21.5 Null Measurements
Potentiometers and the Wheatstone bridge, balanced to zero deflection so a reading no longer depends on the meter's own resistance.
5 exercises
21.5 Exercise 1
This equation is used to calculate the unknown resistance when current through the galvanometer is zero. This method can be very accurate (often to four significant digits), but it is limited by two factors. First, it is not possible to get the current through the galvanometer to be exactly zero. Second, there are always uncertainties in , , and , which contribute to the uncertainty in .
Identi…
21.5 Exercise 4
What is the of a cell being measured in a potentiometer, if the standard cell’s emf is 12.0 V and the potentiometer balances for and ?
21.5 Exercise 6
When an unknown resistance is placed in a Wheatstone bridge, it is possible to balance the bridge by adjusting to be . What is if ?
21.5 Exercise 8
(a) What is the unknown in a potentiometer that balances when is , and balances when is for a standard 3.000-V emf? (b) The same is placed in the same potentiometer, which now balances when is for a standard emf of 3.100 V. At what resistance will the potentiometer balance?
21.5 Exercise 9
Suppose you want to measure resistances in the range from to using a Wheatstone bridge that has . Over what range should be adjustable?
Adapted from College Physics © 2022 Rice University. Licensed under CC BY 4.0. Sources: College Physics 2e, College Physics for AP® Courses 2e. Imported at revision f98d7a7.