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# Work And Power Assignment Help

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Classical Physics - Work And Power

**Work And Power**

In our daily life work implies an activity resulting in muscular or mental exertioan. However, in physics the term work is used when a particle is displaced by the action of a force. Thus, work is a scalar quantity; its**SI **unit is joule, **CGS unit erg**.

**ij = 107 erg**

dW = F ds

W = F . S = Fs cos θ (if F is constant)

W = ∫F . ds (if F is variable)

Work can be positive or negative as **θ** is acute or obtuse. Positive work means parallel to displacement and negative work means opposite to displacement.

Work done in lifting a body upwards from the ground is positive but the work done by the force of gravity (downwards) is negative.

When a body is pulled on a rough surface the work done by the pulling force is positive while work done against frictional force is negative

If a body is in static or dynamic equilibrium

**Work done = 0 because ∑F = 0 **

Work done is zero if displacement is zero or displacement is in direction perpendicular to the applied force. Thus work done by the centripetal force and work done by a moving charged particle in a magnetic field

**[(F = q(v x B )] is zero.**

Work done depends upon the frame of reference because with change in frame of reference displacement may change,. Hence the work done will be different in different frame of references.

In a conservative field, work done is path independent in F versus s curve work done is the area under the curve. The algebraic sum is to be made as illustrated in

**W = ∫v**_{2}v_{1} p. dV area under p – V curve is work.

**W = ∫F. ds = ∫ma. ds = ∫m dv/dt. Ds**

**∫mdv. ds / dt = ∫mv. dv**

= ?KE

Work done on particle by the resultant force acting on it is always equal to change in **KE >**

Thus for positive work **KE**_{final} > KE_{initial}

This theorem is valid for all types of forces (external or internal conservative or non conservative) and is called work energy theorem

**W = ?PE **(change in potential energy) (for conservatives forces)

**W = ½ kx**^{2}

Where **k** is spring constant and **x** is displacement. It could be extension or compression in case of spring.

**W = 1/2 **stress **x** strain **x** volume (in elastic bodies)

Since work is independent of time, the time rate of doing work is defined as power.

**P = dW / dt P average = W / t**

If force is constant

**P = dW / dt = d / dt (F. s) = F. ds / dt = F. v**

Power is a scalar quantity. Its **SI** unit is watt or **j/s**. practical unit **HP, 1 HP = 746W = 550 ft – Ib/s.**

**W = ∫P. dt or area under P – t curve.**

Practical unit of work or energy is **KWH (kilowatt-hour)**

**1 KWH = 3.6 x 1010 j**

Kinetic energy can never be negative.

ExpertsMind.com - Physics Assignment Help, Work And Power Assignment Help, Work And Power Homework Help, Work And Power Assignment Tutors, Work And Power Solutions, Work And Power Answers, Classical Physics Assignment Tutors

**Work And Power**

**SI**unit is joule,

**CGS unit erg**.

**ij = 107 erg**

dW = F ds

W = F . S = Fs cos θ (if F is constant)

W = ∫F . ds (if F is variable)

dW = F ds

W = F . S = Fs cos θ (if F is constant)

W = ∫F . ds (if F is variable)

Work can be positive or negative as

**θ**is acute or obtuse. Positive work means parallel to displacement and negative work means opposite to displacement.

Work done in lifting a body upwards from the ground is positive but the work done by the force of gravity (downwards) is negative.

When a body is pulled on a rough surface the work done by the pulling force is positive while work done against frictional force is negative

If a body is in static or dynamic equilibrium

**Work done = 0 because ∑F = 0**

Work done is zero if displacement is zero or displacement is in direction perpendicular to the applied force. Thus work done by the centripetal force and work done by a moving charged particle in a magnetic field

**[(F = q(v x B )] is zero.**

Work done depends upon the frame of reference because with change in frame of reference displacement may change,. Hence the work done will be different in different frame of references.

In a conservative field, work done is path independent in F versus s curve work done is the area under the curve. The algebraic sum is to be made as illustrated in

**W = ∫v**

_{2}v_{1}p. dV area under p – V curve is work.**W = ∫F. ds = ∫ma. ds = ∫m dv/dt. Ds**

**∫mdv. ds / dt = ∫mv. dv**

= ?KE

= ?KE

Work done on particle by the resultant force acting on it is always equal to change in

**KE >**

Thus for positive work

**KE**

_{final}> KE_{initial}This theorem is valid for all types of forces (external or internal conservative or non conservative) and is called work energy theorem

**W = ?PE**(change in potential energy) (for conservatives forces)

**W = ½ kx**

^{2}

Where

**k**is spring constant and

**x**is displacement. It could be extension or compression in case of spring.

**W = 1/2**stress

**x**strain

**x**volume (in elastic bodies)

Since work is independent of time, the time rate of doing work is defined as power.

**P = dW / dt P average = W / t**

If force is constant

**P = dW / dt = d / dt (F. s) = F. ds / dt = F. v**

Power is a scalar quantity. Its

**SI**unit is watt or

**j/s**. practical unit

**HP, 1 HP = 746W = 550 ft – Ib/s.**

**W = ∫P. dt or area under P – t curve.**

Practical unit of work or energy is

**KWH (kilowatt-hour)**

**1 KWH = 3.6 x 1010 j**

Kinetic energy can never be negative.

ExpertsMind.com - Physics Assignment Help, Work And Power Assignment Help, Work And Power Homework Help, Work And Power Assignment Tutors, Work And Power Solutions, Work And Power Answers, Classical Physics Assignment Tutors