KCET 2020 Physics Questions with Answers Key Solutions
Solution:
gh=g(1−2hR)
gd=g(1−dR)
⇒gh=gd
g(1−2hR)=g(1−dR)
⇒d=2h=2×10=20km
Solution:
Young’s modulus = stress/strain, and for a perfect rigid body we know that strain is equal to 0 and hence Young’s modulus of a perfect rigid body becomes Infinity.
Solution:
ω1=0
ω2=10radsect=5sec
θ=ω1+ω22×t
=102×5=25rad
Solution:
Let V be the total volume of the iceberg and V′ of its volume be submerged into water
Floatation condition weight of iceberg = Weight of water displaced by submerged part by ice
Vρig=V′ρwg
⇒V′/V=ρi/ρw
=0.917/1=0.917
Solution:
Surface area is more for plate and less for sphere. Hence plate will cool the fastest and sphere the slowest.
Solution:
In an adiabatic expansion as temperature decreases from an ideal gas equation PV=nRT.
Product of pressure and volume also decreases.
Solution:
The heat Q is converted into the internal energy and work. According to the first law of thermodynamics,
Q=U+W
⇒nCpΔt=nCvΔt+W
WQ=nCpΔt−nCvΔtnCpΔt
cp−cvcp=1−1γ
=1−153=25
Solution:
We know that
T=2π√mkeff
32=2π√122k
⇒94=4π2×122kk≈105Nm−1
Solution:
Whistling train is the source of sound, vs=B. Before crossing a stationary observer on station, frequency heard is n′=vn(v−vs)=vnv−V= constant, and n′>n2. Here , v is velocity of sound in air and n is actual frequency of whistle. After crossing the stationary observer, frequency heard is n′=v(v+vs)=vv+V= constant and $n^{\prime}
Solution:
ACCORDING TO THE GIVEN PROBLEM, THE CHARGE IS PLACED AT THE CORNER OF THE CUBE AS SHOWN IN FIGHURE_1,
NOW CONSIDER THE ANOTHER FIGURE_2 IN WHICH THE WHOLE CHARGE IS ENCLOSED IN THE FOUR SUCH CUBE,
NOW CALCULATING THE FLUX THROUGH THE ALL CUBES AS TOTAL:
ϕe=qϵ0=EA
WHERE A =6∗(2a)2
FOR ONLY ONE SIDE OF FIRST CUBE,
AREA WILL BE A 0=a2
FROM ABOVE DATA FLUX THROW THE SINGLE FACE (AREA = A0 ) IS GIVEN BY:
ϕe=Qϵ0=EA0
WHERE Q =q24
SO THE FLUX THROUGH THROUGH THE SINGLE FACE IS q24ϵ0;
Solution:
We know that
F=qE=20×20×10−6
=4×10−4V/m−1
Solution:
We know that
E=λ2πε0r
=14×10−210−2×18×109×5
=2.25×108N/C
Solution:
Dipole moment =p electric field =E centroid axis =I Explanation When displaced at an angle θ from its mean position the magnitude of restoring torque is T= −psinθ For small angular displacement sinθ≈θ T=−pEθα=TI=−(PEI)θ=−w2θw2=PEIT=2π√IPE (P.E = moment in electric field)
Solution:
CP−C=6μF
2C−(C/2)=6
C=4μF
Solution:
Electric lines of force in an electric field always flow from a higher potential to a lower potential.
Hence, VA=VB>VC
Solution:
When the radius of a soap bubble increases, the soap bubble gets charged.
Solution:
12mv2=Vq
v=√2Vqm
=2.1×107ms−1
Solution:
Resistance is inversely proportional to area.
Hence resistance will be maximum when the battery is connected across 1cm× (1/2)cm faces.
Solution:
V=E−ir=10.4V
Solution:
Emf of cell in the secondary circuit =potential gradient x balancing length
⇒(10/5)×2=4V
Solution:
Red, Grey, Brown, Silver
Solution:
5/6Ω
Solution:
Slope =1/R=A/ρl
Hence the slope becomes less if the length of the wire is increased.
Solution:
μ0i4π→dl×→rr3
Solution:
The magnetic field increases as the point moves closer to the boundary of the wire and decreases as it moves away from the boundary of the wire.
Solution:
K.E. =q2/m
Hence, a deuteron gains the least kinetic energy.
Solution:
I∝BT
I2I1=B2B1×T1T2
I2=23A/m
Solution:
Magnetic field at the center of the current carrying loop is given by
B= (μ0/4π)×(2πi/a)=(μ0i)/2a.
Magnetic moment at the center of the current carrying loop is given by
M=πa2
thus B/M=μ0/(2πa3)=x( given )
when both current and radius are doubled ratio become x/8 times.
