Instagram story viewer> @engineeringwithjapheth> Posts
375
followers
15
following
🎓 Engineering made simple
📐 Mechanical l Civil l Electrical & Electronics
🔥 Courses l Calculation l Practical
📩 DM for more info
POSTS STORIES REELS TAGGED
Nobody talks about this, but your engineering courses are a chain.

Skip a link and the next course breaks. That's why the same students struggle in Thermodynamics, then Machine Design, then everything after.

Swipe for every Mechanical, Civil and Electrical course in the order I'd learn them.

Comment the course you're struggling with most, and DM me for more info.

#engineeringstudent #mechanicalengineering #civilengineering #electricalengineering #engineeringstudents by @engineeringwithjapheth
1
15 days ago
Download
WAIT UNTIL YOU SEE WHAT HAPPENS WHEN ENGINEERING FINALLY CLICKS.

A student can spend hours staring at an engineering question.

They know the formulas.

They've read the notes.

They've watched the examples.

And they still don't know where to start.

That is where real understanding changes everything.

The goal isn't just to show them how this question is solved.

It's to help them understand:

What is the question asking?
What information matters?
What principle applies?
How do I set up the solution?
Does my answer actually make sense?

Because the real transformation isn't:

“I got this question right.”

It's:

“I understand how to approach this.”

That's the kind of transformation I'm building Engineering With Japheth around.

Mechanical • Civil • Electrical & Electronics

Engineering, made simple.

@engineeringwithjapheth by @engineeringwithjapheth
1
15 days ago
Download
Most people only work hard when someone’s watching.

When the likes are coming. 
When the praise is flowing. 
When the results are public.

But the ones who actually win? 
They go just as hard in the dark.

No audience. 
No applause. 
No one keeping score.

Just them… and the work.

If you can look yourself in the mirror at 11pm, alone, and know you gave everything you had that day — 
you’re already ahead of 99% of people.

That’s the real game.

Be proud of the work no one sees. 
That’s where the unstoppable version of you is built.

#Motivation #Success #Mindset #Discipline by @engineeringwithjapheth
1
25 minutes ago
Download
STUCK ON POLYTROPIC PROCESS CALCULATIONS? START WITH THESE THREE THINGS. ⚙️

When solving a thermodynamics problem involving work done in a polytropic process, identify the initial state, the final state, and the polytropic index before substituting values.

The process follows:

PVⁿ = constant

For n not equal to 1, the boundary work done by the gas is:

W = (P₂V₂ − P₁V₁)/(1 − n)

You can also use the ideal-gas form when the required mass, gas constant, and temperatures are known:

W = mR(T₂ − T₁)/(1 − n)

Here is what you must check before calculating:

- Use absolute temperature in the ideal-gas equation.
- Keep pressure and volume units consistent.
- Distinguish work done by the gas from work done on the gas.
- Check the sign of your answer against whether the gas is expanding or being compressed.
- If n = 1, use the isothermal work equation instead.

These checks help prevent common errors in polytropic process numerical problems and thermodynamics examinations.

The goal is not merely to obtain a numerical answer. It is to know whether that answer makes physical sense.

Follow Engineering With Japheth for worked thermodynamics problems, formula derivations, and engineering concepts explained step by step.

Full video link is in my bio.

#Thermodynamics #SolvedProblems #MechanicalEngineering#mechanicalengineering #mechanicalengineeringstudent by @engineeringwithjapheth
1
2 hours ago
Download
WHEN A GAS EXPANDS, IT CAN DO USEFUL WORK. BUT HOW MUCH? ⚙️

Imagine gas expanding inside a piston-cylinder arrangement. As the gas pushes the piston outward, it transfers energy to its surroundings through boundary work.

For a polytropic process:

PVⁿ = constant

The work done by the gas is found from the area under the pressure-volume curve.

When n is not equal to 1:

W = (P₂V₂ − P₁V₁)/(1 − n)

For an ideal gas:

W = mR(T₂ − T₁)/(1 − n)

For expansion, the final volume is greater than the initial volume, so the work done by the gas is generally positive.

This is one reason pressure-volume diagrams are so important in engineering thermodynamics. The area under the process curve represents boundary work, and the shape of the curve depends on the process relationship.

Engineers use these principles to analyse piston-cylinder devices, reciprocating engines, compressors, and expansion processes in thermal systems.

Remember, the work done is not determined by the volume change alone. Pressure throughout the process also matters.

