Metre Bridge - Special Case of Wheatstone Bridge

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Metre Bridge - Special Case of Wheatstone Bridge: Overview

This topic covers concepts, such as, Meter Bridge, Sensitivity of Meter Bridge Experiment, Construction of Meter Bridge, Limitation of Meter Bridge & Kelvin's Method to Determine Resistance of Galvanometer etc.

Important Questions on Metre Bridge - Special Case of Wheatstone Bridge

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In a meter bridge balance point is found at a distance   l 1  with resistances R and S as shown in the figure.

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When an unknown resistance X is connected in parallel with the resistance S, the balance point shifts to a distance l 2 . Find the expression for X in terms of   l 1 ,   l 2  and S.

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In a meter bridge experiment, resistances are connected as shown in figure. The balancing length l1= 55 cm. Now, an unknown resistance n11 Ω is connected in series with P and the new balancing length is found to be 75 cm . The value of n is (Given, P=4 Ω )

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How do you find the resistance of a wire using a meter bridge?

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What is balance point in Kelvin's method of determination of galvanometer resistance Shaalaa?

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What is the use of Kelvin's method?

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What is the use of Kelvin's method?

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What are the applications of meter bridge

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Why meter bridge is not suitable?

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What are the limitation of Metre bridge?

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On interchanging the resistances, the balance point of a meter bridge shifts to the left by 10 cm10 cm. The resistance of their series combination is . How much was the resistance on the left slot before interchanging the resistances?

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In a meter Bridge experiment resistance x is connected in the right gap. When R1 and R2 are connected in the left gap separately the balance points are 40 cm and 50 cm respectively from the left end. Now if both R1 & R2 are connected in series in the left gap with x in the right gap the new balance point from the left end (in cm) is l', what is the value of 2l'?

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The circuit diagram given in the figure shows the experimental setup for the measurement of unknown resistance by using a meter bridge. The wire connected between the points P & Q has non-uniform resistance such that resistance per unit length varies directly as the distance from the point P. Null point is obtained with the jockey J with R1 and R2 in the given position. On interchanging the positions R1 and R2 in the gaps the jockey has to be displaced through a distance Δ from the previous position along the wire to establish the null point. If the ratio of R1R2=3, find the value of Δ (in cm). Ignore any end corrections. [Take 3=1.7]

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In the given meterbridge, AB is a wire of uniform cross-section and its resistivity changing from A to B as ρ=ρ0x. If deflection in galvanometer is zero at P such that x=α, the value of α is.

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Figure shows a Meter bridge wire AC has uniform cross-section. The length of wire AC is 100 cm X is a standard resistor of 4 Ω and Y is a coil. When Y is immersed in melting ice the null point is at 40 cm from point A. When the coil Y  is heated to 100°C, a 12 Ω resistor has to beconnected in parallel with Y in order to keep the bridge balanced at the same point. The temperature coefficient of resistance of the coil is x×10-2 SI units. Find the value of x.

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Consider the meter bridge circuit without neglecting end corrections. If we used 100 Ω and 200 Ω resistance in place of R and S respectively, we get null deflection at l1=33.0 cm. If we interchange the resistances, the null deflection was found to be at l2=67.0 cm. If α and β are the end correction, then the value of α+β should be

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If the wire in the experiment to determine the resistivity of a material using metre bridge is replaced by copper or hollow wire the balance point i.e. null point shifts to

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Null method is superior over deflection method because

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Where do we get the balancing point of the meter bridge generally?

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In a practical meter bridge circuit as shown, when one more resistance of 100 Ω is connected in parallel with unknown resistance x, then ratio l1l2 become 2. l1 is balancing length. AB is a uniform wire. Then value of x must be:

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