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Question

A beam 300 mm depth and of symmetrical I section has a I = 1 x 108 mm4 and is simply supported over a span of 6 m. Calculate the udl it may carry if the max bending stress is not to exceed 100 N/mm2

The correct answer is

14.81 kN/m

Calculating UDL for Beam Bending Stress

This problem involves determining the maximum uniformly distributed load (UDL) a simply supported beam can carry without exceeding a specified maximum bending stress. We are given the beam's dimensions, moment of inertia, span, and the maximum allowable bending stress.

Given Data

Parameter Value
Beam depth (h) 300 mm
Section Symmetrical I section
Moment of Inertia (I) 1 x 108 mm4
Span (L) 6 m
Maximum bending stress (σmax) 100 N/mm2

Step-by-Step Calculation of UDL

First, let's ensure all units are consistent. The span is given in meters, while other dimensions and stress are in millimeters and Newtons/mm2. We will convert the span to millimeters:

  • Span \(L = 6 \text{ m} = 6 \times 1000 \text{ mm} = 6000 \text{ mm}\)

For a symmetrical I section, the neutral axis is at the mid-depth. The maximum bending stress occurs at the extreme fibers, which are at a distance \(y_{max}\) from the neutral axis.

  • Distance to extreme fiber \(y_{max} = \frac{\text{Beam depth}}{2} = \frac{300 \text{ mm}}{2} = 150 \text{ mm}\)

The section modulus (Z) is a geometric property of the beam's cross-section that relates bending stress to bending moment. It is calculated as:

\[Z = \frac{I}{y_{max}}\]

Substitute the given values:

\[Z = \frac{1 \times 10^8 \text{ mm}^4}{150 \text{ mm}}\] \[Z = \frac{10^8}{150} \text{ mm}^3\]

The relationship between maximum bending stress ($\sigma_{max}$), maximum bending moment ($M_{max}$), and section modulus (Z) is given by the bending formula:

\[\sigma_{max} = \frac{M_{max}}{Z}\]

We can rearrange this formula to find the maximum allowable bending moment:

\[M_{max} = \sigma_{max} \times Z\]

Substitute the values for $\sigma_{max}$ and Z:

\[M_{max} = 100 \text{ N/mm}^2 \times \frac{10^8}{150} \text{ mm}^3\] \[M_{max} = \frac{100 \times 10^8}{150} \text{ N-mm}\] \[M_{max} = \frac{10^{10}}{150} \text{ N-mm}\] \[M_{max} = \frac{10^9}{15} \text{ N-mm}\]

For a simply supported beam subjected to a uniformly distributed load (w) over its entire span (L), the maximum bending moment occurs at the center and is given by the formula:

\[M_{max} = \frac{wL^2}{8}\]

We know $M_{max}$ and $L$, and we need to find 'w'. Rearrange the formula to solve for 'w':

\[w = \frac{8 \times M_{max}}{L^2}\]

Substitute the calculated value of $M_{max}$ and the span $L$ (in mm):

\[w = \frac{8 \times \left(\frac{10^9}{15}\right) \text{ N-mm}}{(6000 \text{ mm})^2}\] \[w = \frac{\frac{8 \times 10^9}{15} \text{ N-mm}}{36 \times 10^6 \text{ mm}^2}\] \[w = \frac{8 \times 10^9}{15 \times 36 \times 10^6} \text{ N/mm}\] \[w = \frac{8 \times 1000}{15 \times 36} \text{ N/mm}\] \[w = \frac{8000}{540} \text{ N/mm}\] \[w = \frac{800}{54} \text{ N/mm}\] \[w = \frac{400}{27} \text{ N/mm}\] \[w \approx 14.8148 \text{ N/mm}\]

The options are given in kN/m or N/mm. Let's convert our result from N/mm to kN/m:

We know that 1 m = 1000 mm and 1 kN = 1000 N.

\[1 \text{ N/mm} = \frac{1 \text{ N}}{1 \text{ mm}} = \frac{1 \times (10^{-3} \text{ kN})}{1 \times (10^{-3} \text{ m})} = \frac{10^{-3} \text{ kN}}{10^{-3} \text{ m}} = 1 \text{ kN/m}\]

Therefore, \(w \approx 14.8148 \text{ N/mm}\) is approximately equal to \(14.8148 \text{ kN/m}\).

Comparing Calculated UDL with Options

Our calculated UDL is approximately 14.8148 kN/m.

  • Option 1: 14.6 kN/m
  • Option 2: 15 N/mm (= 15 kN/m)
  • Option 3: 14.81 kN/m
  • Option 4: 15.14 kN/m

Comparing the calculated value to the options, 14.81 kN/m is the closest match.

Thus, the maximum uniformly distributed load the beam can carry without exceeding the bending stress limit is approximately 14.81 kN/m.

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Important Questions from Beams

  1. For a simply supported beam or slab, the effective span is calculated as:

  2. Which of the following is CORRECT for indeterminate beam condition?

  3. A cantilever beam is one which is -

  4. In case of deep beam or in thin webbed R.C.C members, the first crack formed is-

  5. In case of web crippling, the dispersion of load from bearing plate takes place at:

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