Understand the P-V diagram, and the work equation becomes much easier to interpret.

Follow Engineering With Japheth for practical thermodynamics lessons and step-by-step derivations.

Full video link is in my bio.

#Thermodynamics #BoundaryWork #MechanicalEngineering#mechanicalengineering #mechanicalengineeringstudent by @engineeringwithjapheth
0
5 hours ago
Download
ONE NUMBER CAN CHANGE YOUR POLYTROPIC WORK CALCULATION. ⚙️

That number is the polytropic index, n.

In a polytropic process, pressure and volume are related by:

PVⁿ = constant

The work done by the gas is:

W = (P₂V₂ − P₁V₁)/(1 − n)

Notice that n appears in the denominator. Its value affects the relationship between pressure, volume, and the work transferred during compression or expansion.

For an ideal gas, the same equation becomes:

W = mR(T₂ − T₁)/(1 − n)

The important point is that you cannot choose n arbitrarily for a real process. It represents the pressure-volume relationship being modelled.

For example, n = 1 represents an isothermal ideal-gas process, while n = γ represents a reversible adiabatic process for an ideal gas with constant specific heats.

Understanding these special cases helps you connect polytropic work calculations to isothermal and adiabatic processes in thermodynamics.

This knowledge is useful when solving engineering numerical problems involving compressors, engines, and gas expansion systems.

Don't memorise the equation without understanding the physical meaning of its terms.

Follow Engineering With Japheth for thermodynamics, applied mechanics, and engineering calculations explained clearly.

Full video link is in my bio.

#PolytropicProcess #Thermodynamics #EngineeringEducation#engineeringeducation #thermodynamicshelp by @engineeringwithjapheth
0
8 hours ago
Download
WORK DONE IN A POLYTROPIC PROCESS: THE DERIVATION YOU NEED TO UNDERSTAND ⚙️

How do engineers calculate the work required to compress a gas or the work produced when a gas expands?

In thermodynamics, the answer begins with the relationship between pressure and volume.

A polytropic process follows:

PVⁿ = C

where P is pressure, V is volume, n is the polytropic index, and C is a constant.

The boundary work done by a gas is calculated by integrating pressure with respect to volume. For a polytropic process where n is not equal to 1, this gives:

W = (P₂V₂ − P₁V₁) / (1 − n)

For an ideal gas, using PV = mRT, the equation can also be expressed as:

W = mR(T₂ − T₁) / (1 − n)

These equations calculate the work done by the gas. During expansion, the gas generally does positive boundary work. During compression, the work done by the gas is generally negative, meaning work is being done on it.

But here is what makes this useful beyond examinations.

Engineers use work calculations to analyse compressors, internal combustion engines, gas turbines, and other systems involving gas compression and expansion. Understanding the work required helps with energy balances, power requirements, and equipment performance analysis.

Remember that when n = 1, the process is isothermal for an ideal gas, and the work equation takes a different form:

W = mRT ln(V₂/V₁)

Don't just memorise the formula. Understand where it comes from, what the sign means, and when each equation applies.

Follow Engineering With Japheth for thermodynamics derivations, solved numerical problems, and practical mechanical engineering concepts.

Full video link is in my bio.

#Thermodynamics #PolytropicProcess #MechanicalEngineering#mechanicalengineering #mechanicalengineeringstudent by @engineeringwithjapheth
0
11 hours ago
Download
 by @engineeringwithjapheth
1
14 hours ago
Download
HOW MUCH WORK DOES IT TAKE TO COMPRESS A GAS? ⚙️

Every time a gas is compressed, energy must be transferred to the gas by the surrounding system. But how do engineers calculate exactly how much work is involved?

In thermodynamics, a polytropic process follows the relationship:

PVⁿ = constant

The boundary work done by the gas is obtained by integrating pressure with respect to volume. For a polytropic process where n is not equal to 1:

W = (P₂V₂ − P₁V₁)/(1 − n)

For an ideal gas, this can also be written as:

W = mR(T₂ − T₁)/(1 − n)

During compression, the volume decreases and the work done by the gas is generally negative. The work input required from the surroundings is therefore positive.

This calculation is important in gas compressors, refrigeration systems, pneumatic equipment, and industrial processes where gases must be pressurised.

The polytropic index also matters because it describes the pressure-volume relationship during the process. Different values of n represent different process behaviours and can produce different work requirements.

Engineering is not just about knowing the formula. It is about understanding the energy being transferred and what that means for the machine.

