The resistance of a conductor is reduced to half its initial value. In doing so the heating effects in the conductor will become : a) Half b) One-fourth c) Four times d) Double
@Fifciol
@Festinger
The heating effect of a conductor is given by: \[P=VI\] Assume the conductor is ohmic and thus obeys ohm's law: \[V=IR\] Putting this in the first question you can see that \[P=I^{2}R\] Before making any changes, \[V=I_{1}R_{1}\] and so power is \[P_{1}=\frac{V^{2}}{R_{1}}\] But after we reduce the resistance, current will be another value, following ohm's law: \[V=I_{2}R_{2}\] But \[R_{2}=\frac{1}{2}R_{1}\] and so \[V=\frac{I_{2}R_{1}}{2}\] And thus \[I_{2}=\frac{2V}{R_{1}}\] and power is then: \[P_{2}=I^{2}R_{2}=\frac{4V^{2}R_{1}}{2R_{1}^{2}}=\frac{2V^{2}}{R_{1}}\] Comparing with the first result the heating effect doubles.
the heat effect increases because voltage is directly proportional to current as there it there is some heat but when the resistance of a conductor is reduced to half its initial value then the heat become d) doubled for example: the high voltage fire the materials.
power dissipiated as heat=v^2/r.. if r is halved.. heat produced doubles
\[P _{old} = I _{old} ^{2}R _{old}\] \[I _{new}=\frac{ V }{ R _{old}/2 }=\frac{ 2V }{ R _{old} }=2I _{old}\] \[P _{new}=I _{new}^{2}R _{new}=2^{^2} I _{old }^{2}R _{old}/2=\frac{ 4 }{ 2 } I _{old }^{2}R _{old}=2P _{old}\] It doubles.
thank you so much guys....for helping me @Festinger @Imtiaz7 @mr.singh @ybarrap
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