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Zorluk: Çok zorElectric Current and Resistance

A metallic wire has a resistance of 12.0 Ω12.0\,\Omega at 0 ∘C0\,^\circ\text{C} and a temperature coefficient of resistance of 4.0×10−3 ∘C−14.0 \times 10^{-3}\,^\circ\text{C}^{-1}. The wire is uniformly stretched until its length increases by 25%25\%. Assuming the density and total volume of the wire remain constant during stretching, what is the resistance of the stretched wire at 50 ∘C50\,^\circ\text{C}?

Cevap: 22.5 Ω

Cevap

The resistance of the stretched wire at 50 ∘C50\,^\circ\text{C} is 22.5 Ω22.5\,\Omega.
Stretching a wire by 25%25\% increases its length by a factor of 1.251.25 and reduces its cross-sectional area by a factor of 1.251.25 (since volume is conserved). The resistance at 0 ∘C0\,^\circ\text{C} scales as (1.25)2=1.5625(1.25)^2 = 1.5625, giving 18.75 Ω18.75\,\Omega. Accounting for the temperature increase to 50 ∘C50\,^\circ\text{C} via R(T)=R0′(1+αT)R(T) = R'_0(1 + \alpha T) yields 18.75×(1+4.0×10−3×50)=18.75×1.20=22.5 Ω18.75 \times (1 + 4.0 \times 10^{-3} \times 50) = 18.75 \times 1.20 = 22.5\,\Omega.

Adım Adım Çözüm

1
Calculate the resistance of the wire at 0 ∘C0\,^\circ\text{C} after uniform stretching.
R0′=18.75 ΩR'_0 = 18.75\,\Omega
Uniform stretching by 25%25\% increases length to L′=1.25L0L' = 1.25 L_0. Volume conservation (V=ALV = A L) requires area to decrease to A′=A0/1.25A' = A_0 / 1.25. Since R=ρL/AR = \rho L / A, R0′=R0(L′/L0)2=12.0×(1.25)2=18.75 ΩR'_0 = R_0 (L'/L_0)^2 = 12.0 \times (1.25)^2 = 18.75\,\Omega.
2
Apply the temperature coefficient formula to calculate resistance at 50 ∘C50\,^\circ\text{C}.
R(50)=22.5 ΩR(50) = 22.5\,\Omega
Using R(T)=R0′(1+αT)R(T) = R'_0 (1 + \alpha T), substitute R0′=18.75 ΩR'_0 = 18.75\,\Omega, α=4.0×10−3 ∘C−1\alpha = 4.0 \times 10^{-3}\,^\circ\text{C}^{-1}, and T=50 ∘CT = 50\,^\circ\text{C} to find R(50)=18.75×(1+0.20)=22.5 ΩR(50) = 18.75 \times (1 + 0.20) = 22.5\,\Omega.

Anahtar Kavram

Combined effects of dimensional deformation and temperature on electrical resistance
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