Follow Engineering With Japheth for clear thermodynamics explanations, derivations, and worked engineering calculations.

Full video link is in my bio.

#Thermodynamics #GasCompression #MechanicalEngineering#mechanicalengineering #mechanicalengineeringstudent by @engineeringwithjapheth
0
15 hours ago
Download
HEAT TRANSFER IN A POLYTROPIC PROCESS: DERIVATION OF Q ⚙️

Why memorise a thermodynamics formula when you can derive it from the first law?

A polytropic process follows the relationship PVⁿ = constant. To derive the heat transfer equation, we combine the first law of thermodynamics with the change in internal energy and the boundary work done by an ideal gas.

For a closed system:

Q = ΔU + W

For an ideal gas with constant specific heat capacity:

ΔU = mCv(T₂ − T₁)

For a polytropic process where n is not equal to 1, the boundary work is:

W = mR(T₂ − T₁)/(1 − n)

Substituting these expressions into the first law and simplifying gives:

Q = mCv(T₂ − T₁)(γ − n)/(γ − 1)

Here, Q is the heat transferred to the gas, m is the gas mass, Cv is the specific heat capacity at constant volume, γ is the specific heat ratio, and n is the polytropic index.

The sign of Q tells us the direction of heat transfer. A positive value means heat enters the gas, while a negative value means heat leaves it.

Notice something important: when n equals γ, the process is adiabatic for an ideal gas under these assumptions, and the heat transfer is zero.

Understanding this derivation connects the first law of thermodynamics, internal energy, boundary work, and heat transfer into one calculation.

Follow Engineering With Japheth for thermodynamics derivations, solved engineering problems, and explanations that help you understand why the formulas work.

Full video link is in my bio.

#Thermodynamics #PolytropicProcess #MechanicalEngineering by @engineeringwithjapheth
2
16 hours ago
Download
DOES A COMPRESSED GAS ALWAYS REJECT HEAT? NOT NECESSARILY. ⚙️

In a polytropic process, a gas can be compressed or expanded while exchanging heat with its surroundings. The amount and direction of heat transfer depend on how the pressure and volume change.

The process is described by the polytropic relationship (PV^n = C), where n is the polytropic index.

To determine the heat transfer, we combine the First Law of Thermodynamics with the change in internal energy and the work done during the process.

For an ideal gas, the temperature change helps determine the change in internal energy. The boundary work depends on the pressure-volume path.

This is why you cannot determine heat transfer from compression or expansion alone. You must consider the process conditions.

These principles are important in engineering thermodynamics, gas compressors, piston-cylinder systems, and calculations involving polytropic expansion and compression.

Heat, work, and internal energy are connected, but they are not the same thing.

Follow Engineering With Japheth for clear engineering explanations, thermodynamics formulas, and worked examples.

Full video link is in my bio.

#Thermodynamics #HeatTransfer #MechanicalEngineering

#mechanicalengineering by @engineeringwithjapheth
0
20 hours ago
Download
HEAT TRANSFER IN A POLYTROPIC PROCESS ⚙️

How do you calculate the heat supplied to or rejected by a gas during a polytropic process?

For a closed system, the First Law of Thermodynamics gives us the starting point: heat transfer equals the change in internal energy plus the work done by the system.

For an ideal gas undergoing a polytropic process, where pressure and volume follow the relationship (PV^n = C), the heat transfer can be calculated using the gas properties, the polytropic index, and the temperature change.

For a gas with constant specific heats, when (n \ne 1) and (n \ne \gamma):

Q = mCv(T₂ − T₁) × (γ − n)/(γ − 1)

Here, m is the mass, Cv is the specific heat at constant volume, γ is the ratio of specific heats, and n is the polytropic index.

The sign of Q tells you whether heat enters or leaves the gas under the convention that heat supplied is positive.

This relationship is useful in engineering thermodynamics problems involving polytropic compression, expansion, heat transfer, and gas processes.

Understand the relationship between heat, work, and internal energy before applying the formula.

Follow Engineering With Japheth for thermodynamics derivations, worked calculations, and practical engineering applications.

Full video link is in my bio.

#Thermodynamics #PolytropicProcess #MechanicalEngineering#mechanicalengineering by @engineeringwithjapheth
0
a day ago
Download

Download All

Save the photos and videos currently loaded on this page.

0Photos
0Videos
Ready to download 0 / 0

Keep this tab open until your download is ready.

back to up