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A Wheatstone bridge is constructed using a \(1.00-\mathrm{m}\) -long Nichrome wire (the purple line in the figure) with a conducting contact that can slide along the wire. A resistor, \(R_{1}=100 . \Omega\), is placed on one side of the bridge, and another resistor, \(R\), of unknown resistance, is placed on the other side. The contact is moved along the Nichrome wire, and it is found that the ammeter reading is zero for \(L=25.0 \mathrm{~cm} .\) Knowing that the wire has a uniform cross section throughout its length, determine the unknown resistance.

Short Answer

Expert verified
Answer: The unknown resistance in the Wheatstone bridge is 300Ω.

Step by step solution

01

Write the balanced condition for the Wheatstone Bridge

The balanced condition of the Wheatstone bridge states that the ratio of the resistances in the two branches of the bridge is equal. That is: \(\dfrac{R_{A}}{R_{B}}=\dfrac{R_{1}}{R}\) Here, \(R_A\) and \(R_B\) are the resistances of the segments of the Nichrome wire having lengths \(L\) and \((1.00 - L)\) respectively.
02

Find resistance of Nichrome wire segments

Now, let's write the resistance formula for a wire and find the resistances of the two segments of the Nichrome wire in terms of their lengths: \(R_{A}=\frac{\rho L}{A}\) and \(R_{B}=\frac{\rho(1.00-L)}{A}\) Here, \(\rho\) is the resistivity of the Nichrome wire, which remains constant throughout the wire, and \(A\) is the cross-sectional area of the wire. Since the entire wire has a uniform cross section, \(A\) is the same for both segments.
03

Substitute expressions for wire resistances

Now, substitute the expressions for \(R_A\) and \(R_B\) found in step 2 back into the balanced condition equation found in step 1: \(\frac{\frac{\rho L}{A}}{\frac{\rho(1.00-L)}{A}} = \frac{100\Omega}{R}\)
04

Simplify the equation and solve for the unknown resistance

Simplify the previous equation and solve for the unknown resistance \(R\): \(\frac{L}{1.00-L} = \frac{100\Omega}{R}\) We're given that \(L = 25.0\ \text{cm} = 0.250\ \text{m}\). Substitute this value into the equation and solve for \(R\): \(\frac{0.250}{1.00 - 0.250} = \frac{100\Omega}{R}\) Rearrange the equation to isolate \(R\): \(100\Omega \cdot \frac{1.00 - 0.250}{0.250} = R\) Calculate R: \(100\Omega \cdot \frac{0.75}{0.250} = R\) \(R = 300\Omega\) The unknown resistance in the Wheatstone bridge is \(300\Omega\).

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Most popular questions from this chapter

An ammeter with an internal resistance of \(53.0 \Omega\) measures a current of \(5.25 \mathrm{~mA}\) in a circuit containing a battery and a total resistance of \(1130 \Omega\). The insertion of the ammeter alters the resistance of the circuit, and thus the measurement does not give the actual value of the current in the circuit without the ammeter. Determine the actual value of the current.

During a physics demonstration, a fully charged \(90.0-\mu \mathrm{F}\) capacitor is discharged through a \(60.0-\Omega\) resistor. How long will it take for the capacitor to lose \(80.0 \%\) of its initial energy?

Many electronics devices can be dangerous even after they are shut off. Consider an \(\mathrm{RC}\) circuit with a \(150 .-\mu \mathrm{F}\) capacitor and a \(1.00-\mathrm{M} \Omega\) resistor connected to a 200.-V power source for a long time and then disconnected and shorted, as shown in the figure. How long will it be until the potential difference across the capacitor drops to below \(50.0 \mathrm{~V} ?\)

Consider a series \(\mathrm{RC}\) circuit with \(R=10.0 \Omega\) \(C=10.0 \mu \mathrm{F}\) and \(V=10.0 \mathrm{~V}\) a) How much time, expressed as a multiple of the time constant, does it take for the capacitor to be charged to half of its maximum value? b) At this instant, what is the ratio of the energy stored in the capacitor to its maximum possible value? c) Now suppose the capacitor is fully charged. At time \(t=0,\) the original circuit is opened and the capacitor is allowed to discharge across another resistor, \(R^{\prime}=1.00 \Omega,\) that is connected across the capacitor. What is the time constant for the discharging of the capacitor? d) How many seconds does it take for the capacitor to discharge half of its maximum stored charge, \(Q ?\)

A battery has \(V_{e m f}=12.0 \mathrm{~V}\) and internal resistance \(r=1.00 \Omega\). What resistance, \(R,\) can be put across the battery to extract \(10.0 \mathrm{~W}\) of power from it?

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