Solution:
A permanent magnet at room temperature retains a ferromagnetic property that possesses a dipole moment. And domains are partially aligned due to thermal agitation.
Solution:
We know that the current,
i=BIv/R=(0.04×2×5)/3=133mA
Solution:
Average induced emf, ϵ=Ldl/dt
=0.2((5−2)/0.5)=2/5×3=1.2V
Solution:
V0=√V2R+(VL−VC)2
=√602+(1102−302)=100
Vrms=V0√2=100√2
=100√2×√2√2=100×√22
=50×1.414=70.7V
Q34. The power factor of R-L circuit is 1√3. If the inductive reactance is 2Ω. The value of resistance is
Solution:
cosϕ=1√3,tanϕ=√21tanϕ
=XLR√2=2R
⇒R=√2Ω
Solution:
Resonant frequency of an circuit is given by
f=12π√LC
=12π√0.5×10−3H×20×10−6F
=1592Hz
Solution:
Intensity I=E/A
where E is energy of radiation and A is incident area
⇒E=IA
Momentum of radiation is given by
P=2E/c=2IA/c
Where c is speed of light.
P=2×20×104Wm2×375×10−4m23×108m/s
=5×10−5kgms−1
Solution:
Velocity of image in convex lens Vi=(f/(f+u))2Vo
and image will move from focus to infinity (i.e. away from the lens).
From the formula, velocity of image
(dVi)/dt=(dVi/du)×(du/dt)
=2(f/f+u)fln(f+u)×5 (because du/dt=5m/s)
⇒(dVi)/dt=10f2ln(f+u)/(f+u)
We can see that acceleration of image ∝ln(f+u),
i.e varies with distance of object
So the image moves away from the lens with a non-uniform acceleration
Solution:
n=sin(A+dm2)sin(A2)
⇒cot(A2)=sin(A+dm2)sin(A2)
⇒cos(A2)sin(A2)=sin(A+dm2)sin(A2)
⇒sin(90−A2)=sin(A+dm2)
⇒90−A2=A+dm2
⇒180−2A=dm
Solution:
So, here when we put the concave lens,
let the beam will converge at a distance x=v
Using lens formulae, we have, 1/f=1/v−1/u
Where u=12cm and f=−16cm is given
∴1/v=(1/f)+(1/u)
=(−1/16)+(1/12)=1/48cm
⇒v=48cm
Hence, x=48cm
Solution:
We have unpolarised beam's intensity
I0=128w/m2
Using Malu's law we have
I=I0cos2θ
When beam passed from the first polaroid,
I=I0/2
Again, as the angle between p1 and p2 is 45∘,
beam intensity when it will pass p2 would be
l1=I0/2cos2450=I0/4
And, also the angle between p2 and p3 is 45∘,
beam intensity when it will come out of p3 will be
l2=I0/4cos2450=I0/8
=128/8=16w/m2
Solution:
Given the lateral separation of the poles d=3.14m
The resolving power of the eye is
θ=1min rad
The maximum distance from which poles are distinctly visible is
D = d / \theta
\Rightarrow D =(3.14 \times 60 \times 180) / \pi
=10800 \,m =10.8 \,km
Solution:
Path difference due to insertion of mica sheet \Delta x =(\mu-1) t
Let the shift in the fringe pattern be 'y'
Also, path difference \Delta x=y \times d / D,
so comparing both (\mu-1) t=y \times(d / D)
y =(\mu-1) t \times( D / d ),
where \mu=1.5, D =2.4 and d =1.2
putting the values, we get
y =0.25 \,mm.
Solution:
De-Broglie wavelength is given by
\lambda=12.27 / \sqrt{ E }_{0},
where E _{0} is the ground state energy of the hydrogen atom
whose value is 13.6\, V
\therefore \lambda=12.27 /(\sqrt{1} 3.6)=3.33 \,\mathring{A}
Solution:
Here in the graph we can see that, the Stopping potential is same for 1 and 2 . So, frequencies will be same i.e. \gamma _{1}= \gamma _{2} and, currents are different. So, intensity are different i.e. I_{1} \neq I_{2}.
Solution:
As we know that time period of revolution of an electron is
T =2 \pi r / v,
And r \propto n^{2} / Z^{2} and v \propto Z / n
\therefore T \propto n ^{3} / Z ^{2} and for H -atom
Z =1, T \propto n ^{3}
Solution:
Angular momentum,
L =\frac{ nh }{2 \pi}=\frac{3 h }{2 \pi}
given
also n =3
\therefore E =\frac{-1.36}{ n ^{2}} eV
E =\frac{-13.6}{(3)^{2}} eV
E =\frac{-13.6}{9} eV
E = -1.57 \,eV
Solution:
A' will be maximum and B' will be minimum, because atom is hollow and whole mass of the atom is concentrated in a small centre called nucleus.
