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Current Electricity Test - 34

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Current Electricity Test - 34
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Weekly Quiz Competition
  • Question 1
    1 / -0
    What happens when negative terminal of cell is connected to other negative terminal of cell in a particular circuit?
    Solution
    1.1. Current means flow of electrons and electrons are negative charged and so are attracted to the positive end of the battery and repelled by the negative end.
    2.2. When battery is connected in a circuit that lets the electron flow through it, they flow from negative to positive.
    3.3. When negative terminal of cell is connected to other negative terminal of the cell in a particular circuit then, current will not flow in circuit as electrons cannot flow from negative to negative terminal.
  • Question 2
    1 / -0
    Which of the following has negative temperature coefficient of resistance?
    Solution

  • Question 3
    1 / -0
    In the series combination of two or more than two resistances.
    Solution
    For resistances in series, the current through each resistors remains the same.
  • Question 4
    1 / -0
    If the length of potentiometer wire is increased, then the length of the previously obtained balance point will
    Solution
    When the length of potentiometer wire is increased, the potential gradient decreases and the length of previous balance point is increased.
  • Question 5
    1 / -0
    Combine three resistors 5Ω,4.5Ω5\Omega, 4.5\Omega and 3Ω3\Omega in such a way that the total resistance of this combination is maximum:
    Solution
    Given resistance,
    R1=5ΩR2=4.5ΩR1=3ΩR_1=5\Omega\\R_2=4.5\Omega\\R_1=3\Omega

    In series combination effective resistance will be maximum.
    ie, Req=R1+R2+R3R_{eq}=R_1+R_2+R_3
         Req=5Ω+4.5Ω+3Ω=12.5ΩR_{eq}=5 \Omega + 4.5 \Omega + 3 \Omega = 12.5 \Omega

    Option A
  • Question 6
    1 / -0
    A (75 - j40 ) Ω\Omega load is the connected to a coaxial line of z0=75Ωz _ { 0 } = 75 \Omega The load matching on the line can be accomplished by connecting
    Solution
    A (75 - j40 ) ΩΩ load is the connected to a coaxial line of z0=75Ωz0=75Ω The load matching on the line can be accomplished by connecting a short circuit stub at the load.
    so the option is A.
  • Question 7
    1 / -0
    The value of II in the figure shown below is

    Solution
    Krichhoff's 1st law states that the total current flowing towards a junction is equal to the total current flowing away from that junction.
    At junction a :  I1=205 =15I_1 = 20 - 5  = 15 A
    At junction b :  I3=I1+4I_3=I_1 + 4
    \therefore I3=15+4=19I_3 =15 + 4 = 19 A
    At junction c : I2 =53=2I_2  = 5-3 =2 A
    At junction d :  I4=I3+I2I_4 = I_3 + I_2
    \therefore I4 =19+2=21I_4  = 19+2 =21 A

  • Question 8
    1 / -0
    The Kirchhoff's first law (\sumi=0) and second law (\sumiR=\sumE) , where the symbols have their usual meanings, are respectively based on :
    Solution
    Kirchhoffs first law says that no charge can be accumulated at a junction which implies conservation of charge Kirchhoffs second law states that the energy liberated in the circuit comes from the battery which implies the conservation of energy
  • Question 9
    1 / -0
    The resistance of a wire is 5 ohm at 5050^{\circ}C and 6 ohm at 100100^{\circ}C. The resistance of the wire at 00^{\circ}C will be:
    Solution
    R=R0(1+αΔT)R={ R }_{ 0 }(1+\alpha \Delta T)

    RR at 100 0C=6Ω{ 100 }^{  0} C=6\Omega

    RR at   500c=5Ω{  50}^{ 0 } c =5\Omega

    5(1+α(50))=6(1+α(100))\Rightarrow \dfrac{5}{(1+\alpha (50))}=\dfrac{6}{(1+\alpha (100))}

    6(1+α(50))=5(1+α(100))\Rightarrow 6(1+\alpha (50))=5(1+\alpha (100))

    α=1 200\Rightarrow \alpha =\dfrac { 1 }{  200}

    R=R0 (1+αΔT)R={ R }_{0  } (1+\alpha \Delta T)


    RR at 500C=5Ω{ 50 }^{ 0 } C =5\Omega

    R0 { R }_{0  }  at  00C=R 0{  0}^{ 0 } C ={ R }_{  0}

    R=R 0 (1+ 1 200 ×50)\Rightarrow R={R  }_{0  }(1+\dfrac {  1}{  200}  \times 50)

    5=R 0 (1+ 1 200 ×50)\Rightarrow 5={R  }_{0  }(1+\dfrac {  1}{  200}  \times 50)

    R0=4Ω \Rightarrow R_0 = 4\Omega  
  • Question 10
    1 / -0
    nn identical cells, each of internal resistance (r)(r) are first connected in parallel and then connected in series across a resistance (R)( R). If the current through RR is same in both the cases then: 
    Solution
    If the emf of each cell be E, then for parallel connection, equivalent emf is 

    Eeq=E1r1+E2r2+....1r1+1r2+....=Er+Er+....1r+1r+.....=EE_{eq}= \dfrac{\dfrac{E_1}{r_1}+\dfrac{E_2}{r_2}+....}{\dfrac{1}{r_1}+\dfrac{1}{r_2}+....}= \dfrac{\dfrac{E}{r}+\dfrac{E}{r}+....}{\dfrac{1}{r}+\dfrac{1}{r}+.....}=E

    And equivalent internal resistance of the cells, req=rnr_{eq}=\dfrac{r}{n}

    So net current in parallel connection is

    Ip=Eeqreq+R=Ern+RI_p=\dfrac{E_{eq}}{r_{eq}+R}=\dfrac{E}{\dfrac{r}{n}+R}

    And for series connection of cells, eqv emf , Eeq=E1+E2+...=nEE_{eq}= E_1+E_2+...=nE

    and equivalent internal resistance for series, req=r1+r2+....=nrr_{eq}= r_1+r_2+....=nr

    So current ,Is=Eeqreq+R=nEnr+RI_s=\dfrac{E_{eq}}{r_{eq}+R}=\dfrac{nE}{nr+R}

    Now according to question, both the currents are equal.

    So, Ip=IsI_p=I_s reduces to Ern+R=nEnr+R\dfrac{E}{\dfrac{r}{n}+R}=\dfrac{nE}{nr+R} which gives R=rR=r
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