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Ramesh Chand 6 years, 5 months ago

V=at Dimension of V=dimension of at [LT-1]/[T]=a a=[LT-2] Dimension of c+t=[T] Dimension of b/c+t=dimension of v b=[LT-1]/[T] =[LT-2]
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Sia ? 6 years, 5 months ago

Temperature at which a real gas obeys idea gas behaviour (law) over an appreciable range of pressure.

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Yogita Ingle 6 years, 5 months ago

 and Q have different dimensions...  so  P - Q is not proper..

Perhaps  PQ has the same dimensions as that of R.

PQ/R  quantity is alright.

PR could probably have the same dimension as Q2

R + Q  is not possible... as they have different dimensions.

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Anjali Kumawat 6 years, 5 months ago

You can search in google
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Anjali Kumawat 6 years, 5 months ago

Distance /displacement covered by a particle in time (t) = total area of figure S= area of rectangle OACD + area of triangle ABC S= od *oa + 1/2 ac* bc S= (t-0) * u +1/2 (t-0)* (v-u) S= t*u+ 1/2 *t*at S=ut +1/2 at2 *(multiple)
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Sia ? 6 years, 5 months ago

The work-energy principle states that an increase in the kinetic energy of a rigid body is caused by an equal amount of positive work done on the body by the resultant force acting on that body. Conversely, a decrease in kinetic energy is caused by an equal amount of negative work done by the resultant force.

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Sia ? 6 years, 5 months ago

Let m and r be the respective masses of the hollow cylinder and the solid sphere.
 moment of inertia of the hollow cylinder I1 = mr2
The moment of inertia of the solid sphere I2 {tex}= \frac { 2 } { 5 } m r ^ { 2 }{/tex}
We have the relation:
{tex}\tau = I a{/tex}
For the hollow cylinder, {tex}\tau _ { 1 } = I _ { 1 } \alpha _ { 1 }{/tex}
For the solid sphere, {tex}\tau _ { 2 } = I _ { 2 } \alpha _ { 2 }{/tex}
As an equal torque is applied to both the bodies, {tex}\tau _ { 1 } = \tau _ { 2 }{/tex}
{tex}\therefore \frac {\alpha_ { 2 } } { \alpha _ { 1 } } = \frac { I _ { 1} } { I _ { 2 } } = \frac { M r ^ { 2 } } { \frac { 2 } { 5 } M r ^ { 2 } } = \frac { 2 } { 5 }{/tex}
{tex}a _ { 2 } > a _ { 1 }{/tex} ….(i)
Now, using the relation:
{tex}\omega = \omega _ { 0 } + a t{/tex}
{tex}\omega \propto a{/tex} …(ii)
From equations (i) and (ii), we can write:
{tex}\omega _ { 2 } > \omega _ { 1 }{/tex}
Hence, the angular velocity of the solid sphere will be greater than that of the hollow cylinder.

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Sia ? 6 years, 5 months ago

Let us consider the earth to be spherical mass of ‘M’ and radius ‘R’. A body of mass ‘m’ is placed initially on the surface and finally taken x distance deep into the earth.
We know acceleration due to gravity on the surface of earth is
This expression shows that acceleration due to gravity decreases as we go deep into the earth.
At the centre of earth x=R, so g’=0. Hence, the acceleration due to gravity at the centre of earth is zero (0).

 

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5O75O8 Kulwant Singh Kingra 6 years, 5 months ago

By modern book of physics
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Vipul Jadaun 6 years, 5 months ago

Hi

Mehak Gautam 6 years, 5 months ago

We shall derive the 1st and the 3rdlaw of motion fron the 2nd law. |Derivation of 1st law| According to Newton’s 2 nd law of motion, F = ma Where, F is the force applied, m is the mass of the body and a is the acceleration of the body. So, In absence of a force, F = 0 => ma = 0 => a = 0 Since, m cannot be zero for a body. Zero acceleration means, body at rest will remain at rest and a body in uniform motion will continue its uniform motion. Which is Newton’s 1st law of motion. |Derivation of 3rd law| Consider an isolated system of two bodies A and B. An isolated system is such that no force acts on the system. This is the Newton’s third law of motion for a body exerting some force on another. Thus, Newton’s 2nd law of motion is the most basic law of motion.
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Vivek Lather 6 years, 5 months ago

(3*2)+(-2*-x)+(2*3)= -12 6+2x+6= -12 12+2x= -12 2x= -24 x= -12

Rameshwar Jagtap 6 years, 5 months ago

12

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