Solution:
Nuclear forces are short range force existing in the range of a 10^{-15} m.
If the separation between the particles is greater than 10^{-15} m,
nuclear force is negligible.
Therefore, at a separation of 10 \,nm,
the electromagnetic force is greater than the nuclear force.
Hence, F _{ e } > > F _{ n }
Solution:
During β^- decay, a neutron in the nucleus decays emitting an electron.
Q50. A radio-active elements has half-life of 15 years. What is the fraction that will decay in 30 years?
Solution:
Fraction un decayed is given as,
N / N _{0}=(1 / 2)^{( t / T )}
Here, t =30 years and T =15 years
So,
N / N _{0}=(1 / 2)^{((30 \text { years }) /(15 \text { years }))}
or, N / N _{0}=(1 / 2)^{2}
or, N / N _{0}=1 / 4
Therefore,
Fraction un decayed =1- N / N _{0}
or, Fraction un decayed =1-(1 / 4)
or, Fraction un decayed =3 / 4=0.75
Solution:
During the positive half cycles of input ac, a p-n junction diode is forward biased and hence it conducts.
While during the negative half cycles, the diode will be reverse biased and hence does not conduct.
The capacitor is charged to maximum potential difference.
Therefore, the potential difference across capacitor C is equal to the peak value of the applied ac voltage, i.e..
V = V _{\max }
or, V =\sqrt{2} V _{ rms }
or, V =\sqrt{2} \times 220 \,V =200 \sqrt{2}\, V
Solution:
A NAND gate gives an output 1 if at least one of the inputs is zero.
Hence Q is 1 .
Therefore, the inputs for the upper NAND gate are 1,1 .
Hence P =0.
Solution:
A positive hole in a semiconductor is a vacancy which is created at the site of a covalent bond when an electron leaves a covalent bond.
Solution:
The magnetic field due to a long straight current carrying wire is given by,
B =\left(\mu_{0} I \right) / 2 \pi r
or, B \propto 1 / r
At the point exactly mid-way between the conductors, the net magnetic field is zero. Using right hand thumb rule, we find that the magnetic field due to left wire will be in \hat{j} direction while due to the right wire is in (-\hat{j}) direction.
Magnetic field at a distance x from the left wire, lying between the wires.
B=\frac{\mu_{0} I}{2 \pi x} \hat{j}+\frac{\mu_{0} I}{2 \pi(2 d-x)}(-\hat{j})
or, B=\frac{\mu_{0} I}{2 \pi}\left(\frac{1}{x}-\frac{1}{2 d-x}\right)
At x=d, B=0
For x < d, B is along \hat{j}
For x > d, B is along -\hat{j}
On the left side of the left conductor, magnetic fields due to the currents will add up and the net magnetic field will be along (-\hat{j}) direction.
To the right side of second conductor, the total magnetic field will be along \hat{j} direction.
Solution:
\rho=\frac{m}{V}=\frac{m}{\pi r^{2} l}
or,\frac{\Delta \rho}{\rho}=\frac{\Delta m}{m}+2 \frac{\Delta r }{r}+\frac{\Delta l}{l}
or, \frac{\Delta \rho}{\rho} \times 100=\left(\frac{0.003}{0.3}+2 \frac{0.005}{0.5}+\frac{0.06}{6}\right) \times 100
or, \frac{\Delta \rho}{\rho} \times 100=(0.01+0.02+0.01) \times 100
or, \frac{\Delta \rho}{\rho} \times 100=0.04 \times 100
(\Delta \rho / \rho) \times 100=4 \%
Therefore, the percentage error in the measurement of density is 4 .
Solution:
Let, the length of the escalator be L.
Velocity of the girl, v_{g}=L / t_{1}=L / 20
Velocity of the escalator, v _{ e }= L / t _{2}= L / 30
On moving escalator.
v_{\text {net }}=v_{g}+v_{e}
or, v _{\text {net }}=( L / 20)+( L / 30)
or, v _{\text {net }}= L / 12
Since, v_{\text {net }}=L / t
Therefore,
L / t = L / 12
t =12 s
Solution:
To protect herself from the rain, the woman must hold her umbrella in the direction of the relative velocity of the rain with respect to the woman.
\tan\, \theta= v _{ w } / v _{ f }=12\, m / s
or, \tan \,\theta=1
or, \theta=45^{\circ}
Therefore, the direction in which she should hold her umbrella is 45^{\circ} toward west.
Solution:
When a particle connected to a string revolves in a circular path around a centre, the centripetal force is provided by the tension produced in the string. Hence, in the given case, the net force on the particle is the tension T. \left(T=\left( mv ^{2}\right) / I \right)
Solution:
As we know,
P = Fv
where, P is the power, F is the force and v is the velocity.
or, P = mav
or, P = ma ^{2} t
or, P \propto t
Solution: