Page 183 - NCERT Science Class 10 English Medium
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Figure 11.5 Electric circuit to study the factors on which the  resistance of conducting wires depends
               Figure 11.5
               Figure 11.5
               Figure 11.5
               Figure 11.5
                 n Now, plug the key. Note the current in the ammeter.
                 n Replace the nichrome wire by another nichrome wire of same thickness but twice the
                   length, that is 2l [marked (2) in the Fig. 11.5].
                 n Note the ammeter reading.
                 n Now replace the wire by a thicker nichrome wire, of the same length l  [marked (3)]. A
                   thicker wire has a larger cross-sectional area. Again note down the current through the
                   circuit.
                 n Instead of taking a nichrome wire, connect a copper wire [marked (4) in Fig. 11.5] in the
                   circuit. Let the wire be of the same length and same area of cross-section as that of the
                   first nichrome wire [marked (1)]. Note the value of the current.
                 n Notice the difference in the current in all cases.
                 n Does the current depend on the length of the conductor?
                 n Does the current depend on the area of cross-section of the wire used?




                                         It is observed that the ammeter reading decreases to one-half when
                                     the length of the wire is doubled. The ammeter reading is increased when
                                     a thicker wire of the same material and of the same length is used in the
                                     circuit. A change in ammeter reading is observed when a wire of different
                                     material of the same length and the same area of cross-section is used.
                                     On applying Ohm’s law [Eqs. (11.5) – (11.7)], we observe that the
                                     resistance of the conductor depends (i) on its length, (ii) on its area of
                                     cross-section, and (iii) on the nature of its material. Precise measurements
                                     have shown that resistance of a uniform metallic conductor is directly
                                     proportional to its length (l) and inversely proportional to the area of
                                     cross-section (A). That is,
                                                R ∝ l                                                 (11.8)
                                         and    R ∝ 1/A                                               (11.9)
                                     Combining Eqs. (11.8) and (11.9) we get

                                                     l
                                                R ∝
                                                     A
                                                      l
                                         or,    R = ρ                                                (11.10)
                                                      A
                                     where ρ (rho) is a constant of proportionality and is called the electrical
                                     resistivity of the material of the conductor. The SI unit of resistivity is
                                     Ω m. It is a characteristic property of the material. The metals and alloys



               178                                                                                   Science


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