Created by Boundless
The total resistance in the circuit with resistors connected in series is equal to the
A
sum of the inverse of each individual resistances
B
resistance of the smallest resistor
C
sum of the individual resistances
D
resistance of the largest resistor
2
Created by Boundless
The total resistance in the circuit with resistors connected in parallel is equal to the
A
sum of the individual resistances
B
sum of the inverse of each individual resistances
C
resistance of the smallest resistor
D
resistance of the largest resistor
3
Created by Boundless
A combination circuit contains resistors connected
A
only in series
B
either in series or in parallel
C
both in series and in parallel
D
4
only in parallel
Created by Boundless
One practical implication of a combination circuit is that
A
its resistance is extremely high
B
resistance in wires reduces the current and power delivered
to a resistor
C
all resistors are subject to the same voltage
D
the current through all of the resistors is the same
5
Created by Boundless
When voltage sources are connected in series,
A
both electromotive forces and resistances are additive
B
both electromotive forces and resistances are the same
C
electromotive forces are the same while resistances are
additive
D
electromotive forces are additive while resistances are the
same
6
Created by Boundless
When voltage sources are connected in parallel,
A
both electromotive forces and resistances are additive
B
electromotive forces are additive while resistances are the
same
C
electromotive forces are the same while resistances are
additive
D
both electromotive forces and resistances are the same
7
Created by Boundless
When the voltage sources are connected in the same polarity in series, they
A
produce a higher current
B
are additive and result in a higher total electromotive force
C
are subtractive and result in a lower total electromotive
force
D
can be used to charge the lower voltage source
8
Created by Boundless
The output, or terminal voltage of a voltage source such as a battery, depends
9
A
both on the electromotive force and internal resistance
B
both on the electromotive force and external resistance
C
only on the external resistance
D
only on the electromotive force
Created by Boundless
Terminal voltage (V) is calculated from the electromotive force (emf) using:
A
B
C
D
V = emf + I r , where r is the internal resistance and I is
the current flowing at the time of the measurement
−
emf
, where r is the internal resistance and I is the
current flowing at the time of the measurement
V =
Ir
emf
, where r is the internal resistance and I is the
Ir
current flowing at the time of the measurement
V =
V = emf − I r , where r is the internal resistance and I is
the current flowing at the time of the measurement
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